,id,country_affiliations,value_affiliations,ordre_auteurs,name_auteurs,source,title,count_auteurs,ratio_auteurs,count_affiliations,ratio_affiliations,affiliation_norm,Affiliation,Code
44335,44455,,,750,"Iemmi, F.",Springer,Measurements of Higgs boson properties in the diphoton decay channel in proton-proton collisions at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>13</mn> </math>  $$ \sqrt{s}=13 $$  TeV,2302,0.0004344048653344917,,,nan,,NOT SCOAP3 Switzerland
44336,44455,,,772,"Latino, G.",Springer,Measurements of Higgs boson properties in the diphoton decay channel in proton-proton collisions at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>13</mn> </math>  $$ \sqrt{s}=13 $$  TeV,2302,0.0004344048653344917,,,nan,,NOT SCOAP3 Switzerland
44337,44455,,,841,"Lujan, P.",Springer,Measurements of Higgs boson properties in the diphoton decay channel in proton-proton collisions at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>13</mn> </math>  $$ \sqrt{s}=13 $$  TeV,2302,0.0004344048653344917,,,nan,,NOT SCOAP3 Switzerland
44338,44455,,,848,"Tiko, A.",Springer,Measurements of Higgs boson properties in the diphoton decay channel in proton-proton collisions at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>13</mn> </math>  $$ \sqrt{s}=13 $$  TeV,2302,0.0004344048653344917,,,nan,,NOT SCOAP3 Switzerland
44339,44455,,,882,"Borrello, L.",Springer,Measurements of Higgs boson properties in the diphoton decay channel in proton-proton collisions at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>13</mn> </math>  $$ \sqrt{s}=13 $$  TeV,2302,0.0004344048653344917,,,nan,,NOT SCOAP3 Switzerland
47814,44564,,,777,"Latino, G.",Springer,"Search for heavy resonances decaying into a vector boson and a Higgs boson in final states with charged leptons, neutrinos and b quarks at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>13</mn> </math>  $$ \sqrt{s}=13 $$  TeV",2302,0.0004344048653344917,,,nan,,NOT SCOAP3 Switzerland
47815,44564,,,830,"Bragagnolo, A.",Springer,"Search for heavy resonances decaying into a vector boson and a Higgs boson in final states with charged leptons, neutrinos and b quarks at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>13</mn> </math>  $$ \sqrt{s}=13 $$  TeV",2302,0.0004344048653344917,,,nan,,NOT SCOAP3 Switzerland
47816,44564,,,841,"Lujan, P.",Springer,"Search for heavy resonances decaying into a vector boson and a Higgs boson in final states with charged leptons, neutrinos and b quarks at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>13</mn> </math>  $$ \sqrt{s}=13 $$  TeV",2302,0.0004344048653344917,,,nan,,NOT SCOAP3 Switzerland
47817,44564,,,848,"Tiko, A.",Springer,"Search for heavy resonances decaying into a vector boson and a Higgs boson in final states with charged leptons, neutrinos and b quarks at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>13</mn> </math>  $$ \sqrt{s}=13 $$  TeV",2302,0.0004344048653344917,,,nan,,NOT SCOAP3 Switzerland
47818,44564,,,882,"Borrello, L.",Springer,"Search for heavy resonances decaying into a vector boson and a Higgs boson in final states with charged leptons, neutrinos and b quarks at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>13</mn> </math>  $$ \sqrt{s}=13 $$  TeV",2302,0.0004344048653344917,,,nan,,NOT SCOAP3 Switzerland
47819,44564,,,929,"Cometti, S.",Springer,"Search for heavy resonances decaying into a vector boson and a Higgs boson in final states with charged leptons, neutrinos and b quarks at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>13</mn> </math>  $$ \sqrt{s}=13 $$  TeV",2302,0.0004344048653344917,,,nan,,NOT SCOAP3 Switzerland
47820,44564,,,951,"Soldi, D.",Springer,"Search for heavy resonances decaying into a vector boson and a Higgs boson in final states with charged leptons, neutrinos and b quarks at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>13</mn> </math>  $$ \sqrt{s}=13 $$  TeV",2302,0.0004344048653344917,,,nan,,NOT SCOAP3 Switzerland
50393,44432,,,749,"Fontanesi, E.",Springer,Search for resonances in the mass spectrum of muon pairs produced in association with b quark jets in proton-proton collisions at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>8</mn> </math>  $$ \sqrt{s}=8 $$  and 13 TeV,2305,0.0004338394793926247,,,nan,,NOT SCOAP3 Switzerland
50394,44432,,,775,"Latino, G.",Springer,Search for resonances in the mass spectrum of muon pairs produced in association with b quark jets in proton-proton collisions at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>8</mn> </math>  $$ \sqrt{s}=8 $$  and 13 TeV,2305,0.0004338394793926247,,,nan,,NOT SCOAP3 Switzerland
50395,44432,,,806,"Monti, F.",Springer,Search for resonances in the mass spectrum of muon pairs produced in association with b quark jets in proton-proton collisions at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>8</mn> </math>  $$ \sqrt{s}=8 $$  and 13 TeV,2305,0.0004338394793926247,,,nan,,NOT SCOAP3 Switzerland
50396,44432,,,831,"Bragagnolo, A.",Springer,Search for resonances in the mass spectrum of muon pairs produced in association with b quark jets in proton-proton collisions at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>8</mn> </math>  $$ \sqrt{s}=8 $$  and 13 TeV,2305,0.0004338394793926247,,,nan,,NOT SCOAP3 Switzerland
50397,44432,,,840,"Hoh, S.",Springer,Search for resonances in the mass spectrum of muon pairs produced in association with b quark jets in proton-proton collisions at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>8</mn> </math>  $$ \sqrt{s}=8 $$  and 13 TeV,2305,0.0004338394793926247,,,nan,,NOT SCOAP3 Switzerland
50398,44432,,,842,"Lujan, P.",Springer,Search for resonances in the mass spectrum of muon pairs produced in association with b quark jets in proton-proton collisions at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>8</mn> </math>  $$ \sqrt{s}=8 $$  and 13 TeV,2305,0.0004338394793926247,,,nan,,NOT SCOAP3 Switzerland
50399,44432,,,851,"Tiko, A.",Springer,Search for resonances in the mass spectrum of muon pairs produced in association with b quark jets in proton-proton collisions at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>8</mn> </math>  $$ \sqrt{s}=8 $$  and 13 TeV,2305,0.0004338394793926247,,,nan,,NOT SCOAP3 Switzerland
50400,44432,,,884,"Borrello, L.",Springer,Search for resonances in the mass spectrum of muon pairs produced in association with b quark jets in proton-proton collisions at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>8</mn> </math>  $$ \sqrt{s}=8 $$  and 13 TeV,2305,0.0004338394793926247,,,nan,,NOT SCOAP3 Switzerland
52968,43942,,,775,"Latino, G.",Springer,Search for the decay of a Higgs boson in the ℓℓγ channel in proton-proton collisions at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>13</mn> </math>  $$ \sqrt{s}=13 $$  TeV,2301,0.000434593654932638,,,nan,,NOT SCOAP3 Switzerland
52969,43942,,,828,"Bragagnolo, A.",Springer,Search for the decay of a Higgs boson in the ℓℓγ channel in proton-proton collisions at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>13</mn> </math>  $$ \sqrt{s}=13 $$  TeV,2301,0.000434593654932638,,,nan,,NOT SCOAP3 Switzerland
52970,43942,,,837,"Lujan, P.",Springer,Search for the decay of a Higgs boson in the ℓℓγ channel in proton-proton collisions at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>13</mn> </math>  $$ \sqrt{s}=13 $$  TeV,2301,0.000434593654932638,,,nan,,NOT SCOAP3 Switzerland
52971,43942,,,844,"Tiko, A.",Springer,Search for the decay of a Higgs boson in the ℓℓγ channel in proton-proton collisions at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>13</mn> </math>  $$ \sqrt{s}=13 $$  TeV,2301,0.000434593654932638,,,nan,,NOT SCOAP3 Switzerland
52972,43942,,,879,"Borrello, L.",Springer,Search for the decay of a Higgs boson in the ℓℓγ channel in proton-proton collisions at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>13</mn> </math>  $$ \sqrt{s}=13 $$  TeV,2301,0.000434593654932638,,,nan,,NOT SCOAP3 Switzerland
52973,43942,,,926,"Cometti, S.",Springer,Search for the decay of a Higgs boson in the ℓℓγ channel in proton-proton collisions at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>13</mn> </math>  $$ \sqrt{s}=13 $$  TeV,2301,0.000434593654932638,,,nan,,NOT SCOAP3 Switzerland
52974,43942,,,948,"Soldi, D.",Springer,Search for the decay of a Higgs boson in the ℓℓγ channel in proton-proton collisions at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>13</mn> </math>  $$ \sqrt{s}=13 $$  TeV,2301,0.000434593654932638,,,nan,,NOT SCOAP3 Switzerland
55520,43954,,,775,"Latino, G.",Springer,Search for supersymmetry in events with a τ lepton pair and missing transverse momentum in proton-proton collisions at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>13</mn> </math>  $$ \sqrt{s}=13 $$  TeV,2298,0.0004351610095735422,,,nan,,NOT SCOAP3 Switzerland
55521,43954,,,828,"Bragagnolo, A.",Springer,Search for supersymmetry in events with a τ lepton pair and missing transverse momentum in proton-proton collisions at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>13</mn> </math>  $$ \sqrt{s}=13 $$  TeV,2298,0.0004351610095735422,,,nan,,NOT SCOAP3 Switzerland
55522,43954,,,838,"Lujan, P.",Springer,Search for supersymmetry in events with a τ lepton pair and missing transverse momentum in proton-proton collisions at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>13</mn> </math>  $$ \sqrt{s}=13 $$  TeV,2298,0.0004351610095735422,,,nan,,NOT SCOAP3 Switzerland
55523,43954,,,846,"Tiko, A.",Springer,Search for supersymmetry in events with a τ lepton pair and missing transverse momentum in proton-proton collisions at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>13</mn> </math>  $$ \sqrt{s}=13 $$  TeV,2298,0.0004351610095735422,,,nan,,NOT SCOAP3 Switzerland
55524,43954,,,879,"Borrello, L.",Springer,Search for supersymmetry in events with a τ lepton pair and missing transverse momentum in proton-proton collisions at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>13</mn> </math>  $$ \sqrt{s}=13 $$  TeV,2298,0.0004351610095735422,,,nan,,NOT SCOAP3 Switzerland
55525,43954,,,925,"Cometti, S.",Springer,Search for supersymmetry in events with a τ lepton pair and missing transverse momentum in proton-proton collisions at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>13</mn> </math>  $$ \sqrt{s}=13 $$  TeV,2298,0.0004351610095735422,,,nan,,NOT SCOAP3 Switzerland
55526,43954,,,947,"Soldi, D.",Springer,Search for supersymmetry in events with a τ lepton pair and missing transverse momentum in proton-proton collisions at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>13</mn> </math>  $$ \sqrt{s}=13 $$  TeV,2298,0.0004351610095735422,,,nan,,NOT SCOAP3 Switzerland
66680,43916,,,775,"Latino, G.",Springer,Search for a charged Higgs boson decaying to charm and bottom quarks in proton-proton collisions at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>8</mn> </math>  $$ \sqrt{s}=8 $$  TeV,2304,0.00043402777777777775,,,nan,,NOT SCOAP3 Switzerland
66681,43916,,,829,"Bragagnolo, A.",Springer,Search for a charged Higgs boson decaying to charm and bottom quarks in proton-proton collisions at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>8</mn> </math>  $$ \sqrt{s}=8 $$  TeV,2304,0.00043402777777777775,,,nan,,NOT SCOAP3 Switzerland
66682,43916,,,840,"Lujan, P.",Springer,Search for a charged Higgs boson decaying to charm and bottom quarks in proton-proton collisions at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>8</mn> </math>  $$ \sqrt{s}=8 $$  TeV,2304,0.00043402777777777775,,,nan,,NOT SCOAP3 Switzerland
66683,43916,,,846,"Tiko, A.",Springer,Search for a charged Higgs boson decaying to charm and bottom quarks in proton-proton collisions at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>8</mn> </math>  $$ \sqrt{s}=8 $$  TeV,2304,0.00043402777777777775,,,nan,,NOT SCOAP3 Switzerland
66684,43916,,,880,"Borrello, L.",Springer,Search for a charged Higgs boson decaying to charm and bottom quarks in proton-proton collisions at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>8</mn> </math>  $$ \sqrt{s}=8 $$  TeV,2304,0.00043402777777777775,,,nan,,NOT SCOAP3 Switzerland
66685,43916,,,926,"Cometti, S.",Springer,Search for a charged Higgs boson decaying to charm and bottom quarks in proton-proton collisions at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>8</mn> </math>  $$ \sqrt{s}=8 $$  TeV,2304,0.00043402777777777775,,,nan,,NOT SCOAP3 Switzerland
66686,43916,,,948,"Soldi, D.",Springer,Search for a charged Higgs boson decaying to charm and bottom quarks in proton-proton collisions at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>8</mn> </math>  $$ \sqrt{s}=8 $$  TeV,2304,0.00043402777777777775,,,nan,,NOT SCOAP3 Switzerland
69238,44052,,,773,"Latino, G.",Springer,Measurements of the differential jet cross section as a function of the jet mass in dijet events from proton-proton collisions at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>13</mn> </math>  $$ \sqrt{s}=13 $$  TeV,2300,0.0004347826086956522,,,nan,,NOT SCOAP3 Switzerland
69239,44052,,,809,"Zuolo, D.",Springer,Measurements of the differential jet cross section as a function of the jet mass in dijet events from proton-proton collisions at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>13</mn> </math>  $$ \sqrt{s}=13 $$  TeV,2300,0.0004347826086956522,,,nan,,NOT SCOAP3 Switzerland
69240,44052,,,827,"Bragagnolo, A.",Springer,Measurements of the differential jet cross section as a function of the jet mass in dijet events from proton-proton collisions at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>13</mn> </math>  $$ \sqrt{s}=13 $$  TeV,2300,0.0004347826086956522,,,nan,,NOT SCOAP3 Switzerland
69241,44052,,,837,"Hoh, S.",Springer,Measurements of the differential jet cross section as a function of the jet mass in dijet events from proton-proton collisions at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>13</mn> </math>  $$ \sqrt{s}=13 $$  TeV,2300,0.0004347826086956522,,,nan,,NOT SCOAP3 Switzerland
69242,44052,,,839,"Lujan, P.",Springer,Measurements of the differential jet cross section as a function of the jet mass in dijet events from proton-proton collisions at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>13</mn> </math>  $$ \sqrt{s}=13 $$  TeV,2300,0.0004347826086956522,,,nan,,NOT SCOAP3 Switzerland
69243,44052,,,847,"Tiko, A.",Springer,Measurements of the differential jet cross section as a function of the jet mass in dijet events from proton-proton collisions at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>13</mn> </math>  $$ \sqrt{s}=13 $$  TeV,2300,0.0004347826086956522,,,nan,,NOT SCOAP3 Switzerland
69244,44052,,,880,"Borrello, L.",Springer,Measurements of the differential jet cross section as a function of the jet mass in dijet events from proton-proton collisions at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>13</mn> </math>  $$ \sqrt{s}=13 $$  TeV,2300,0.0004347826086956522,,,nan,,NOT SCOAP3 Switzerland
86357,43627,,,778,"Latino, G.",Springer,Searches for pair production of charginos and top squarks in final states with two oppositely charged leptons in proton-proton collisions at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>13</mn> </math>  $$ \sqrt{s}=13 $$  TeV,2304,0.00043402777777777775,,,nan,,NOT SCOAP3 Switzerland
86358,43627,,,814,"Zuolo, D.",Springer,Searches for pair production of charginos and top squarks in final states with two oppositely charged leptons in proton-proton collisions at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>13</mn> </math>  $$ \sqrt{s}=13 $$  TeV,2304,0.00043402777777777775,,,nan,,NOT SCOAP3 Switzerland
86359,43627,,,832,"Bragagnolo, A.",Springer,Searches for pair production of charginos and top squarks in final states with two oppositely charged leptons in proton-proton collisions at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>13</mn> </math>  $$ \sqrt{s}=13 $$  TeV,2304,0.00043402777777777775,,,nan,,NOT SCOAP3 Switzerland
86360,43627,,,843,"Lujan, P.",Springer,Searches for pair production of charginos and top squarks in final states with two oppositely charged leptons in proton-proton collisions at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>13</mn> </math>  $$ \sqrt{s}=13 $$  TeV,2304,0.00043402777777777775,,,nan,,NOT SCOAP3 Switzerland
86361,43627,,,850,"Tiko, A.",Springer,Searches for pair production of charginos and top squarks in final states with two oppositely charged leptons in proton-proton collisions at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>13</mn> </math>  $$ \sqrt{s}=13 $$  TeV,2304,0.00043402777777777775,,,nan,,NOT SCOAP3 Switzerland
86362,43627,,,885,"Borrello, L.",Springer,Searches for pair production of charginos and top squarks in final states with two oppositely charged leptons in proton-proton collisions at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>13</mn> </math>  $$ \sqrt{s}=13 $$  TeV,2304,0.00043402777777777775,,,nan,,NOT SCOAP3 Switzerland
86363,43627,,,932,"Cometti, S.",Springer,Searches for pair production of charginos and top squarks in final states with two oppositely charged leptons in proton-proton collisions at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>13</mn> </math>  $$ \sqrt{s}=13 $$  TeV,2304,0.00043402777777777775,,,nan,,NOT SCOAP3 Switzerland
86364,43627,,,954,"Soldi, D.",Springer,Searches for pair production of charginos and top squarks in final states with two oppositely charged leptons in proton-proton collisions at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>13</mn> </math>  $$ \sqrt{s}=13 $$  TeV,2304,0.00043402777777777775,,,nan,,NOT SCOAP3 Switzerland
111165,44040,,,777,"Latino, G.",Springer,Search for black holes and sphalerons in high-multiplicity final states in proton-proton collisions at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>13</mn> </math>  $$ \sqrt{s}=13 $$  TeV,2304,0.00043402777777777775,,,nan,,NOT SCOAP3 Switzerland
111166,44040,,,830,"Bragagnolo, A.",Springer,Search for black holes and sphalerons in high-multiplicity final states in proton-proton collisions at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>13</mn> </math>  $$ \sqrt{s}=13 $$  TeV,2304,0.00043402777777777775,,,nan,,NOT SCOAP3 Switzerland
111167,44040,,,839,"Lujan, P.",Springer,Search for black holes and sphalerons in high-multiplicity final states in proton-proton collisions at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>13</mn> </math>  $$ \sqrt{s}=13 $$  TeV,2304,0.00043402777777777775,,,nan,,NOT SCOAP3 Switzerland
111168,44040,,,848,"Tiko, A.",Springer,Search for black holes and sphalerons in high-multiplicity final states in proton-proton collisions at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>13</mn> </math>  $$ \sqrt{s}=13 $$  TeV,2304,0.00043402777777777775,,,nan,,NOT SCOAP3 Switzerland
111169,44040,,,883,"Borrello, L.",Springer,Search for black holes and sphalerons in high-multiplicity final states in proton-proton collisions at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>13</mn> </math>  $$ \sqrt{s}=13 $$  TeV,2304,0.00043402777777777775,,,nan,,NOT SCOAP3 Switzerland
111170,44040,,,930,"Cometti, S.",Springer,Search for black holes and sphalerons in high-multiplicity final states in proton-proton collisions at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>13</mn> </math>  $$ \sqrt{s}=13 $$  TeV,2304,0.00043402777777777775,,,nan,,NOT SCOAP3 Switzerland
111171,44040,,,952,"Soldi, D.",Springer,Search for black holes and sphalerons in high-multiplicity final states in proton-proton collisions at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>13</mn> </math>  $$ \sqrt{s}=13 $$  TeV,2304,0.00043402777777777775,,,nan,,NOT SCOAP3 Switzerland
116812,44199,,,778,"Latino, G.",Springer,Search for an exotic decay of the Higgs boson to a pair of light pseudoscalars in the final state of two muons and two τ leptons in proton-proton collisions at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>13</mn> </math>  $$ \sqrt{s}=13 $$  TeV,2302,0.0004344048653344917,,,nan,,NOT SCOAP3 Switzerland
116813,44199,,,831,"Bragagnolo, A.",Springer,Search for an exotic decay of the Higgs boson to a pair of light pseudoscalars in the final state of two muons and two τ leptons in proton-proton collisions at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>13</mn> </math>  $$ \sqrt{s}=13 $$  TeV,2302,0.0004344048653344917,,,nan,,NOT SCOAP3 Switzerland
116814,44199,,,841,"Lujan, P.",Springer,Search for an exotic decay of the Higgs boson to a pair of light pseudoscalars in the final state of two muons and two τ leptons in proton-proton collisions at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>13</mn> </math>  $$ \sqrt{s}=13 $$  TeV,2302,0.0004344048653344917,,,nan,,NOT SCOAP3 Switzerland
116815,44199,,,849,"Tiko, A.",Springer,Search for an exotic decay of the Higgs boson to a pair of light pseudoscalars in the final state of two muons and two τ leptons in proton-proton collisions at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>13</mn> </math>  $$ \sqrt{s}=13 $$  TeV,2302,0.0004344048653344917,,,nan,,NOT SCOAP3 Switzerland
116816,44199,,,884,"Borrello, L.",Springer,Search for an exotic decay of the Higgs boson to a pair of light pseudoscalars in the final state of two muons and two τ leptons in proton-proton collisions at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>13</mn> </math>  $$ \sqrt{s}=13 $$  TeV,2302,0.0004344048653344917,,,nan,,NOT SCOAP3 Switzerland
116817,44199,,,931,"Cometti, S.",Springer,Search for an exotic decay of the Higgs boson to a pair of light pseudoscalars in the final state of two muons and two τ leptons in proton-proton collisions at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>13</mn> </math>  $$ \sqrt{s}=13 $$  TeV,2302,0.0004344048653344917,,,nan,,NOT SCOAP3 Switzerland
116818,44199,,,953,"Soldi, D.",Springer,Search for an exotic decay of the Higgs boson to a pair of light pseudoscalars in the final state of two muons and two τ leptons in proton-proton collisions at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>13</mn> </math>  $$ \sqrt{s}=13 $$  TeV,2302,0.0004344048653344917,,,nan,,NOT SCOAP3 Switzerland
128467,43344,,,229,"Finger, M.",APS,Search for physics beyond the standard model in high-mass diphoton events from proton-proton collisions at <math><mrow><msqrt><mrow><mi>s</mi></mrow></msqrt><mo>=</mo><mn>13</mn><mtext> </mtext><mtext> </mtext><mi>TeV</mi></mrow></math>,2298,0.0004351610095735422,,,nan,,NOT SCOAP3 Switzerland
144647,44113,,,778,"Latino, G.",Springer,Measurement of the groomed jet mass in PbPb and pp collisions at   <math> <msqrt> <msub> <mi>s</mi> <mrow> <mi>N</mi> <mi>N</mi> </mrow> </msub> </msqrt> <mo>=</mo> <mn>5.02</mn> </math>  $$ \sqrt{s_{\mathrm{NN}}}=5.02 $$  TeV,2300,0.0004347826086956522,,,nan,,NOT SCOAP3 Switzerland
144648,44113,,,814,"Zuolo, D.",Springer,Measurement of the groomed jet mass in PbPb and pp collisions at   <math> <msqrt> <msub> <mi>s</mi> <mrow> <mi>N</mi> <mi>N</mi> </mrow> </msub> </msqrt> <mo>=</mo> <mn>5.02</mn> </math>  $$ \sqrt{s_{\mathrm{NN}}}=5.02 $$  TeV,2300,0.0004347826086956522,,,nan,,NOT SCOAP3 Switzerland
144649,44113,,,832,"Bragagnolo, A.",Springer,Measurement of the groomed jet mass in PbPb and pp collisions at   <math> <msqrt> <msub> <mi>s</mi> <mrow> <mi>N</mi> <mi>N</mi> </mrow> </msub> </msqrt> <mo>=</mo> <mn>5.02</mn> </math>  $$ \sqrt{s_{\mathrm{NN}}}=5.02 $$  TeV,2300,0.0004347826086956522,,,nan,,NOT SCOAP3 Switzerland
144650,44113,,,842,"Hoh, S.",Springer,Measurement of the groomed jet mass in PbPb and pp collisions at   <math> <msqrt> <msub> <mi>s</mi> <mrow> <mi>N</mi> <mi>N</mi> </mrow> </msub> </msqrt> <mo>=</mo> <mn>5.02</mn> </math>  $$ \sqrt{s_{\mathrm{NN}}}=5.02 $$  TeV,2300,0.0004347826086956522,,,nan,,NOT SCOAP3 Switzerland
144651,44113,,,844,"Lujan, P.",Springer,Measurement of the groomed jet mass in PbPb and pp collisions at   <math> <msqrt> <msub> <mi>s</mi> <mrow> <mi>N</mi> <mi>N</mi> </mrow> </msub> </msqrt> <mo>=</mo> <mn>5.02</mn> </math>  $$ \sqrt{s_{\mathrm{NN}}}=5.02 $$  TeV,2300,0.0004347826086956522,,,nan,,NOT SCOAP3 Switzerland
144652,44113,,,851,"Tiko, A.",Springer,Measurement of the groomed jet mass in PbPb and pp collisions at   <math> <msqrt> <msub> <mi>s</mi> <mrow> <mi>N</mi> <mi>N</mi> </mrow> </msub> </msqrt> <mo>=</mo> <mn>5.02</mn> </math>  $$ \sqrt{s_{\mathrm{NN}}}=5.02 $$  TeV,2300,0.0004347826086956522,,,nan,,NOT SCOAP3 Switzerland
144653,44113,,,886,"Borrello, L.",Springer,Measurement of the groomed jet mass in PbPb and pp collisions at   <math> <msqrt> <msub> <mi>s</mi> <mrow> <mi>N</mi> <mi>N</mi> </mrow> </msub> </msqrt> <mo>=</mo> <mn>5.02</mn> </math>  $$ \sqrt{s_{\mathrm{NN}}}=5.02 $$  TeV,2300,0.0004347826086956522,,,nan,,NOT SCOAP3 Switzerland
144654,44113,,,933,"Cometti, S.",Springer,Measurement of the groomed jet mass in PbPb and pp collisions at   <math> <msqrt> <msub> <mi>s</mi> <mrow> <mi>N</mi> <mi>N</mi> </mrow> </msub> </msqrt> <mo>=</mo> <mn>5.02</mn> </math>  $$ \sqrt{s_{\mathrm{NN}}}=5.02 $$  TeV,2300,0.0004347826086956522,,,nan,,NOT SCOAP3 Switzerland
144655,44113,,,955,"Soldi, D.",Springer,Measurement of the groomed jet mass in PbPb and pp collisions at   <math> <msqrt> <msub> <mi>s</mi> <mrow> <mi>N</mi> <mi>N</mi> </mrow> </msub> </msqrt> <mo>=</mo> <mn>5.02</mn> </math>  $$ \sqrt{s_{\mathrm{NN}}}=5.02 $$  TeV,2300,0.0004347826086956522,,,nan,,NOT SCOAP3 Switzerland
154614,44203,,,749,"Fontanesi, E.",Springer,"Charged-particle nuclear modification factors in XeXe collisions at   <math> <msqrt> <msub> <mi>s</mi> <mrow> <mi>N</mi> <mi>N</mi> </mrow> </msub> </msqrt> <mo>=</mo> <mspace width=""0.25em""></mspace> <mn>5.44</mn> </math>  $$ \sqrt{s_{\mathrm{NN}}} = 5.44 $$  TeV",2302,0.0004344048653344917,,,nan,,NOT SCOAP3 Switzerland
154615,44203,,,775,"Latino, G.",Springer,"Charged-particle nuclear modification factors in XeXe collisions at   <math> <msqrt> <msub> <mi>s</mi> <mrow> <mi>N</mi> <mi>N</mi> </mrow> </msub> </msqrt> <mo>=</mo> <mspace width=""0.25em""></mspace> <mn>5.44</mn> </math>  $$ \sqrt{s_{\mathrm{NN}}} = 5.44 $$  TeV",2302,0.0004344048653344917,,,nan,,NOT SCOAP3 Switzerland
154616,44203,,,806,"Monti, F.",Springer,"Charged-particle nuclear modification factors in XeXe collisions at   <math> <msqrt> <msub> <mi>s</mi> <mrow> <mi>N</mi> <mi>N</mi> </mrow> </msub> </msqrt> <mo>=</mo> <mspace width=""0.25em""></mspace> <mn>5.44</mn> </math>  $$ \sqrt{s_{\mathrm{NN}}} = 5.44 $$  TeV",2302,0.0004344048653344917,,,nan,,NOT SCOAP3 Switzerland
154617,44203,,,831,"Bragagnolo, A.",Springer,"Charged-particle nuclear modification factors in XeXe collisions at   <math> <msqrt> <msub> <mi>s</mi> <mrow> <mi>N</mi> <mi>N</mi> </mrow> </msub> </msqrt> <mo>=</mo> <mspace width=""0.25em""></mspace> <mn>5.44</mn> </math>  $$ \sqrt{s_{\mathrm{NN}}} = 5.44 $$  TeV",2302,0.0004344048653344917,,,nan,,NOT SCOAP3 Switzerland
154618,44203,,,841,"Hoh, S.",Springer,"Charged-particle nuclear modification factors in XeXe collisions at   <math> <msqrt> <msub> <mi>s</mi> <mrow> <mi>N</mi> <mi>N</mi> </mrow> </msub> </msqrt> <mo>=</mo> <mspace width=""0.25em""></mspace> <mn>5.44</mn> </math>  $$ \sqrt{s_{\mathrm{NN}}} = 5.44 $$  TeV",2302,0.0004344048653344917,,,nan,,NOT SCOAP3 Switzerland
154619,44203,,,843,"Lujan, P.",Springer,"Charged-particle nuclear modification factors in XeXe collisions at   <math> <msqrt> <msub> <mi>s</mi> <mrow> <mi>N</mi> <mi>N</mi> </mrow> </msub> </msqrt> <mo>=</mo> <mspace width=""0.25em""></mspace> <mn>5.44</mn> </math>  $$ \sqrt{s_{\mathrm{NN}}} = 5.44 $$  TeV",2302,0.0004344048653344917,,,nan,,NOT SCOAP3 Switzerland
154620,44203,,,850,"Tiko, A.",Springer,"Charged-particle nuclear modification factors in XeXe collisions at   <math> <msqrt> <msub> <mi>s</mi> <mrow> <mi>N</mi> <mi>N</mi> </mrow> </msub> </msqrt> <mo>=</mo> <mspace width=""0.25em""></mspace> <mn>5.44</mn> </math>  $$ \sqrt{s_{\mathrm{NN}}} = 5.44 $$  TeV",2302,0.0004344048653344917,,,nan,,NOT SCOAP3 Switzerland
154621,44203,,,884,"Borrello, L.",Springer,"Charged-particle nuclear modification factors in XeXe collisions at   <math> <msqrt> <msub> <mi>s</mi> <mrow> <mi>N</mi> <mi>N</mi> </mrow> </msub> </msqrt> <mo>=</mo> <mspace width=""0.25em""></mspace> <mn>5.44</mn> </math>  $$ \sqrt{s_{\mathrm{NN}}} = 5.44 $$  TeV",2302,0.0004344048653344917,,,nan,,NOT SCOAP3 Switzerland
160300,44195,,,779,"Latino, G.",Springer,Measurement of the production cross section for single top quarks in association with W bosons in proton-proton collisions at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>13</mn> </math>  $$ \sqrt{s}=13 $$  TeV,2313,0.00043233895373973193,,,nan,,NOT SCOAP3 Switzerland
160301,44195,,,792,"Calvelli, V.",Springer,Measurement of the production cross section for single top quarks in association with W bosons in proton-proton collisions at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>13</mn> </math>  $$ \sqrt{s}=13 $$  TeV,2313,0.00043233895373973193,,,nan,,NOT SCOAP3 Switzerland
160302,44195,,,853,"Tiko, A.",Springer,Measurement of the production cross section for single top quarks in association with W bosons in proton-proton collisions at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>13</mn> </math>  $$ \sqrt{s}=13 $$  TeV,2313,0.00043233895373973193,,,nan,,NOT SCOAP3 Switzerland
160303,44195,,,888,"Borrello, L.",Springer,Measurement of the production cross section for single top quarks in association with W bosons in proton-proton collisions at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>13</mn> </math>  $$ \sqrt{s}=13 $$  TeV,2313,0.00043233895373973193,,,nan,,NOT SCOAP3 Switzerland
191362,42848,,,1978,"Perez-Victoria, M.",APS,Combination of searches for heavy resonances decaying into bosonic and leptonic final states using <math><mrow><mn>36</mn><mtext> </mtext><mtext> </mtext><msup><mrow><mi>fb</mi></mrow><mrow><mo>−</mo><mn>1</mn></mrow></msup></mrow></math> of proton-proton collision data at <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn><mtext> </mtext><mtext> </mtext><mi>TeV</mi></math> with the ATLAS detector,2928,0.00034153005464480874,,,nan,,NOT SCOAP3 Switzerland
193880,42903,,,816,"Lujan, P.",Springer,Search for Zγ resonances using leptonic and hadronic final states in proton-proton collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2262,0.0004420866489832007,,,nan,,NOT SCOAP3 Switzerland
193881,42903,,,856,"Borrello, L.",Springer,Search for Zγ resonances using leptonic and hadronic final states in proton-proton collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2262,0.0004420866489832007,,,nan,,NOT SCOAP3 Switzerland
208725,42768,,,773,"Latino, G.",Springer,Search for a heavy resonance decaying into a Z boson and a Z or W boson in 2ℓ2q final states at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2303,0.0004342162396873643,,,nan,,NOT SCOAP3 Switzerland
208726,42768,,,842,"Lujan, P.",Springer,Search for a heavy resonance decaying into a Z boson and a Z or W boson in 2ℓ2q final states at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2303,0.0004342162396873643,,,nan,,NOT SCOAP3 Switzerland
208727,42768,,,849,"Tiko, A.",Springer,Search for a heavy resonance decaying into a Z boson and a Z or W boson in 2ℓ2q final states at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2303,0.0004342162396873643,,,nan,,NOT SCOAP3 Switzerland
208728,42768,,,883,"Borrello, L.",Springer,Search for a heavy resonance decaying into a Z boson and a Z or W boson in 2ℓ2q final states at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2303,0.0004342162396873643,,,nan,,NOT SCOAP3 Switzerland
223085,42673,,,769,"Latino, G.",Springer,Search for top squarks decaying via four-body or chargino-mediated modes in single-lepton final states in proton-proton collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2290,0.0004366812227074236,,,nan,,NOT SCOAP3 Switzerland
223086,42673,,,825,"Bragagnolo, A.",Springer,Search for top squarks decaying via four-body or chargino-mediated modes in single-lepton final states in proton-proton collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2290,0.0004366812227074236,,,nan,,NOT SCOAP3 Switzerland
223087,42673,,,834,"Lujan, P.",Springer,Search for top squarks decaying via four-body or chargino-mediated modes in single-lepton final states in proton-proton collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2290,0.0004366812227074236,,,nan,,NOT SCOAP3 Switzerland
223088,42673,,,842,"Tiko, A.",Springer,Search for top squarks decaying via four-body or chargino-mediated modes in single-lepton final states in proton-proton collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2290,0.0004366812227074236,,,nan,,NOT SCOAP3 Switzerland
223089,42673,,,876,"Borrello, L.",Springer,Search for top squarks decaying via four-body or chargino-mediated modes in single-lepton final states in proton-proton collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2290,0.0004366812227074236,,,nan,,NOT SCOAP3 Switzerland
225823,42610,,,777,"Latino, G.",Springer,Search for dark matter produced in association with a Higgs boson decaying to γγ or τ + τ − at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2304,0.00043402777777777775,,,nan,,NOT SCOAP3 Switzerland
225824,42610,,,830,"Bragagnolo, A.",Springer,Search for dark matter produced in association with a Higgs boson decaying to γγ or τ + τ − at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2304,0.00043402777777777775,,,nan,,NOT SCOAP3 Switzerland
225825,42610,,,841,"Lujan, P.",Springer,Search for dark matter produced in association with a Higgs boson decaying to γγ or τ + τ − at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2304,0.00043402777777777775,,,nan,,NOT SCOAP3 Switzerland
225826,42610,,,848,"Tiko, A.",Springer,Search for dark matter produced in association with a Higgs boson decaying to γγ or τ + τ − at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2304,0.00043402777777777775,,,nan,,NOT SCOAP3 Switzerland
225827,42610,,,883,"Borrello, L.",Springer,Search for dark matter produced in association with a Higgs boson decaying to γγ or τ + τ − at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2304,0.00043402777777777775,,,nan,,NOT SCOAP3 Switzerland
225828,42610,,,930,"Cometti, S.",Springer,Search for dark matter produced in association with a Higgs boson decaying to γγ or τ + τ − at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2304,0.00043402777777777775,,,nan,,NOT SCOAP3 Switzerland
225829,42610,,,952,"Soldi, D.",Springer,Search for dark matter produced in association with a Higgs boson decaying to γγ or τ + τ − at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2304,0.00043402777777777775,,,nan,,NOT SCOAP3 Switzerland
236986,42517,,,774,"Latino, G.",Springer,Search for additional neutral MSSM Higgs bosons in the τ τ final state in proton-proton collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2305,0.0004338394793926247,,,nan,,NOT SCOAP3 Switzerland
236987,42517,,,841,"Lujan, P.",Springer,Search for additional neutral MSSM Higgs bosons in the τ τ final state in proton-proton collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2305,0.0004338394793926247,,,nan,,NOT SCOAP3 Switzerland
236988,42517,,,848,"Tiko, A.",Springer,Search for additional neutral MSSM Higgs bosons in the τ τ final state in proton-proton collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2305,0.0004338394793926247,,,nan,,NOT SCOAP3 Switzerland
236989,42517,,,884,"Borrello, L.",Springer,Search for additional neutral MSSM Higgs bosons in the τ τ final state in proton-proton collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2305,0.0004338394793926247,,,nan,,NOT SCOAP3 Switzerland
262573,42427,,,769,"Latino, G.",Springer,Search for vector-like T and B quark pairs in final states with leptons at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2291,0.00043649061545176777,,,nan,,NOT SCOAP3 Switzerland
262574,42427,,,824,"Bragagnolo, A.",Springer,Search for vector-like T and B quark pairs in final states with leptons at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2291,0.00043649061545176777,,,nan,,NOT SCOAP3 Switzerland
262575,42427,,,834,"Lujan, P.",Springer,Search for vector-like T and B quark pairs in final states with leptons at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2291,0.00043649061545176777,,,nan,,NOT SCOAP3 Switzerland
262576,42427,,,841,"Tiko, A.",Springer,Search for vector-like T and B quark pairs in final states with leptons at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2291,0.00043649061545176777,,,nan,,NOT SCOAP3 Switzerland
262577,42427,,,876,"Borrello, L.",Springer,Search for vector-like T and B quark pairs in final states with leptons at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2291,0.00043649061545176777,,,nan,,NOT SCOAP3 Switzerland
265148,42255,,,771,"Latino, G.",Springer,Search for resonant pair production of Higgs bosons decaying to bottom quark-antiquark pairs in proton-proton collisions at 13 TeV,2304,0.00043402777777777775,,,nan,,NOT SCOAP3 Switzerland
265149,42255,,,838,"Lujan, P.",Springer,Search for resonant pair production of Higgs bosons decaying to bottom quark-antiquark pairs in proton-proton collisions at 13 TeV,2304,0.00043402777777777775,,,nan,,NOT SCOAP3 Switzerland
265150,42255,,,846,"Tiko, A.",Springer,Search for resonant pair production of Higgs bosons decaying to bottom quark-antiquark pairs in proton-proton collisions at 13 TeV,2304,0.00043402777777777775,,,nan,,NOT SCOAP3 Switzerland
265151,42255,,,881,"Borrello, L.",Springer,Search for resonant pair production of Higgs bosons decaying to bottom quark-antiquark pairs in proton-proton collisions at 13 TeV,2304,0.00043402777777777775,,,nan,,NOT SCOAP3 Switzerland
265152,42255,,,891,"Malara, A.",Springer,Search for resonant pair production of Higgs bosons decaying to bottom quark-antiquark pairs in proton-proton collisions at 13 TeV,2304,0.00043402777777777775,,,nan,,NOT SCOAP3 Switzerland
274195,42313,,,752,"Iemmi, F.",Springer,Search for narrow and broad dijet resonances in proton-proton collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV and constraints on dark matter mediators and other new particles,2304,0.00043402777777777775,,,nan,,NOT SCOAP3 Switzerland
274196,42313,,,774,"Latino, G.",Springer,Search for narrow and broad dijet resonances in proton-proton collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV and constraints on dark matter mediators and other new particles,2304,0.00043402777777777775,,,nan,,NOT SCOAP3 Switzerland
274197,42313,,,848,"Tiko, A.",Springer,Search for narrow and broad dijet resonances in proton-proton collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV and constraints on dark matter mediators and other new particles,2304,0.00043402777777777775,,,nan,,NOT SCOAP3 Switzerland
274198,42313,,,883,"Borrello, L.",Springer,Search for narrow and broad dijet resonances in proton-proton collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV and constraints on dark matter mediators and other new particles,2304,0.00043402777777777775,,,nan,,NOT SCOAP3 Switzerland
276744,42181,,,769,"Latino, G.",Springer,Search for beyond the standard model Higgs bosons decaying into a  <math><mi>b</mi><mover><mi>b</mi><mo>¯</mo></mover></math> $$ \mathrm{b}\overline{\mathrm{b}} $$ pair in pp collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2293,0.0004361098996947231,,,nan,,NOT SCOAP3 Switzerland
276745,42181,,,826,"Bragagnolo, A.",Springer,Search for beyond the standard model Higgs bosons decaying into a  <math><mi>b</mi><mover><mi>b</mi><mo>¯</mo></mover></math> $$ \mathrm{b}\overline{\mathrm{b}} $$ pair in pp collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2293,0.0004361098996947231,,,nan,,NOT SCOAP3 Switzerland
276746,42181,,,836,"Lujan, P.",Springer,Search for beyond the standard model Higgs bosons decaying into a  <math><mi>b</mi><mover><mi>b</mi><mo>¯</mo></mover></math> $$ \mathrm{b}\overline{\mathrm{b}} $$ pair in pp collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2293,0.0004361098996947231,,,nan,,NOT SCOAP3 Switzerland
276747,42181,,,843,"Tiko, A.",Springer,Search for beyond the standard model Higgs bosons decaying into a  <math><mi>b</mi><mover><mi>b</mi><mo>¯</mo></mover></math> $$ \mathrm{b}\overline{\mathrm{b}} $$ pair in pp collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2293,0.0004361098996947231,,,nan,,NOT SCOAP3 Switzerland
276748,42181,,,876,"Borrello, L.",Springer,Search for beyond the standard model Higgs bosons decaying into a  <math><mi>b</mi><mover><mi>b</mi><mo>¯</mo></mover></math> $$ \mathrm{b}\overline{\mathrm{b}} $$ pair in pp collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2293,0.0004361098996947231,,,nan,,NOT SCOAP3 Switzerland
289491,42111,,,772,"Latino, G.",Springer,"Evidence for associated production of a Higgs boson with a top quark pair in final states with electrons, muons, and hadronically decaying τ leptons at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV",2301,0.000434593654932638,,,nan,,NOT SCOAP3 Switzerland
289492,42111,,,840,"Lujan, P.",Springer,"Evidence for associated production of a Higgs boson with a top quark pair in final states with electrons, muons, and hadronically decaying τ leptons at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV",2301,0.000434593654932638,,,nan,,NOT SCOAP3 Switzerland
289493,42111,,,847,"Tiko, A.",Springer,"Evidence for associated production of a Higgs boson with a top quark pair in final states with electrons, muons, and hadronically decaying τ leptons at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV",2301,0.000434593654932638,,,nan,,NOT SCOAP3 Switzerland
289494,42111,,,882,"Borrello, L.",Springer,"Evidence for associated production of a Higgs boson with a top quark pair in final states with electrons, muons, and hadronically decaying τ leptons at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV",2301,0.000434593654932638,,,nan,,NOT SCOAP3 Switzerland
302384,41933,,,770,"Latino, G.",Springer,Search for disappearing tracks as a signature of new long-lived particles in proton-proton collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2290,0.0004366812227074236,,,nan,,NOT SCOAP3 Switzerland
302385,41933,,,825,"Bragagnolo, A.",Springer,Search for disappearing tracks as a signature of new long-lived particles in proton-proton collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2290,0.0004366812227074236,,,nan,,NOT SCOAP3 Switzerland
302386,41933,,,836,"Lujan, P.",Springer,Search for disappearing tracks as a signature of new long-lived particles in proton-proton collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2290,0.0004366812227074236,,,nan,,NOT SCOAP3 Switzerland
302387,41933,,,843,"Tiko, A.",Springer,Search for disappearing tracks as a signature of new long-lived particles in proton-proton collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2290,0.0004366812227074236,,,nan,,NOT SCOAP3 Switzerland
302388,41933,,,876,"Borrello, L.",Springer,Search for disappearing tracks as a signature of new long-lived particles in proton-proton collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2290,0.0004366812227074236,,,nan,,NOT SCOAP3 Switzerland
302389,41933,,,922,"Cometti, S.",Springer,Search for disappearing tracks as a signature of new long-lived particles in proton-proton collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2290,0.0004366812227074236,,,nan,,NOT SCOAP3 Switzerland
302390,41933,,,944,"Soldi, D.",Springer,Search for disappearing tracks as a signature of new long-lived particles in proton-proton collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2290,0.0004366812227074236,,,nan,,NOT SCOAP3 Switzerland
311335,41829,,,813,"Lujan, P.",Springer,Measurement of the cross section for top quark pair production in association with a W or Z boson in proton-proton collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2258,0.0004428697962798937,,,nan,,NOT SCOAP3 Switzerland
311336,41829,,,853,"Borrello, L.",Springer,Measurement of the cross section for top quark pair production in association with a W or Z boson in proton-proton collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2258,0.0004428697962798937,,,nan,,NOT SCOAP3 Switzerland
326610,41700,,,734,"Iemmi, F.",Springer,Measurement of the inelastic proton-proton cross section at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2283,0.0004380201489268506,,,nan,,NOT SCOAP3 Switzerland
326611,41700,,,757,"Latino, G.",Springer,Measurement of the inelastic proton-proton cross section at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2283,0.0004380201489268506,,,nan,,NOT SCOAP3 Switzerland
326612,41700,,,823,"Lujan, P.",Springer,Measurement of the inelastic proton-proton cross section at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2283,0.0004380201489268506,,,nan,,NOT SCOAP3 Switzerland
326613,41700,,,830,"Tiko, A.",Springer,Measurement of the inelastic proton-proton cross section at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2283,0.0004380201489268506,,,nan,,NOT SCOAP3 Switzerland
326614,41700,,,865,"Borrello, L.",Springer,Measurement of the inelastic proton-proton cross section at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2283,0.0004380201489268506,,,nan,,NOT SCOAP3 Switzerland
329295,41665,,,748,"Iemmi, F.",Springer,"Observation of proton-tagged, central (semi)exclusive production of high-mass lepton pairs in pp collisions at 13 TeV with the CMS-TOTEM precision proton spectrometer",2383,0.000419639110365086,,,nan,,NOT SCOAP3 Switzerland
329296,41665,,,771,"Latino, G.",Springer,"Observation of proton-tagged, central (semi)exclusive production of high-mass lepton pairs in pp collisions at 13 TeV with the CMS-TOTEM precision proton spectrometer",2383,0.000419639110365086,,,nan,,NOT SCOAP3 Switzerland
329297,41665,,,845,"Tiko, A.",Springer,"Observation of proton-tagged, central (semi)exclusive production of high-mass lepton pairs in pp collisions at 13 TeV with the CMS-TOTEM precision proton spectrometer",2383,0.000419639110365086,,,nan,,NOT SCOAP3 Switzerland
329298,41665,,,880,"Borrello, L.",Springer,"Observation of proton-tagged, central (semi)exclusive production of high-mass lepton pairs in pp collisions at 13 TeV with the CMS-TOTEM precision proton spectrometer",2383,0.000419639110365086,,,nan,,NOT SCOAP3 Switzerland
341310,41530,,,776,"Latino, G.",Springer,Search for a singly produced third-generation scalar leptoquark decaying to a τ lepton and a bottom quark in proton-proton collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2302,0.0004344048653344917,,,nan,,NOT SCOAP3 Switzerland
341311,41530,,,829,"Bragagnolo, A.",Springer,Search for a singly produced third-generation scalar leptoquark decaying to a τ lepton and a bottom quark in proton-proton collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2302,0.0004344048653344917,,,nan,,NOT SCOAP3 Switzerland
341312,41530,,,840,"Lujan, P.",Springer,Search for a singly produced third-generation scalar leptoquark decaying to a τ lepton and a bottom quark in proton-proton collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2302,0.0004344048653344917,,,nan,,NOT SCOAP3 Switzerland
341313,41530,,,847,"Tiko, A.",Springer,Search for a singly produced third-generation scalar leptoquark decaying to a τ lepton and a bottom quark in proton-proton collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2302,0.0004344048653344917,,,nan,,NOT SCOAP3 Switzerland
341314,41530,,,882,"Borrello, L.",Springer,Search for a singly produced third-generation scalar leptoquark decaying to a τ lepton and a bottom quark in proton-proton collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2302,0.0004344048653344917,,,nan,,NOT SCOAP3 Switzerland
341315,41530,,,929,"Cometti, S.",Springer,Search for a singly produced third-generation scalar leptoquark decaying to a τ lepton and a bottom quark in proton-proton collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2302,0.0004344048653344917,,,nan,,NOT SCOAP3 Switzerland
341316,41530,,,951,"Soldi, D.",Springer,Search for a singly produced third-generation scalar leptoquark decaying to a τ lepton and a bottom quark in proton-proton collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2302,0.0004344048653344917,,,nan,,NOT SCOAP3 Switzerland
350371,41283,,,824,"Lujan, P.",Springer,Search for a heavy resonance decaying into a Z boson and a vector boson in the  <math><mi>ν</mi><mover><mi>ν</mi><mo>¯</mo></mover><mi>q</mi><mover><mi>q</mi><mo>¯</mo></mover></math> $$ \nu \overline{\nu}\mathrm{q}\overline{\mathrm{q}} $$ final state,2276,0.0004393673110720562,,,nan,,NOT SCOAP3 Switzerland
350372,41283,,,863,"Borrello, L.",Springer,Search for a heavy resonance decaying into a Z boson and a vector boson in the  <math><mi>ν</mi><mover><mi>ν</mi><mo>¯</mo></mover><mi>q</mi><mover><mi>q</mi><mo>¯</mo></mover></math> $$ \nu \overline{\nu}\mathrm{q}\overline{\mathrm{q}} $$ final state,2276,0.0004393673110720562,,,nan,,NOT SCOAP3 Switzerland
360556,41128,,,806,"Lujan, P.",Springer,Measurement of the underlying event activity in inclusive Z boson production in proton-proton collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2241,0.0004462293618920125,,,nan,,NOT SCOAP3 Switzerland
360557,41128,,,823,"Ressegotti, M.",Springer,Measurement of the underlying event activity in inclusive Z boson production in proton-proton collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2241,0.0004462293618920125,,,nan,,NOT SCOAP3 Switzerland
360558,41128,,,848,"Borrello, L.",Springer,Measurement of the underlying event activity in inclusive Z boson production in proton-proton collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2241,0.0004462293618920125,,,nan,,NOT SCOAP3 Switzerland
368286,41458,,,772,"Latino, G.",Springer,Search for a new scalar resonance decaying to a pair of Z bosons in proton-proton collisions at      <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>13</mn> </math>  $$ sqrt{s}=13 $$  TeV,2303,0.0004342162396873643,,,nan,,NOT SCOAP3 Switzerland
368287,41458,,,841,"Lujan, P.",Springer,Search for a new scalar resonance decaying to a pair of Z bosons in proton-proton collisions at      <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>13</mn> </math>  $$ sqrt{s}=13 $$  TeV,2303,0.0004342162396873643,,,nan,,NOT SCOAP3 Switzerland
368288,41458,,,847,"Tiko, A.",Springer,Search for a new scalar resonance decaying to a pair of Z bosons in proton-proton collisions at      <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>13</mn> </math>  $$ sqrt{s}=13 $$  TeV,2303,0.0004342162396873643,,,nan,,NOT SCOAP3 Switzerland
368289,41458,,,882,"Borrello, L.",Springer,Search for a new scalar resonance decaying to a pair of Z bosons in proton-proton collisions at      <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>13</mn> </math>  $$ sqrt{s}=13 $$  TeV,2303,0.0004342162396873643,,,nan,,NOT SCOAP3 Switzerland
370856,40970,,,772,"Latino, G.",Springer,Search for high-mass resonances in final states with a lepton and missing transverse momentum at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2301,0.000434593654932638,,,nan,,NOT SCOAP3 Switzerland
370857,40970,,,846,"Tiko, A.",Springer,Search for high-mass resonances in final states with a lepton and missing transverse momentum at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2301,0.000434593654932638,,,nan,,NOT SCOAP3 Switzerland
370858,40970,,,881,"Borrello, L.",Springer,Search for high-mass resonances in final states with a lepton and missing transverse momentum at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2301,0.000434593654932638,,,nan,,NOT SCOAP3 Switzerland
376484,41461,,,772,"Latino, G.",Springer,Search for high-mass resonances in dilepton final states in proton-proton collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2304,0.00043402777777777775,,,nan,,NOT SCOAP3 Switzerland
376485,41461,,,842,"Lujan, P.",Springer,Search for high-mass resonances in dilepton final states in proton-proton collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2304,0.00043402777777777775,,,nan,,NOT SCOAP3 Switzerland
376486,41461,,,849,"Tiko, A.",Springer,Search for high-mass resonances in dilepton final states in proton-proton collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2304,0.00043402777777777775,,,nan,,NOT SCOAP3 Switzerland
376487,41461,,,883,"Borrello, L.",Springer,Search for high-mass resonances in dilepton final states in proton-proton collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2304,0.00043402777777777775,,,nan,,NOT SCOAP3 Switzerland
388857,41477,,,772,"Latino, G.",Springer,Search for  <math><mi>t</mi><mover><mi>t</mi><mo>¯</mo></mover><mi>H</mi></math> $$ \mathrm{t}\overline{\mathrm{t}}\mathrm{H} $$ production in the all-jet final state in proton-proton collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2301,0.000434593654932638,,,nan,,NOT SCOAP3 Switzerland
388858,41477,,,846,"Tiko, A.",Springer,Search for  <math><mi>t</mi><mover><mi>t</mi><mo>¯</mo></mover><mi>H</mi></math> $$ \mathrm{t}\overline{\mathrm{t}}\mathrm{H} $$ production in the all-jet final state in proton-proton collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2301,0.000434593654932638,,,nan,,NOT SCOAP3 Switzerland
388859,41477,,,881,"Borrello, L.",Springer,Search for  <math><mi>t</mi><mover><mi>t</mi><mo>¯</mo></mover><mi>H</mi></math> $$ \mathrm{t}\overline{\mathrm{t}}\mathrm{H} $$ production in the all-jet final state in proton-proton collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2301,0.000434593654932638,,,nan,,NOT SCOAP3 Switzerland
391404,41462,,,739,"Iemmi, F.",Springer,Search for the flavor-changing neutral current interactions of the top quark and the Higgs boson which decays into a pair of b quarks at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2284,0.00043782837127845885,,,nan,,NOT SCOAP3 Switzerland
391405,41462,,,827,"Lujan, P.",Springer,Search for the flavor-changing neutral current interactions of the top quark and the Higgs boson which decays into a pair of b quarks at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2284,0.00043782837127845885,,,nan,,NOT SCOAP3 Switzerland
391406,41462,,,834,"Tiko, A.",Springer,Search for the flavor-changing neutral current interactions of the top quark and the Higgs boson which decays into a pair of b quarks at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2284,0.00043782837127845885,,,nan,,NOT SCOAP3 Switzerland
391407,41462,,,869,"Borrello, L.",Springer,Search for the flavor-changing neutral current interactions of the top quark and the Higgs boson which decays into a pair of b quarks at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2284,0.00043782837127845885,,,nan,,NOT SCOAP3 Switzerland
417694,40642,,,816,"Lujan, P.",Springer,"Search for dark matter in events with energetic, hadronically decaying top quarks and missing transverse momentum at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV",2261,0.0004422821760283061,,,nan,,NOT SCOAP3 Switzerland
417695,40642,,,855,"Borrello, L.",Springer,"Search for dark matter in events with energetic, hadronically decaying top quarks and missing transverse momentum at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV",2261,0.0004422821760283061,,,nan,,NOT SCOAP3 Switzerland
420239,40666,,,737,"Iemmi, F.",Springer,Search for single production of vector-like quarks decaying to a b quark and a Higgs boson,2283,0.0004380201489268506,,,nan,,NOT SCOAP3 Switzerland
420240,40666,,,826,"Lujan, P.",Springer,Search for single production of vector-like quarks decaying to a b quark and a Higgs boson,2283,0.0004380201489268506,,,nan,,NOT SCOAP3 Switzerland
420241,40666,,,833,"Tiko, A.",Springer,Search for single production of vector-like quarks decaying to a b quark and a Higgs boson,2283,0.0004380201489268506,,,nan,,NOT SCOAP3 Switzerland
420242,40666,,,868,"Borrello, L.",Springer,Search for single production of vector-like quarks decaying to a b quark and a Higgs boson,2283,0.0004380201489268506,,,nan,,NOT SCOAP3 Switzerland
429225,40567,,,745,"Iemmi, F.",Springer,Measurements of differential cross sections of top quark pair production as a function of kinematic event variables in proton-proton collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2293,0.0004361098996947231,,,nan,,NOT SCOAP3 Switzerland
429226,40567,,,767,"Latino, G.",Springer,Measurements of differential cross sections of top quark pair production as a function of kinematic event variables in proton-proton collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2293,0.0004361098996947231,,,nan,,NOT SCOAP3 Switzerland
429227,40567,,,834,"Lujan, P.",Springer,Measurements of differential cross sections of top quark pair production as a function of kinematic event variables in proton-proton collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2293,0.0004361098996947231,,,nan,,NOT SCOAP3 Switzerland
429228,40567,,,841,"Tiko, A.",Springer,Measurements of differential cross sections of top quark pair production as a function of kinematic event variables in proton-proton collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2293,0.0004361098996947231,,,nan,,NOT SCOAP3 Switzerland
429229,40567,,,875,"Borrello, L.",Springer,Measurements of differential cross sections of top quark pair production as a function of kinematic event variables in proton-proton collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2293,0.0004361098996947231,,,nan,,NOT SCOAP3 Switzerland
431756,40571,,,774,"Beschi, A.",Springer,Search for lepton flavour violating decays of the Higgs boson to μτ and eτ in proton-proton collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2270,0.0004405286343612335,,,nan,,NOT SCOAP3 Switzerland
431757,40571,,,821,"Lujan, P.",Springer,Search for lepton flavour violating decays of the Higgs boson to μτ and eτ in proton-proton collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2270,0.0004405286343612335,,,nan,,NOT SCOAP3 Switzerland
431758,40571,,,862,"Borrello, L.",Springer,Search for lepton flavour violating decays of the Higgs boson to μτ and eτ in proton-proton collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2270,0.0004405286343612335,,,nan,,NOT SCOAP3 Switzerland
446641,40439,,,773,"Latino, G.",Springer,Search for a heavy right-handed W boson and a heavy neutrino in events with two same-flavor leptons and two jets at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2302,0.0004344048653344917,,,nan,,NOT SCOAP3 Switzerland
446642,40439,,,847,"Tiko, A.",Springer,Search for a heavy right-handed W boson and a heavy neutrino in events with two same-flavor leptons and two jets at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2302,0.0004344048653344917,,,nan,,NOT SCOAP3 Switzerland
446643,40439,,,882,"Borrello, L.",Springer,Search for a heavy right-handed W boson and a heavy neutrino in events with two same-flavor leptons and two jets at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2302,0.0004344048653344917,,,nan,,NOT SCOAP3 Switzerland
460949,40379,,,735,"Iemmi, F.",Springer,Search for decays of stopped exotic long-lived particles produced in proton-proton collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2281,0.00043840420868040335,,,nan,,NOT SCOAP3 Switzerland
460950,40379,,,758,"Latino, G.",Springer,Search for decays of stopped exotic long-lived particles produced in proton-proton collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2281,0.00043840420868040335,,,nan,,NOT SCOAP3 Switzerland
460951,40379,,,824,"Lujan, P.",Springer,Search for decays of stopped exotic long-lived particles produced in proton-proton collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2281,0.00043840420868040335,,,nan,,NOT SCOAP3 Switzerland
460952,40379,,,831,"Tiko, A.",Springer,Search for decays of stopped exotic long-lived particles produced in proton-proton collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2281,0.00043840420868040335,,,nan,,NOT SCOAP3 Switzerland
460953,40379,,,866,"Borrello, L.",Springer,Search for decays of stopped exotic long-lived particles produced in proton-proton collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2281,0.00043840420868040335,,,nan,,NOT SCOAP3 Switzerland
469889,25610,,,772,"Latino, G.",Springer,Search for a heavy resonance decaying to a pair of vector bosons in the lepton plus merged jet final state at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2300,0.0004347826086956522,,,nan,,NOT SCOAP3 Switzerland
469890,25610,,,846,"Tiko, A.",Springer,Search for a heavy resonance decaying to a pair of vector bosons in the lepton plus merged jet final state at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2300,0.0004347826086956522,,,nan,,NOT SCOAP3 Switzerland
469891,25610,,,881,"Borrello, L.",Springer,Search for a heavy resonance decaying to a pair of vector bosons in the lepton plus merged jet final state at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2300,0.0004347826086956522,,,nan,,NOT SCOAP3 Switzerland
479794,25608,,,749,"Iemmi, F.",Springer,Search for natural and split supersymmetry in proton-proton collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV in final states with jets and missing transverse momentum,2301,0.000434593654932638,,,nan,,NOT SCOAP3 Switzerland
479795,25608,,,771,"Latino, G.",Springer,Search for natural and split supersymmetry in proton-proton collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV in final states with jets and missing transverse momentum,2301,0.000434593654932638,,,nan,,NOT SCOAP3 Switzerland
479796,25608,,,845,"Tiko, A.",Springer,Search for natural and split supersymmetry in proton-proton collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV in final states with jets and missing transverse momentum,2301,0.000434593654932638,,,nan,,NOT SCOAP3 Switzerland
479797,25608,,,880,"Borrello, L.",Springer,Search for natural and split supersymmetry in proton-proton collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV in final states with jets and missing transverse momentum,2301,0.000434593654932638,,,nan,,NOT SCOAP3 Switzerland
482372,25607,,,773,"Latino, G.",Springer,"Jet properties in PbPb and pp collisions at  <math><msqrt><msub><mi>s</mi><mrow><mi>N</mi><mspace width=""0.12em""></mspace><mi>N</mi></mrow></msub></msqrt><mo>=</mo><mn>5.02</mn></math> $$ \sqrt{s_{\mathrm{N}\;\mathrm{N}}}=5.02 $$ TeV",2303,0.0004342162396873643,,,nan,,NOT SCOAP3 Switzerland
482373,25607,,,847,"Tiko, A.",Springer,"Jet properties in PbPb and pp collisions at  <math><msqrt><msub><mi>s</mi><mrow><mi>N</mi><mspace width=""0.12em""></mspace><mi>N</mi></mrow></msub></msqrt><mo>=</mo><mn>5.02</mn></math> $$ \sqrt{s_{\mathrm{N}\;\mathrm{N}}}=5.02 $$ TeV",2303,0.0004342162396873643,,,nan,,NOT SCOAP3 Switzerland
482374,25607,,,882,"Borrello, L.",Springer,"Jet properties in PbPb and pp collisions at  <math><msqrt><msub><mi>s</mi><mrow><mi>N</mi><mspace width=""0.12em""></mspace><mi>N</mi></mrow></msub></msqrt><mo>=</mo><mn>5.02</mn></math> $$ \sqrt{s_{\mathrm{N}\;\mathrm{N}}}=5.02 $$ TeV",2303,0.0004342162396873643,,,nan,,NOT SCOAP3 Switzerland
500036,25570,,,747,"Iemmi, F.",Springer,Search for lepton-flavor violating decays of heavy resonances and quantum black holes to eμ final states in proton-proton collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2301,0.000434593654932638,,,nan,,NOT SCOAP3 Switzerland
500037,25570,,,770,"Latino, G.",Springer,Search for lepton-flavor violating decays of heavy resonances and quantum black holes to eμ final states in proton-proton collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2301,0.000434593654932638,,,nan,,NOT SCOAP3 Switzerland
500038,25570,,,839,"Lujan, P.",Springer,Search for lepton-flavor violating decays of heavy resonances and quantum black holes to eμ final states in proton-proton collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2301,0.000434593654932638,,,nan,,NOT SCOAP3 Switzerland
500039,25570,,,846,"Tiko, A.",Springer,Search for lepton-flavor violating decays of heavy resonances and quantum black holes to eμ final states in proton-proton collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2301,0.000434593654932638,,,nan,,NOT SCOAP3 Switzerland
500040,25570,,,880,"Borrello, L.",Springer,Search for lepton-flavor violating decays of heavy resonances and quantum black holes to eμ final states in proton-proton collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2301,0.000434593654932638,,,nan,,NOT SCOAP3 Switzerland
502858,25236,,,702,"Battilana, C.",Springer,Measurement of normalized differential  <math><mi>t</mi><mover><mi>t</mi><mo>¯</mo></mover></math> $$ \mathrm{t}\overline{\mathrm{t}} $$ cross sections in the dilepton channel from pp collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2223,0.000449842555105713,,,nan,,NOT SCOAP3 Switzerland
502859,25236,,,821,"Ressegotti, M.",Springer,Measurement of normalized differential  <math><mi>t</mi><mover><mi>t</mi><mo>¯</mo></mover></math> $$ \mathrm{t}\overline{\mathrm{t}} $$ cross sections in the dilepton channel from pp collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2223,0.000449842555105713,,,nan,,NOT SCOAP3 Switzerland
502860,25236,,,837,"Spiga, D.",Springer,Measurement of normalized differential  <math><mi>t</mi><mover><mi>t</mi><mo>¯</mo></mover></math> $$ \mathrm{t}\overline{\mathrm{t}} $$ cross sections in the dilepton channel from pp collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2223,0.000449842555105713,,,nan,,NOT SCOAP3 Switzerland
502861,25236,,,843,"Borrello, L.",Springer,Measurement of normalized differential  <math><mi>t</mi><mover><mi>t</mi><mo>¯</mo></mover></math> $$ \mathrm{t}\overline{\mathrm{t}} $$ cross sections in the dilepton channel from pp collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2223,0.000449842555105713,,,nan,,NOT SCOAP3 Switzerland
518676,25446,,,3642,"Lujan, P.",Springer,Combination of inclusive and differential  <math><mi>t</mi><mover><mi>t</mi><mo>¯</mo></mover></math> $$ \mathrm{t}\overline{\mathrm{t}} $$ charge asymmetry measurements using ATLAS and CMS data at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>7</mn></math> $$ \sqrt{s}=7 $$ and 8 TeV,5098,0.00019615535504119262,,,nan,,NOT SCOAP3 Switzerland
518677,25446,,,3682,"Borrello, L.",Springer,Combination of inclusive and differential  <math><mi>t</mi><mover><mi>t</mi><mo>¯</mo></mover></math> $$ \mathrm{t}\overline{\mathrm{t}} $$ charge asymmetry measurements using ATLAS and CMS data at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>7</mn></math> $$ \sqrt{s}=7 $$ and 8 TeV,5098,0.00019615535504119262,,,nan,,NOT SCOAP3 Switzerland
537105,25062,,,747,"Iemmi, F.",Springer,Comparing transverse momentum balance of b jet pairs in pp and PbPb collisions at   <math> <msqrt> <msub> <mi>s</mi> <mrow> <mi>N</mi> <mi>N</mi> </mrow> </msub> </msqrt> <mo>=</mo> <mn>5.02</mn> </math>  $$ \sqrt{s_{\mathrm{NN}}}=5.02 $$  TeV,2297,0.00043535045711797995,,,nan,,NOT SCOAP3 Switzerland
537106,25062,,,770,"Latino, G.",Springer,Comparing transverse momentum balance of b jet pairs in pp and PbPb collisions at   <math> <msqrt> <msub> <mi>s</mi> <mrow> <mi>N</mi> <mi>N</mi> </mrow> </msub> </msqrt> <mo>=</mo> <mn>5.02</mn> </math>  $$ \sqrt{s_{\mathrm{NN}}}=5.02 $$  TeV,2297,0.00043535045711797995,,,nan,,NOT SCOAP3 Switzerland
537107,25062,,,839,"Lujan, P.",Springer,Comparing transverse momentum balance of b jet pairs in pp and PbPb collisions at   <math> <msqrt> <msub> <mi>s</mi> <mrow> <mi>N</mi> <mi>N</mi> </mrow> </msub> </msqrt> <mo>=</mo> <mn>5.02</mn> </math>  $$ \sqrt{s_{\mathrm{NN}}}=5.02 $$  TeV,2297,0.00043535045711797995,,,nan,,NOT SCOAP3 Switzerland
537108,25062,,,845,"Tiko, A.",Springer,Comparing transverse momentum balance of b jet pairs in pp and PbPb collisions at   <math> <msqrt> <msub> <mi>s</mi> <mrow> <mi>N</mi> <mi>N</mi> </mrow> </msub> </msqrt> <mo>=</mo> <mn>5.02</mn> </math>  $$ \sqrt{s_{\mathrm{NN}}}=5.02 $$  TeV,2297,0.00043535045711797995,,,nan,,NOT SCOAP3 Switzerland
537109,25062,,,880,"Borrello, L.",Springer,Comparing transverse momentum balance of b jet pairs in pp and PbPb collisions at   <math> <msqrt> <msub> <mi>s</mi> <mrow> <mi>N</mi> <mi>N</mi> </mrow> </msub> </msqrt> <mo>=</mo> <mn>5.02</mn> </math>  $$ \sqrt{s_{\mathrm{NN}}}=5.02 $$  TeV,2297,0.00043535045711797995,,,nan,,NOT SCOAP3 Switzerland
543699,24838,,,816,"Lujan, P.",Springer,Measurement of differential cross sections in the kinematic angular variable ϕ * for inclusive Z boson production in pp collisions at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>8</mn> </math>  $$ \sqrt{s}=8 $$  TeV,2262,0.0004420866489832007,,,nan,,NOT SCOAP3 Switzerland
543700,24838,,,856,"Borrello, L.",Springer,Measurement of differential cross sections in the kinematic angular variable ϕ * for inclusive Z boson production in pp collisions at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>8</mn> </math>  $$ \sqrt{s}=8 $$  TeV,2262,0.0004420866489832007,,,nan,,NOT SCOAP3 Switzerland
552322,24841,,,847,"Borrello, L.",Springer,Combined search for electroweak production of charginos and neutralinos in proton-proton collisions at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>13</mn> </math>  $$ \sqrt{s}=13 $$  TeV,2253,0.0004438526409232135,,,nan,,NOT SCOAP3 Switzerland
554809,25079,,,709,"Battilana, C.",Springer,Search for natural supersymmetry in events with top quark pairs and photons in pp collisions at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>8</mn> </math>  $$ \sqrt{s}=8 $$  TeV,2226,0.0004492362982929021,,,nan,,NOT SCOAP3 Switzerland
554810,25079,,,767,"Ciriolo, V.",Springer,Search for natural supersymmetry in events with top quark pairs and photons in pp collisions at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>8</mn> </math>  $$ \sqrt{s}=8 $$  TeV,2226,0.0004492362982929021,,,nan,,NOT SCOAP3 Switzerland
554811,25079,,,827,"Ressegotti, M.",Springer,Search for natural supersymmetry in events with top quark pairs and photons in pp collisions at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>8</mn> </math>  $$ \sqrt{s}=8 $$  TeV,2226,0.0004492362982929021,,,nan,,NOT SCOAP3 Switzerland
557302,25078,,,825,"Ressegotti, M.",Springer,Search for electroweak production of charginos and neutralinos in multilepton final states in proton-proton collisions at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>13</mn> </math>  $$ \sqrt{s}=13 $$  TeV,2233,0.0004478280340349306,,,nan,,NOT SCOAP3 Switzerland
557303,25078,,,850,"Borrello, L.",Springer,Search for electroweak production of charginos and neutralinos in multilepton final states in proton-proton collisions at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>13</mn> </math>  $$ \sqrt{s}=13 $$  TeV,2233,0.0004478280340349306,,,nan,,NOT SCOAP3 Switzerland
557304,25078,,,1071,"Oreshkin, V.",Springer,Search for electroweak production of charginos and neutralinos in multilepton final states in proton-proton collisions at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>13</mn> </math>  $$ \sqrt{s}=13 $$  TeV,2233,0.0004478280340349306,,,nan,,NOT SCOAP3 Switzerland
570067,24527,,,808,"Lujan, P.",Springer,Measurement of the inclusive  <math><mi>t</mi><mover><mi>t</mi><mo>¯</mo></mover></math> $$ \mathrm{t}\overline{\mathrm{t}} $$ cross section in pp collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>5.02</mn></math> $$ \sqrt{s}=5.02 $$ TeV using final states with at least one charged lepton,2239,0.00044662795891022776,,,nan,,NOT SCOAP3 Switzerland
570068,24527,,,824,"Ressegotti, M.",Springer,Measurement of the inclusive  <math><mi>t</mi><mover><mi>t</mi><mo>¯</mo></mover></math> $$ \mathrm{t}\overline{\mathrm{t}} $$ cross section in pp collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>5.02</mn></math> $$ \sqrt{s}=5.02 $$ TeV using final states with at least one charged lepton,2239,0.00044662795891022776,,,nan,,NOT SCOAP3 Switzerland
570069,24527,,,848,"Borrello, L.",Springer,Measurement of the inclusive  <math><mi>t</mi><mover><mi>t</mi><mo>¯</mo></mover></math> $$ \mathrm{t}\overline{\mathrm{t}} $$ cross section in pp collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>5.02</mn></math> $$ \sqrt{s}=5.02 $$ TeV using final states with at least one charged lepton,2239,0.00044662795891022776,,,nan,,NOT SCOAP3 Switzerland
587615,41209,,,806,"Lujan, P.",Springer,"Search for new phenomena in final states with two opposite-charge, same-flavor leptons, jets, and missing transverse momentum in pp collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV",2239,0.00044662795891022776,,,nan,,NOT SCOAP3 Switzerland
587616,41209,,,822,"Ressegotti, M.",Springer,"Search for new phenomena in final states with two opposite-charge, same-flavor leptons, jets, and missing transverse momentum in pp collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV",2239,0.00044662795891022776,,,nan,,NOT SCOAP3 Switzerland
587617,41209,,,847,"Borrello, L.",Springer,"Search for new phenomena in final states with two opposite-charge, same-flavor leptons, jets, and missing transverse momentum in pp collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV",2239,0.00044662795891022776,,,nan,,NOT SCOAP3 Switzerland
590343,44027,,,806,"Lujan, P.",Springer,"Search for new phenomena in final states with two opposite-charge, same-flavor leptons, jets, and missing transverse momentum in pp collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV",2239,0.00044662795891022776,,,nan,,NOT SCOAP3 Switzerland
590344,44027,,,822,"Ressegotti, M.",Springer,"Search for new phenomena in final states with two opposite-charge, same-flavor leptons, jets, and missing transverse momentum in pp collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV",2239,0.00044662795891022776,,,nan,,NOT SCOAP3 Switzerland
590345,44027,,,847,"Borrello, L.",Springer,"Search for new phenomena in final states with two opposite-charge, same-flavor leptons, jets, and missing transverse momentum in pp collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV",2239,0.00044662795891022776,,,nan,,NOT SCOAP3 Switzerland
604300,24178,,,822,"Lujan, P.",Springer,Search for ZZ resonances in the 2ℓ2ν final state in proton-proton collisions at 13 TeV,2280,0.0004385964912280702,,,nan,,NOT SCOAP3 Switzerland
604301,24178,,,863,"Borrello, L.",Springer,Search for ZZ resonances in the 2ℓ2ν final state in proton-proton collisions at 13 TeV,2280,0.0004385964912280702,,,nan,,NOT SCOAP3 Switzerland
612889,24041,,,2,"Vairinhos, Hélvio",APS,Strong-coupling lattice QCD on anisotropic lattices,3,0.3333333333333333,,,nan,,NOT SCOAP3 Switzerland
653204,23808,,,806,"Lujan, P.",Springer/SISSA,"Search for supersymmetry in events with at least three electrons or muons, jets, and missing transverse momentum in proton-proton collisions at s = 13 $$ \sqrt{s}=13 $$ TeV",2236,0.0004472271914132379,,,nan,,NOT SCOAP3 Switzerland
653205,23808,,,846,"Borrello, L.",Springer/SISSA,"Search for supersymmetry in events with at least three electrons or muons, jets, and missing transverse momentum in proton-proton collisions at s = 13 $$ \sqrt{s}=13 $$ TeV",2236,0.0004472271914132379,,,nan,,NOT SCOAP3 Switzerland
667430,23728,,,805,"Lujan, P.",Springer/SISSA,Constraints on the double-parton scattering cross section from same-sign W boson pair production in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2230,0.0004484304932735426,,,nan,,NOT SCOAP3 Switzerland
667431,23728,,,844,"Borrello, L.",Springer/SISSA,Constraints on the double-parton scattering cross section from same-sign W boson pair production in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2230,0.0004484304932735426,,,nan,,NOT SCOAP3 Switzerland
695969,23383,,,810,"Lujan, P.",Springer,Search for low mass vector resonances decaying into quark-antiquark pairs in proton-proton collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2263,0.0004418912947414936,,,nan,,NOT SCOAP3 Switzerland
695970,23383,,,850,"Borrello, L.",Springer,Search for low mass vector resonances decaying into quark-antiquark pairs in proton-proton collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2263,0.0004418912947414936,,,nan,,NOT SCOAP3 Switzerland
707088,23138,,,767,"Gundacker, S.",Springer,Search for resonant and nonresonant Higgs boson pair production in the  <math><mi>b</mi><mover><mi>b</mi><mo>¯</mo></mover><mi>ℓνℓν</mi></math> $$ \mathrm{b}\overline{\mathrm{b}}\mathit{\ell \nu \ell \nu } $$ final state in proton-proton collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2235,0.00044742729306487697,,,nan,,NOT SCOAP3 Switzerland
707089,23138,,,807,"Lujan, P.",Springer,Search for resonant and nonresonant Higgs boson pair production in the  <math><mi>b</mi><mover><mi>b</mi><mo>¯</mo></mover><mi>ℓνℓν</mi></math> $$ \mathrm{b}\overline{\mathrm{b}}\mathit{\ell \nu \ell \nu } $$ final state in proton-proton collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2235,0.00044742729306487697,,,nan,,NOT SCOAP3 Switzerland
707090,23138,,,822,"Ressegotti, M.",Springer,Search for resonant and nonresonant Higgs boson pair production in the  <math><mi>b</mi><mover><mi>b</mi><mo>¯</mo></mover><mi>ℓνℓν</mi></math> $$ \mathrm{b}\overline{\mathrm{b}}\mathit{\ell \nu \ell \nu } $$ final state in proton-proton collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2235,0.00044742729306487697,,,nan,,NOT SCOAP3 Switzerland
707091,23138,,,847,"Borrello, L.",Springer,Search for resonant and nonresonant Higgs boson pair production in the  <math><mi>b</mi><mover><mi>b</mi><mo>¯</mo></mover><mi>ℓνℓν</mi></math> $$ \mathrm{b}\overline{\mathrm{b}}\mathit{\ell \nu \ell \nu } $$ final state in proton-proton collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2235,0.00044742729306487697,,,nan,,NOT SCOAP3 Switzerland
712723,23202,,,714,"Battilana, C.",Springer,Erratum 2: Search for dark matter and unparticles in events with a Z boson and missing transverse momentum in proton-proton collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2244,0.000445632798573975,,,nan,,NOT SCOAP3 Switzerland
712724,23202,,,770,"Ciriolo, V.",Springer,Erratum 2: Search for dark matter and unparticles in events with a Z boson and missing transverse momentum in proton-proton collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2244,0.000445632798573975,,,nan,,NOT SCOAP3 Switzerland
712725,23202,,,788,"Nardo, G.",Springer,Erratum 2: Search for dark matter and unparticles in events with a Z boson and missing transverse momentum in proton-proton collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2244,0.000445632798573975,,,nan,,NOT SCOAP3 Switzerland
712726,23202,,,855,"Fedi, G.",Springer,Erratum 2: Search for dark matter and unparticles in events with a Z boson and missing transverse momentum in proton-proton collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2244,0.000445632798573975,,,nan,,NOT SCOAP3 Switzerland
718333,23232,,,767,"Beschi, A.",Springer,Pseudorapidity distributions of charged hadrons in proton-lead collisions at  <math><msqrt><msub><mi>s</mi><mrow><mi>N</mi><mi>N</mi></mrow></msub></msqrt><mo>=</mo><mn>5.02</mn></math> $$ \sqrt{s_{\mathrm{NN}}}=5.02 $$ and 8.16 TeV,2258,0.0004428697962798937,,,nan,,NOT SCOAP3 Switzerland
718334,23232,,,854,"Borrello, L.",Springer,Pseudorapidity distributions of charged hadrons in proton-lead collisions at  <math><msqrt><msub><mi>s</mi><mrow><mi>N</mi><mi>N</mi></mrow></msub></msqrt><mo>=</mo><mn>5.02</mn></math> $$ \sqrt{s_{\mathrm{NN}}}=5.02 $$ and 8.16 TeV,2258,0.0004428697962798937,,,nan,,NOT SCOAP3 Switzerland
723998,22969,,,824,"Ressegotti, M.",Springer/SISSA,"Search for supersymmetry in events with at least one photon, missing transverse momentum, and large transverse event activity in proton-proton collisions at s = 13 $$ \sqrt{s}=13 $$ TeV",2231,0.00044822949350067237,,,nan,,NOT SCOAP3 Switzerland
723999,22969,,,849,"Borrello, L.",Springer/SISSA,"Search for supersymmetry in events with at least one photon, missing transverse momentum, and large transverse event activity in proton-proton collisions at s = 13 $$ \sqrt{s}=13 $$ TeV",2231,0.00044822949350067237,,,nan,,NOT SCOAP3 Switzerland
755614,22677,,,455,"Chen, S.",Springer/SISSA,Evidence for the H → b b ¯ $$ H\to b\overline{b} $$ decay with the ATLAS detector,2897,0.00034518467380048324,,,nan,,NOT SCOAP3 Switzerland
755615,22677,,,1198,"Jin, S.",Springer/SISSA,Evidence for the H → b b ¯ $$ H\to b\overline{b} $$ decay with the ATLAS detector,2897,0.00034518467380048324,,,nan,,NOT SCOAP3 Switzerland
755616,22677,,,2699,"Wang, C.",Springer/SISSA,Evidence for the H → b b ¯ $$ H\to b\overline{b} $$ decay with the ATLAS detector,2897,0.00034518467380048324,,,nan,,NOT SCOAP3 Switzerland
755617,22677,,,2860,"Zhang, P.",Springer/SISSA,Evidence for the H → b b ¯ $$ H\to b\overline{b} $$ decay with the ATLAS detector,2897,0.00034518467380048324,,,nan,,NOT SCOAP3 Switzerland
793249,22373,,,705,"Battilana, C.",Springer,Search for pair production of vector-like T and B quarks in single-lepton final states using boosted jet substructure in proton-proton collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2226,0.0004492362982929021,,,nan,,NOT SCOAP3 Switzerland
793250,22373,,,822,"Ressegotti, M.",Springer,Search for pair production of vector-like T and B quarks in single-lepton final states using boosted jet substructure in proton-proton collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2226,0.0004492362982929021,,,nan,,NOT SCOAP3 Switzerland
793251,22373,,,838,"Spiga, D.",Springer,Search for pair production of vector-like T and B quarks in single-lepton final states using boosted jet substructure in proton-proton collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2226,0.0004492362982929021,,,nan,,NOT SCOAP3 Switzerland
793252,22373,,,844,"Borrello, L.",Springer,Search for pair production of vector-like T and B quarks in single-lepton final states using boosted jet substructure in proton-proton collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2226,0.0004492362982929021,,,nan,,NOT SCOAP3 Switzerland
799680,22309,,,803,"Lujan, P.",Springer,Measurements of properties of the Higgs boson decaying into the four-lepton final state in pp collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2240,0.0004464285714285714,,,nan,,NOT SCOAP3 Switzerland
799681,22309,,,821,"Ressegotti, M.",Springer,Measurements of properties of the Higgs boson decaying into the four-lepton final state in pp collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2240,0.0004464285714285714,,,nan,,NOT SCOAP3 Switzerland
799682,22309,,,846,"Borrello, L.",Springer,Measurements of properties of the Higgs boson decaying into the four-lepton final state in pp collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2240,0.0004464285714285714,,,nan,,NOT SCOAP3 Switzerland
799683,22309,,,891,"Cappati, A.",Springer,Measurements of properties of the Higgs boson decaying into the four-lepton final state in pp collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2240,0.0004464285714285714,,,nan,,NOT SCOAP3 Switzerland
803090,22325,,,825,"Ressegotti, M.",Springer,Search for electroweak production of charginos and neutralinos in WH events in proton-proton collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2232,0.00044802867383512545,,,nan,,NOT SCOAP3 Switzerland
803091,22325,,,850,"Borrello, L.",Springer,Search for electroweak production of charginos and neutralinos in WH events in proton-proton collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn></math> $$ \sqrt{s}=13 $$ TeV,2232,0.00044802867383512545,,,nan,,NOT SCOAP3 Switzerland
813396,22238,,,767,"Gundacker, S.",Springer,Search for a light pseudoscalar Higgs boson produced in association with bottom quarks in pp collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>8</mn></math> $$ \sqrt{s}=8 $$ TeV,2235,0.00044742729306487697,,,nan,,NOT SCOAP3 Switzerland
813397,22238,,,806,"Lujan, P.",Springer,Search for a light pseudoscalar Higgs boson produced in association with bottom quarks in pp collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>8</mn></math> $$ \sqrt{s}=8 $$ TeV,2235,0.00044742729306487697,,,nan,,NOT SCOAP3 Switzerland
813398,22238,,,822,"Ressegotti, M.",Springer,Search for a light pseudoscalar Higgs boson produced in association with bottom quarks in pp collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>8</mn></math> $$ \sqrt{s}=8 $$ TeV,2235,0.00044742729306487697,,,nan,,NOT SCOAP3 Switzerland
813399,22238,,,847,"Borrello, L.",Springer,Search for a light pseudoscalar Higgs boson produced in association with bottom quarks in pp collisions at  <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>8</mn></math> $$ \sqrt{s}=8 $$ TeV,2235,0.00044742729306487697,,,nan,,NOT SCOAP3 Switzerland
827452,22254,,,705,"Battilana, C.",Springer/SISSA,Search for associated production of dark matter with a Higgs boson decaying to b b ¯ $$ \mathrm{b}\overline{\mathrm{b}} $$ or γγ at s = 13 $$ \sqrt{s}=13 $$ TeV,2233,0.0004478280340349306,,,nan,,NOT SCOAP3 Switzerland
827453,22254,,,763,"Ciriolo, V.",Springer/SISSA,Search for associated production of dark matter with a Higgs boson decaying to b b ¯ $$ \mathrm{b}\overline{\mathrm{b}} $$ or γγ at s = 13 $$ \sqrt{s}=13 $$ TeV,2233,0.0004478280340349306,,,nan,,NOT SCOAP3 Switzerland
827454,22254,,,781,"Nardo, G.",Springer/SISSA,Search for associated production of dark matter with a Higgs boson decaying to b b ¯ $$ \mathrm{b}\overline{\mathrm{b}} $$ or γγ at s = 13 $$ \sqrt{s}=13 $$ TeV,2233,0.0004478280340349306,,,nan,,NOT SCOAP3 Switzerland
827455,22254,,,825,"Ressegotti, M.",Springer/SISSA,Search for associated production of dark matter with a Higgs boson decaying to b b ¯ $$ \mathrm{b}\overline{\mathrm{b}} $$ or γγ at s = 13 $$ \sqrt{s}=13 $$ TeV,2233,0.0004478280340349306,,,nan,,NOT SCOAP3 Switzerland
827456,22254,,,849,"Fedi, G.",Springer/SISSA,Search for associated production of dark matter with a Higgs boson decaying to b b ¯ $$ \mathrm{b}\overline{\mathrm{b}} $$ or γγ at s = 13 $$ \sqrt{s}=13 $$ TeV,2233,0.0004478280340349306,,,nan,,NOT SCOAP3 Switzerland
842814,21997,,,704,"Battilana, C.",Springer/SISSA,Measurements of jet charge with dijet events in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2228,0.0004488330341113106,,,nan,,NOT SCOAP3 Switzerland
842815,21997,,,762,"Ciriolo, V.",Springer/SISSA,Measurements of jet charge with dijet events in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2228,0.0004488330341113106,,,nan,,NOT SCOAP3 Switzerland
842816,21997,,,780,"Nardo, G.",Springer/SISSA,Measurements of jet charge with dijet events in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2228,0.0004488330341113106,,,nan,,NOT SCOAP3 Switzerland
842817,21997,,,846,"Fedi, G.",Springer/SISSA,Measurements of jet charge with dijet events in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2228,0.0004488330341113106,,,nan,,NOT SCOAP3 Switzerland
854931,21891,,,709,"Battilana, C.",Springer/SISSA,Measurements of the pp → Wγγ and pp → Zγγ cross sections and limits on anomalous quartic gauge couplings at s = 8 $$ \sqrt{s}=8 $$ TeV,2228,0.0004488330341113106,,,nan,,NOT SCOAP3 Switzerland
854932,21891,,,767,"Ciriolo, V.",Springer/SISSA,Measurements of the pp → Wγγ and pp → Zγγ cross sections and limits on anomalous quartic gauge couplings at s = 8 $$ \sqrt{s}=8 $$ TeV,2228,0.0004488330341113106,,,nan,,NOT SCOAP3 Switzerland
854933,21891,,,829,"Ressegotti, M.",Springer/SISSA,Measurements of the pp → Wγγ and pp → Zγγ cross sections and limits on anomalous quartic gauge couplings at s = 8 $$ \sqrt{s}=8 $$ TeV,2228,0.0004488330341113106,,,nan,,NOT SCOAP3 Switzerland
860454,21916,,,689,"Battilana, C.",Springer/SISSA,Search for new physics in the monophoton final state in proton-proton collisions at s = 13 $$ \sqrt{s}=13 $$ TeV,2206,0.00045330915684496827,,,nan,,NOT SCOAP3 Switzerland
860455,21916,,,747,"Ciriolo, V.",Springer/SISSA,Search for new physics in the monophoton final state in proton-proton collisions at s = 13 $$ \sqrt{s}=13 $$ TeV,2206,0.00045330915684496827,,,nan,,NOT SCOAP3 Switzerland
860456,21916,,,807,"Ressegotti, M.",Springer/SISSA,Search for new physics in the monophoton final state in proton-proton collisions at s = 13 $$ \sqrt{s}=13 $$ TeV,2206,0.00045330915684496827,,,nan,,NOT SCOAP3 Switzerland
862980,21930,,,162,"Vargas, J.",Springer/SISSA,Search for light bosons in decays of the 125 GeV Higgs boson in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2270,0.0004405286343612335,,,nan,,NOT SCOAP3 Switzerland
862981,21930,,,717,"Battilana, C.",Springer/SISSA,Search for light bosons in decays of the 125 GeV Higgs boson in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2270,0.0004405286343612335,,,nan,,NOT SCOAP3 Switzerland
862982,21930,,,778,"Malberti, M.",Springer/SISSA,Search for light bosons in decays of the 125 GeV Higgs boson in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2270,0.0004405286343612335,,,nan,,NOT SCOAP3 Switzerland
862983,21930,,,785,"Pigazzini, S.",Springer/SISSA,Search for light bosons in decays of the 125 GeV Higgs boson in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2270,0.0004405286343612335,,,nan,,NOT SCOAP3 Switzerland
862984,21930,,,790,"Nardo, G.",Springer/SISSA,Search for light bosons in decays of the 125 GeV Higgs boson in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2270,0.0004405286343612335,,,nan,,NOT SCOAP3 Switzerland
862985,21930,,,801,"Thyssen, F.",Springer/SISSA,Search for light bosons in decays of the 125 GeV Higgs boson in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2270,0.0004405286343612335,,,nan,,NOT SCOAP3 Switzerland
862986,21930,,,825,"Zanetti, M.",Springer/SISSA,Search for light bosons in decays of the 125 GeV Higgs boson in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2270,0.0004405286343612335,,,nan,,NOT SCOAP3 Switzerland
862987,21930,,,856,"Fedi, G.",Springer/SISSA,Search for light bosons in decays of the 125 GeV Higgs boson in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2270,0.0004405286343612335,,,nan,,NOT SCOAP3 Switzerland
868854,21814,,,825,"Ressegotti, M.",Springer/SISSA,Search for top squark pair production in pp collisions at s = 13 $$ \sqrt{s}=13 $$ TeV using single lepton events,2232,0.00044802867383512545,,,nan,,NOT SCOAP3 Switzerland
868855,21814,,,850,"Borrello, L.",Springer/SISSA,Search for top squark pair production in pp collisions at s = 13 $$ \sqrt{s}=13 $$ TeV using single lepton events,2232,0.00044802867383512545,,,nan,,NOT SCOAP3 Switzerland
871358,21780,,,825,"Ressegotti, M.",Springer/SISSA,Search for direct production of supersymmetric partners of the top quark in the all-jets final state in proton-proton collisions at s = 13 $$ \sqrt{s}=13 $$ TeV,2233,0.0004478280340349306,,,nan,,NOT SCOAP3 Switzerland
871359,21780,,,850,"Borrello, L.",Springer/SISSA,Search for direct production of supersymmetric partners of the top quark in the all-jets final state in proton-proton collisions at s = 13 $$ \sqrt{s}=13 $$ TeV,2233,0.0004478280340349306,,,nan,,NOT SCOAP3 Switzerland
873849,21781,,,704,"Battilana, C.",Springer/SISSA,Measurement of the semileptonic t t ¯ $$ \mathrm{t}\overline{\mathrm{t}} $$ + γ production cross section in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2230,0.0004484304932735426,,,nan,,NOT SCOAP3 Switzerland
873850,21781,,,762,"Ciriolo, V.",Springer/SISSA,Measurement of the semileptonic t t ¯ $$ \mathrm{t}\overline{\mathrm{t}} $$ + γ production cross section in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2230,0.0004484304932735426,,,nan,,NOT SCOAP3 Switzerland
873851,21781,,,780,"Nardo, G.",Springer/SISSA,Measurement of the semileptonic t t ¯ $$ \mathrm{t}\overline{\mathrm{t}} $$ + γ production cross section in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2230,0.0004484304932735426,,,nan,,NOT SCOAP3 Switzerland
873852,21781,,,848,"Fedi, G.",Springer/SISSA,Measurement of the semileptonic t t ¯ $$ \mathrm{t}\overline{\mathrm{t}} $$ + γ production cross section in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2230,0.0004484304932735426,,,nan,,NOT SCOAP3 Switzerland
896368,21747,,,714,"Battilana, C.",Springer,Erratum to: Search for dark matter and unparticles in events with a Z boson and missing transverse momentum in proton-proton collisions at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>13</mn> </math>  $$ \sqrt{s}=13 $$  TeV,2244,0.000445632798573975,,,nan,,NOT SCOAP3 Switzerland
896369,21747,,,770,"Ciriolo, V.",Springer,Erratum to: Search for dark matter and unparticles in events with a Z boson and missing transverse momentum in proton-proton collisions at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>13</mn> </math>  $$ \sqrt{s}=13 $$  TeV,2244,0.000445632798573975,,,nan,,NOT SCOAP3 Switzerland
896370,21747,,,788,"Nardo, G.",Springer,Erratum to: Search for dark matter and unparticles in events with a Z boson and missing transverse momentum in proton-proton collisions at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>13</mn> </math>  $$ \sqrt{s}=13 $$  TeV,2244,0.000445632798573975,,,nan,,NOT SCOAP3 Switzerland
896371,21747,,,855,"Fedi, G.",Springer,Erratum to: Search for dark matter and unparticles in events with a Z boson and missing transverse momentum in proton-proton collisions at   <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>13</mn> </math>  $$ \sqrt{s}=13 $$  TeV,2244,0.000445632798573975,,,nan,,NOT SCOAP3 Switzerland
906445,21518,,,704,"Battilana, C.",Springer/SISSA,Search for a heavy resonance decaying to a top quark and a vector-like top quark at s = 13 $$ \sqrt{s}=13 $$ TeV,2230,0.0004484304932735426,,,nan,,NOT SCOAP3 Switzerland
906446,21518,,,762,"Ciriolo, V.",Springer/SISSA,Search for a heavy resonance decaying to a top quark and a vector-like top quark at s = 13 $$ \sqrt{s}=13 $$ TeV,2230,0.0004484304932735426,,,nan,,NOT SCOAP3 Switzerland
906447,21518,,,780,"Nardo, G.",Springer/SISSA,Search for a heavy resonance decaying to a top quark and a vector-like top quark at s = 13 $$ \sqrt{s}=13 $$ TeV,2230,0.0004484304932735426,,,nan,,NOT SCOAP3 Switzerland
906448,21518,,,848,"Fedi, G.",Springer/SISSA,Search for a heavy resonance decaying to a top quark and a vector-like top quark at s = 13 $$ \sqrt{s}=13 $$ TeV,2230,0.0004484304932735426,,,nan,,NOT SCOAP3 Switzerland
908950,21491,,,714,"Battilana, C.",Springer/SISSA,Measurement of the t t ¯ $$ \mathrm{t}\overline{\mathrm{t}} $$ production cross section using events with one lepton and at least one jet in pp collisions at s = 13 $$ \sqrt{s}=13 $$ TeV,2245,0.00044543429844097997,,,nan,,NOT SCOAP3 Switzerland
908951,21491,,,770,"Ciriolo, V.",Springer/SISSA,Measurement of the t t ¯ $$ \mathrm{t}\overline{\mathrm{t}} $$ production cross section using events with one lepton and at least one jet in pp collisions at s = 13 $$ \sqrt{s}=13 $$ TeV,2245,0.00044543429844097997,,,nan,,NOT SCOAP3 Switzerland
908952,21491,,,788,"Nardo, G.",Springer/SISSA,Measurement of the t t ¯ $$ \mathrm{t}\overline{\mathrm{t}} $$ production cross section using events with one lepton and at least one jet in pp collisions at s = 13 $$ \sqrt{s}=13 $$ TeV,2245,0.00044543429844097997,,,nan,,NOT SCOAP3 Switzerland
908953,21491,,,854,"Fedi, G.",Springer/SISSA,Measurement of the t t ¯ $$ \mathrm{t}\overline{\mathrm{t}} $$ production cross section using events with one lepton and at least one jet in pp collisions at s = 13 $$ \sqrt{s}=13 $$ TeV,2245,0.00044543429844097997,,,nan,,NOT SCOAP3 Switzerland
914477,21399,,,65,"Ancu, L.",Springer/SISSA,Measurement of the inclusive jet cross-sections in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV with the ATLAS detector,2852,0.0003506311360448808,,,nan,,NOT SCOAP3 Switzerland
914478,21399,,,205,"Benoit, M.",Springer/SISSA,Measurement of the inclusive jet cross-sections in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV with the ATLAS detector,2852,0.0003506311360448808,,,nan,,NOT SCOAP3 Switzerland
914479,21399,,,241,"Bilbao De Mendizabal, J.",Springer/SISSA,Measurement of the inclusive jet cross-sections in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV with the ATLAS detector,2852,0.0003506311360448808,,,nan,,NOT SCOAP3 Switzerland
914480,21399,,,366,"Calace, N.",Springer/SISSA,Measurement of the inclusive jet cross-sections in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV with the ATLAS detector,2852,0.0003506311360448808,,,nan,,NOT SCOAP3 Switzerland
914481,21399,,,442,"Chatterjee, A.",Springer/SISSA,Measurement of the inclusive jet cross-sections in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV with the ATLAS detector,2852,0.0003506311360448808,,,nan,,NOT SCOAP3 Switzerland
914482,21399,,,495,"Clark, A.",Springer/SISSA,Measurement of the inclusive jet cross-sections in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV with the ATLAS detector,2852,0.0003506311360448808,,,nan,,NOT SCOAP3 Switzerland
914483,21399,,,503,"Coccaro, A.",Springer/SISSA,Measurement of the inclusive jet cross-sections in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV with the ATLAS detector,2852,0.0003506311360448808,,,nan,,NOT SCOAP3 Switzerland
914484,21399,,,610,"Delitzsch, C.",Springer/SISSA,Measurement of the inclusive jet cross-sections in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV with the ATLAS detector,2852,0.0003506311360448808,,,nan,,NOT SCOAP3 Switzerland
914485,21399,,,615,"Volpe, D.",Springer/SISSA,Measurement of the inclusive jet cross-sections in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV with the ATLAS detector,2852,0.0003506311360448808,,,nan,,NOT SCOAP3 Switzerland
914486,21399,,,660,"Djobava, T.",Springer/SISSA,Measurement of the inclusive jet cross-sections in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV with the ATLAS detector,2852,0.0003506311360448808,,,nan,,NOT SCOAP3 Switzerland
914487,21399,,,696,"Durglishvili, A.",Springer/SISSA,Measurement of the inclusive jet cross-sections in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV with the ATLAS detector,2852,0.0003506311360448808,,,nan,,NOT SCOAP3 Switzerland
914488,21399,,,778,"Ferrere, D.",Springer/SISSA,Measurement of the inclusive jet cross-sections in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV with the ATLAS detector,2852,0.0003506311360448808,,,nan,,NOT SCOAP3 Switzerland
914489,21399,,,906,"Golling, T.",Springer/SISSA,Measurement of the inclusive jet cross-sections in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV with the ATLAS detector,2852,0.0003506311360448808,,,nan,,NOT SCOAP3 Switzerland
914490,21399,,,916,"Gonzalez-Sevilla, S.",Springer/SISSA,Measurement of the inclusive jet cross-sections in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV with the ATLAS detector,2852,0.0003506311360448808,,,nan,,NOT SCOAP3 Switzerland
914491,21399,,,935,"Gramling, J.",Springer/SISSA,Measurement of the inclusive jet cross-sections in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV with the ATLAS detector,2852,0.0003506311360448808,,,nan,,NOT SCOAP3 Switzerland
914492,21399,,,1127,"Iacobucci, G.",Springer/SISSA,Measurement of the inclusive jet cross-sections in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV with the ATLAS detector,2852,0.0003506311360448808,,,nan,,NOT SCOAP3 Switzerland
914493,21399,,,1240,"Katre, A.",Springer/SISSA,Measurement of the inclusive jet cross-sections in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV with the ATLAS detector,2852,0.0003506311360448808,,,nan,,NOT SCOAP3 Switzerland
914494,21399,,,1263,"Khoo, T.",Springer/SISSA,Measurement of the inclusive jet cross-sections in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV with the ATLAS detector,2852,0.0003506311360448808,,,nan,,NOT SCOAP3 Switzerland
914495,21399,,,1415,"Lanfermann, M.",Springer/SISSA,Measurement of the inclusive jet cross-sections in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV with the ATLAS detector,2852,0.0003506311360448808,,,nan,,NOT SCOAP3 Switzerland
914496,21399,,,1492,"Lionti, A.",Springer/SISSA,Measurement of the inclusive jet cross-sections in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV with the ATLAS detector,2852,0.0003506311360448808,,,nan,,NOT SCOAP3 Switzerland
914497,21399,,,1610,"March, L.",Springer/SISSA,Measurement of the inclusive jet cross-sections in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV with the ATLAS detector,2852,0.0003506311360448808,,,nan,,NOT SCOAP3 Switzerland
914498,21399,,,1679,"Mermod, P.",Springer/SISSA,Measurement of the inclusive jet cross-sections in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV with the ATLAS detector,2852,0.0003506311360448808,,,nan,,NOT SCOAP3 Switzerland
914499,21399,,,1752,"Mosidze, M.",Springer/SISSA,Measurement of the inclusive jet cross-sections in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV with the ATLAS detector,2852,0.0003506311360448808,,,nan,,NOT SCOAP3 Switzerland
914500,21399,,,1774,"Nackenhorst, O.",Springer/SISSA,Measurement of the inclusive jet cross-sections in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV with the ATLAS detector,2852,0.0003506311360448808,,,nan,,NOT SCOAP3 Switzerland
914501,21399,,,1908,"Paolozzi, L.",Springer/SISSA,Measurement of the inclusive jet cross-sections in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV with the ATLAS detector,2852,0.0003506311360448808,,,nan,,NOT SCOAP3 Switzerland
914502,21399,,,2078,"Ristić, B.",Springer/SISSA,Measurement of the inclusive jet cross-sections in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV with the ATLAS detector,2852,0.0003506311360448808,,,nan,,NOT SCOAP3 Switzerland
914503,21399,,,2233,"Schramm, S.",Springer/SISSA,Measurement of the inclusive jet cross-sections in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV with the ATLAS detector,2852,0.0003506311360448808,,,nan,,NOT SCOAP3 Switzerland
914504,21399,,,2270,"Sfyrla, A.",Springer/SISSA,Measurement of the inclusive jet cross-sections in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV with the ATLAS detector,2852,0.0003506311360448808,,,nan,,NOT SCOAP3 Switzerland
914505,21399,,,2542,"Tskhadadze, E.",Springer/SISSA,Measurement of the inclusive jet cross-sections in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV with the ATLAS detector,2852,0.0003506311360448808,,,nan,,NOT SCOAP3 Switzerland
914506,21399,,,2749,"Wu, X.",Springer/SISSA,Measurement of the inclusive jet cross-sections in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV with the ATLAS detector,2852,0.0003506311360448808,,,nan,,NOT SCOAP3 Switzerland
932200,21243,,,695,"Battilana, C.",Springer/SISSA,Search for top quark partners with charge 5/3 in proton-proton collisions at s = 13 $$ \sqrt{s}=13 $$ TeV,2192,0.0004562043795620438,,,nan,,NOT SCOAP3 Switzerland
932201,21243,,,751,"Ciriolo, V.",Springer/SISSA,Search for top quark partners with charge 5/3 in proton-proton collisions at s = 13 $$ \sqrt{s}=13 $$ TeV,2192,0.0004562043795620438,,,nan,,NOT SCOAP3 Switzerland
932202,21243,,,763,"Pauwels, K.",Springer/SISSA,Search for top quark partners with charge 5/3 in proton-proton collisions at s = 13 $$ \sqrt{s}=13 $$ TeV,2192,0.0004562043795620438,,,nan,,NOT SCOAP3 Switzerland
932203,21243,,,812,"Ressegotti, M.",Springer/SISSA,Search for top quark partners with charge 5/3 in proton-proton collisions at s = 13 $$ \sqrt{s}=13 $$ TeV,2192,0.0004562043795620438,,,nan,,NOT SCOAP3 Switzerland
932204,21243,,,828,"Spiga, D.",Springer/SISSA,Search for top quark partners with charge 5/3 in proton-proton collisions at s = 13 $$ \sqrt{s}=13 $$ TeV,2192,0.0004562043795620438,,,nan,,NOT SCOAP3 Switzerland
932205,21243,,,834,"Borrello, L.",Springer/SISSA,Search for top quark partners with charge 5/3 in proton-proton collisions at s = 13 $$ \sqrt{s}=13 $$ TeV,2192,0.0004562043795620438,,,nan,,NOT SCOAP3 Switzerland
938743,21042,,,704,"Battilana, C.",Springer/SISSA,Measurement of the inclusive energy spectrum in the very forward direction in proton-proton collisions at s = 13 $$ \sqrt{s}=13 $$ TeV,2234,0.0004476275738585497,,,nan,,NOT SCOAP3 Switzerland
938744,21042,,,762,"Ciriolo, V.",Springer/SISSA,Measurement of the inclusive energy spectrum in the very forward direction in proton-proton collisions at s = 13 $$ \sqrt{s}=13 $$ TeV,2234,0.0004476275738585497,,,nan,,NOT SCOAP3 Switzerland
938745,21042,,,780,"Nardo, G.",Springer/SISSA,Measurement of the inclusive energy spectrum in the very forward direction in proton-proton collisions at s = 13 $$ \sqrt{s}=13 $$ TeV,2234,0.0004476275738585497,,,nan,,NOT SCOAP3 Switzerland
938746,21042,,,848,"Fedi, G.",Springer/SISSA,Measurement of the inclusive energy spectrum in the very forward direction in proton-proton collisions at s = 13 $$ \sqrt{s}=13 $$ TeV,2234,0.0004476275738585497,,,nan,,NOT SCOAP3 Switzerland
945189,21141,,,159,"Ruiz Vargas, J.",Springer/SISSA,Erratum to: search for dark matter in proton-proton collisions at 8 TeV with missing transverse momentum and vector boson tagged jets,2267,0.0004411116012351125,,,nan,,NOT SCOAP3 Switzerland
945190,21141,,,719,"Battilana, C.",Springer/SISSA,Erratum to: search for dark matter in proton-proton collisions at 8 TeV with missing transverse momentum and vector boson tagged jets,2267,0.0004411116012351125,,,nan,,NOT SCOAP3 Switzerland
945191,21141,,,789,"Pigazzini, S.",Springer/SISSA,Erratum to: search for dark matter in proton-proton collisions at 8 TeV with missing transverse momentum and vector boson tagged jets,2267,0.0004411116012351125,,,nan,,NOT SCOAP3 Switzerland
945192,21141,,,794,"Nardo, G.",Springer/SISSA,Erratum to: search for dark matter in proton-proton collisions at 8 TeV with missing transverse momentum and vector boson tagged jets,2267,0.0004411116012351125,,,nan,,NOT SCOAP3 Switzerland
945193,21141,,,804,"Thyssen, F.",Springer/SISSA,Erratum to: search for dark matter in proton-proton collisions at 8 TeV with missing transverse momentum and vector boson tagged jets,2267,0.0004411116012351125,,,nan,,NOT SCOAP3 Switzerland
945194,21141,,,828,"Zanetti, M.",Springer/SISSA,Erratum to: search for dark matter in proton-proton collisions at 8 TeV with missing transverse momentum and vector boson tagged jets,2267,0.0004411116012351125,,,nan,,NOT SCOAP3 Switzerland
945195,21141,,,860,"Fedi, G.",Springer/SISSA,Erratum to: search for dark matter in proton-proton collisions at 8 TeV with missing transverse momentum and vector boson tagged jets,2267,0.0004411116012351125,,,nan,,NOT SCOAP3 Switzerland
947653,21013,,,700,"Battilana, C.",Springer/SISSA,Searches for W′ bosons decaying to a top quark and a bottom quark in proton-proton collisions at 13 TeV,2205,0.00045351473922902497,,,nan,,NOT SCOAP3 Switzerland
947654,21013,,,816,"Ressegotti, M.",Springer/SISSA,Searches for W′ bosons decaying to a top quark and a bottom quark in proton-proton collisions at 13 TeV,2205,0.00045351473922902497,,,nan,,NOT SCOAP3 Switzerland
947655,21013,,,832,"Spiga, D.",Springer/SISSA,Searches for W′ bosons decaying to a top quark and a bottom quark in proton-proton collisions at 13 TeV,2205,0.00045351473922902497,,,nan,,NOT SCOAP3 Switzerland
947656,21013,,,838,"Borrello, L.",Springer/SISSA,Searches for W′ bosons decaying to a top quark and a bottom quark in proton-proton collisions at 13 TeV,2205,0.00045351473922902497,,,nan,,NOT SCOAP3 Switzerland
958864,20940,,,702,"Battilana, C.",Springer/SISSA,Search for third-generation scalar leptoquarks and heavy right-handed neutrinos in final states with two tau leptons and two jets in proton-proton collisions at s = 13 $$ \sqrt{s}=13 $$ TeV,2232,0.00044802867383512545,,,nan,,NOT SCOAP3 Switzerland
958865,20940,,,760,"Ciriolo, V.",Springer/SISSA,Search for third-generation scalar leptoquarks and heavy right-handed neutrinos in final states with two tau leptons and two jets in proton-proton collisions at s = 13 $$ \sqrt{s}=13 $$ TeV,2232,0.00044802867383512545,,,nan,,NOT SCOAP3 Switzerland
958866,20940,,,778,"Nardo, G.",Springer/SISSA,Search for third-generation scalar leptoquarks and heavy right-handed neutrinos in final states with two tau leptons and two jets in proton-proton collisions at s = 13 $$ \sqrt{s}=13 $$ TeV,2232,0.00044802867383512545,,,nan,,NOT SCOAP3 Switzerland
958867,20940,,,846,"Fedi, G.",Springer/SISSA,Search for third-generation scalar leptoquarks and heavy right-handed neutrinos in final states with two tau leptons and two jets in proton-proton collisions at s = 13 $$ \sqrt{s}=13 $$ TeV,2232,0.00044802867383512545,,,nan,,NOT SCOAP3 Switzerland
983137,20749,,,704,"Battilana, C.",Springer/SISSA,Search for new physics with dijet angular distributions in proton-proton collisions at s = 13 $$ \sqrt{s}=13 $$ TeV,2235,0.00044742729306487697,,,nan,,NOT SCOAP3 Switzerland
983138,20749,,,762,"Ciriolo, V.",Springer/SISSA,Search for new physics with dijet angular distributions in proton-proton collisions at s = 13 $$ \sqrt{s}=13 $$ TeV,2235,0.00044742729306487697,,,nan,,NOT SCOAP3 Switzerland
983139,20749,,,780,"Nardo, G.",Springer/SISSA,Search for new physics with dijet angular distributions in proton-proton collisions at s = 13 $$ \sqrt{s}=13 $$ TeV,2235,0.00044742729306487697,,,nan,,NOT SCOAP3 Switzerland
983140,20749,,,847,"Fedi, G.",Springer/SISSA,Search for new physics with dijet angular distributions in proton-proton collisions at s = 13 $$ \sqrt{s}=13 $$ TeV,2235,0.00044742729306487697,,,nan,,NOT SCOAP3 Switzerland
986501,20774,,,702,"Battilana, C.",Springer/SISSA,Search for dark matter produced with an energetic jet or a hadronically decaying W or Z boson at s = 13 $$ \sqrt{s}=13 $$ TeV,2231,0.00044822949350067237,,,nan,,NOT SCOAP3 Switzerland
986502,20774,,,760,"Ciriolo, V.",Springer/SISSA,Search for dark matter produced with an energetic jet or a hadronically decaying W or Z boson at s = 13 $$ \sqrt{s}=13 $$ TeV,2231,0.00044822949350067237,,,nan,,NOT SCOAP3 Switzerland
986503,20774,,,778,"Nardo, G.",Springer/SISSA,Search for dark matter produced with an energetic jet or a hadronically decaying W or Z boson at s = 13 $$ \sqrt{s}=13 $$ TeV,2231,0.00044822949350067237,,,nan,,NOT SCOAP3 Switzerland
986504,20774,,,846,"Fedi, G.",Springer/SISSA,Search for dark matter produced with an energetic jet or a hadronically decaying W or Z boson at s = 13 $$ \sqrt{s}=13 $$ TeV,2231,0.00044822949350067237,,,nan,,NOT SCOAP3 Switzerland
988952,20724,,,695,"Battilana, C.",Springer/SISSA,Search for t t ¯ $$ \mathrm{t}\overline{\mathrm{t}} $$ resonances in highly boosted lepton+jets and fully hadronic final states in proton-proton collisions at s = 13 $$ \sqrt{s}=13 $$ TeV,2197,0.0004551661356395084,,,nan,,NOT SCOAP3 Switzerland
988953,20724,,,749,"Ciriolo, V.",Springer/SISSA,Search for t t ¯ $$ \mathrm{t}\overline{\mathrm{t}} $$ resonances in highly boosted lepton+jets and fully hadronic final states in proton-proton collisions at s = 13 $$ \sqrt{s}=13 $$ TeV,2197,0.0004551661356395084,,,nan,,NOT SCOAP3 Switzerland
988954,20724,,,761,"Pauwels, K.",Springer/SISSA,Search for t t ¯ $$ \mathrm{t}\overline{\mathrm{t}} $$ resonances in highly boosted lepton+jets and fully hadronic final states in proton-proton collisions at s = 13 $$ \sqrt{s}=13 $$ TeV,2197,0.0004551661356395084,,,nan,,NOT SCOAP3 Switzerland
988955,20724,,,811,"Ressegotti, M.",Springer/SISSA,Search for t t ¯ $$ \mathrm{t}\overline{\mathrm{t}} $$ resonances in highly boosted lepton+jets and fully hadronic final states in proton-proton collisions at s = 13 $$ \sqrt{s}=13 $$ TeV,2197,0.0004551661356395084,,,nan,,NOT SCOAP3 Switzerland
988956,20724,,,827,"Spiga, D.",Springer/SISSA,Search for t t ¯ $$ \mathrm{t}\overline{\mathrm{t}} $$ resonances in highly boosted lepton+jets and fully hadronic final states in proton-proton collisions at s = 13 $$ \sqrt{s}=13 $$ TeV,2197,0.0004551661356395084,,,nan,,NOT SCOAP3 Switzerland
988957,20724,,,833,"Borrello, L.",Springer/SISSA,Search for t t ¯ $$ \mathrm{t}\overline{\mathrm{t}} $$ resonances in highly boosted lepton+jets and fully hadronic final states in proton-proton collisions at s = 13 $$ \sqrt{s}=13 $$ TeV,2197,0.0004551661356395084,,,nan,,NOT SCOAP3 Switzerland
991452,20725,,,706,"Battilana, C.",Springer/SISSA,Search for associated production of a Z boson with a single top quark and for tZ flavour-changing interactions in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2233,0.0004478280340349306,,,nan,,NOT SCOAP3 Switzerland
991453,20725,,,764,"Ciriolo, V.",Springer/SISSA,Search for associated production of a Z boson with a single top quark and for tZ flavour-changing interactions in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2233,0.0004478280340349306,,,nan,,NOT SCOAP3 Switzerland
991454,20725,,,782,"Nardo, G.",Springer/SISSA,Search for associated production of a Z boson with a single top quark and for tZ flavour-changing interactions in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2233,0.0004478280340349306,,,nan,,NOT SCOAP3 Switzerland
991455,20725,,,849,"Fedi, G.",Springer/SISSA,Search for associated production of a Z boson with a single top quark and for tZ flavour-changing interactions in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2233,0.0004478280340349306,,,nan,,NOT SCOAP3 Switzerland
1006697,20581,,,158,"Ruiz Vargas, J.",Springer/SISSA,Measurement of electroweak-induced production of Wγ with two jets in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV and constraints on anomalous quartic gauge couplings,2266,0.000441306266548985,,,nan,,NOT SCOAP3 Switzerland
1006698,20581,,,719,"Battilana, C.",Springer/SISSA,Measurement of electroweak-induced production of Wγ with two jets in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV and constraints on anomalous quartic gauge couplings,2266,0.000441306266548985,,,nan,,NOT SCOAP3 Switzerland
1006699,20581,,,782,"Malberti, M.",Springer/SISSA,Measurement of electroweak-induced production of Wγ with two jets in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV and constraints on anomalous quartic gauge couplings,2266,0.000441306266548985,,,nan,,NOT SCOAP3 Switzerland
1006700,20581,,,790,"Pigazzini, S.",Springer/SISSA,Measurement of electroweak-induced production of Wγ with two jets in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV and constraints on anomalous quartic gauge couplings,2266,0.000441306266548985,,,nan,,NOT SCOAP3 Switzerland
1006701,20581,,,795,"Nardo, G.",Springer/SISSA,Measurement of electroweak-induced production of Wγ with two jets in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV and constraints on anomalous quartic gauge couplings,2266,0.000441306266548985,,,nan,,NOT SCOAP3 Switzerland
1006702,20581,,,805,"Thyssen, F.",Springer/SISSA,Measurement of electroweak-induced production of Wγ with two jets in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV and constraints on anomalous quartic gauge couplings,2266,0.000441306266548985,,,nan,,NOT SCOAP3 Switzerland
1006703,20581,,,829,"Zanetti, M.",Springer/SISSA,Measurement of electroweak-induced production of Wγ with two jets in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV and constraints on anomalous quartic gauge couplings,2266,0.000441306266548985,,,nan,,NOT SCOAP3 Switzerland
1006704,20581,,,861,"Fedi, G.",Springer/SISSA,Measurement of electroweak-induced production of Wγ with two jets in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV and constraints on anomalous quartic gauge couplings,2266,0.000441306266548985,,,nan,,NOT SCOAP3 Switzerland
1049051,20114,,,703,"Battilana, C.",Springer/SISSA,Search for single production of vector-like quarks decaying to a Z boson and a top or a bottom quark in proton-proton collisions at s = 13 $$ \sqrt{s}=13 $$ TeV,2231,0.00044822949350067237,,,nan,,NOT SCOAP3 Switzerland
1049052,20114,,,779,"Nardo, G.",Springer/SISSA,Search for single production of vector-like quarks decaying to a Z boson and a top or a bottom quark in proton-proton collisions at s = 13 $$ \sqrt{s}=13 $$ TeV,2231,0.00044822949350067237,,,nan,,NOT SCOAP3 Switzerland
1049053,20114,,,846,"Fedi, G.",Springer/SISSA,Search for single production of vector-like quarks decaying to a Z boson and a top or a bottom quark in proton-proton collisions at s = 13 $$ \sqrt{s}=13 $$ TeV,2231,0.00044822949350067237,,,nan,,NOT SCOAP3 Switzerland
1052523,19992,,,160,"Ruiz Vargas, J.",Springer/SISSA,Observation of Y(1S) pair production in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2279,0.00043878894251864854,,,nan,,NOT SCOAP3 Switzerland
1052524,19992,,,723,"Battilana, C.",Springer/SISSA,Observation of Y(1S) pair production in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2279,0.00043878894251864854,,,nan,,NOT SCOAP3 Switzerland
1052525,19992,,,798,"Nardo, G.",Springer/SISSA,Observation of Y(1S) pair production in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2279,0.00043878894251864854,,,nan,,NOT SCOAP3 Switzerland
1052526,19992,,,809,"Thyssen, F.",Springer/SISSA,Observation of Y(1S) pair production in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2279,0.00043878894251864854,,,nan,,NOT SCOAP3 Switzerland
1052527,19992,,,834,"Zanetti, M.",Springer/SISSA,Observation of Y(1S) pair production in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2279,0.00043878894251864854,,,nan,,NOT SCOAP3 Switzerland
1052528,19992,,,864,"Fedi, G.",Springer/SISSA,Observation of Y(1S) pair production in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2279,0.00043878894251864854,,,nan,,NOT SCOAP3 Switzerland
1070061,19845,,,714,"Battilana, C.",Springer/SISSA,Search for electroweak production of a vector-like quark decaying to a top quark and a Higgs boson using boosted topologies in fully hadronic final states,2246,0.0004452359750667854,,,nan,,NOT SCOAP3 Switzerland
1070062,19845,,,770,"Ciriolo, V.",Springer/SISSA,Search for electroweak production of a vector-like quark decaying to a top quark and a Higgs boson using boosted topologies in fully hadronic final states,2246,0.0004452359750667854,,,nan,,NOT SCOAP3 Switzerland
1070063,19845,,,788,"Nardo, G.",Springer/SISSA,Search for electroweak production of a vector-like quark decaying to a top quark and a Higgs boson using boosted topologies in fully hadronic final states,2246,0.0004452359750667854,,,nan,,NOT SCOAP3 Switzerland
1070064,19845,,,854,"Fedi, G.",Springer/SISSA,Search for electroweak production of a vector-like quark decaying to a top quark and a Higgs boson using boosted topologies in fully hadronic final states,2246,0.0004452359750667854,,,nan,,NOT SCOAP3 Switzerland
1095868,19673,,,161,"Vargas, J.",Springer/SISSA,Charged-particle nuclear modification factors in PbPb and pPb collisions at s N N = 5.02 $$ \sqrt{s_{\mathrm{N}\;\mathrm{N}}}=5.02 $$ TeV,2272,0.00044014084507042255,,,nan,,NOT SCOAP3 Switzerland
1095869,19673,,,717,"Battilana, C.",Springer/SISSA,Charged-particle nuclear modification factors in PbPb and pPb collisions at s N N = 5.02 $$ \sqrt{s_{\mathrm{N}\;\mathrm{N}}}=5.02 $$ TeV,2272,0.00044014084507042255,,,nan,,NOT SCOAP3 Switzerland
1095870,19673,,,791,"Nardo, G.",Springer/SISSA,Charged-particle nuclear modification factors in PbPb and pPb collisions at s N N = 5.02 $$ \sqrt{s_{\mathrm{N}\;\mathrm{N}}}=5.02 $$ TeV,2272,0.00044014084507042255,,,nan,,NOT SCOAP3 Switzerland
1095871,19673,,,826,"Zanetti, M.",Springer/SISSA,Charged-particle nuclear modification factors in PbPb and pPb collisions at s N N = 5.02 $$ \sqrt{s_{\mathrm{N}\;\mathrm{N}}}=5.02 $$ TeV,2272,0.00044014084507042255,,,nan,,NOT SCOAP3 Switzerland
1095872,19673,,,857,"Fedi, G.",Springer/SISSA,Charged-particle nuclear modification factors in PbPb and pPb collisions at s N N = 5.02 $$ \sqrt{s_{\mathrm{N}\;\mathrm{N}}}=5.02 $$ TeV,2272,0.00044014084507042255,,,nan,,NOT SCOAP3 Switzerland
1101678,19634,,,159,"Vargas, J.",Springer/SISSA,Measurements of differential production cross sections for a Z boson in association with jets in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2264,0.00044169611307420494,,,nan,,NOT SCOAP3 Switzerland
1101679,19634,,,715,"Battilana, C.",Springer/SISSA,Measurements of differential production cross sections for a Z boson in association with jets in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2264,0.00044169611307420494,,,nan,,NOT SCOAP3 Switzerland
1101680,19634,,,778,"Malberti, M.",Springer/SISSA,Measurements of differential production cross sections for a Z boson in association with jets in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2264,0.00044169611307420494,,,nan,,NOT SCOAP3 Switzerland
1101681,19634,,,786,"Pigazzini, S.",Springer/SISSA,Measurements of differential production cross sections for a Z boson in association with jets in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2264,0.00044169611307420494,,,nan,,NOT SCOAP3 Switzerland
1101682,19634,,,791,"Nardo, G.",Springer/SISSA,Measurements of differential production cross sections for a Z boson in association with jets in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2264,0.00044169611307420494,,,nan,,NOT SCOAP3 Switzerland
1101683,19634,,,801,"Thyssen, F.",Springer/SISSA,Measurements of differential production cross sections for a Z boson in association with jets in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2264,0.00044169611307420494,,,nan,,NOT SCOAP3 Switzerland
1101684,19634,,,825,"Zanetti, M.",Springer/SISSA,Measurements of differential production cross sections for a Z boson in association with jets in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2264,0.00044169611307420494,,,nan,,NOT SCOAP3 Switzerland
1101685,19634,,,857,"Fedi, G.",Springer/SISSA,Measurements of differential production cross sections for a Z boson in association with jets in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2264,0.00044169611307420494,,,nan,,NOT SCOAP3 Switzerland
1104204,19648,,,159,"Ruiz Vargas, J.",Springer/SISSA,Search for electroweak production of charginos in final states with two τ leptons in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2261,0.0004422821760283061,,,nan,,NOT SCOAP3 Switzerland
1104205,19648,,,713,"Battilana, C.",Springer/SISSA,Search for electroweak production of charginos in final states with two τ leptons in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2261,0.0004422821760283061,,,nan,,NOT SCOAP3 Switzerland
1104206,19648,,,776,"Malberti, M.",Springer/SISSA,Search for electroweak production of charginos in final states with two τ leptons in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2261,0.0004422821760283061,,,nan,,NOT SCOAP3 Switzerland
1104207,19648,,,784,"Pigazzini, S.",Springer/SISSA,Search for electroweak production of charginos in final states with two τ leptons in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2261,0.0004422821760283061,,,nan,,NOT SCOAP3 Switzerland
1104208,19648,,,789,"Nardo, G.",Springer/SISSA,Search for electroweak production of charginos in final states with two τ leptons in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2261,0.0004422821760283061,,,nan,,NOT SCOAP3 Switzerland
1104209,19648,,,799,"Thyssen, F.",Springer/SISSA,Search for electroweak production of charginos in final states with two τ leptons in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2261,0.0004422821760283061,,,nan,,NOT SCOAP3 Switzerland
1104210,19648,,,823,"Zanetti, M.",Springer/SISSA,Search for electroweak production of charginos in final states with two τ leptons in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2261,0.0004422821760283061,,,nan,,NOT SCOAP3 Switzerland
1104211,19648,,,855,"Fedi, G.",Springer/SISSA,Search for electroweak production of charginos in final states with two τ leptons in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2261,0.0004422821760283061,,,nan,,NOT SCOAP3 Switzerland
1107649,19573,,,715,"Battilana, C.",Springer/SISSA,"Search for massive resonances decaying into WW, WZ or ZZ bosons in proton-proton collisions at s = 13 $$ \sqrt{s}=13 $$ TeV",2239,0.00044662795891022776,,,nan,,NOT SCOAP3 Switzerland
1107650,19573,,,791,"Nardo, G.",Springer/SISSA,"Search for massive resonances decaying into WW, WZ or ZZ bosons in proton-proton collisions at s = 13 $$ \sqrt{s}=13 $$ TeV",2239,0.00044662795891022776,,,nan,,NOT SCOAP3 Switzerland
1107651,19573,,,857,"Fedi, G.",Springer/SISSA,"Search for massive resonances decaying into WW, WZ or ZZ bosons in proton-proton collisions at s = 13 $$ \sqrt{s}=13 $$ TeV",2239,0.00044662795891022776,,,nan,,NOT SCOAP3 Switzerland
1113272,19582,,,159,"Ruiz Vargas, J.",Springer/SISSA,Measurement and QCD analysis of double-differential inclusive jet cross sections in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV and cross section ratios to 2.76 and 7 TeV,2257,0.00044306601683650863,,,nan,,NOT SCOAP3 Switzerland
1113273,19582,,,721,"Battilana, C.",Springer/SISSA,Measurement and QCD analysis of double-differential inclusive jet cross sections in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV and cross section ratios to 2.76 and 7 TeV,2257,0.00044306601683650863,,,nan,,NOT SCOAP3 Switzerland
1113274,19582,,,778,"Brianza, L.",Springer/SISSA,Measurement and QCD analysis of double-differential inclusive jet cross sections in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV and cross section ratios to 2.76 and 7 TeV,2257,0.00044306601683650863,,,nan,,NOT SCOAP3 Switzerland
1113275,19582,,,791,"Pigazzini, S.",Springer/SISSA,Measurement and QCD analysis of double-differential inclusive jet cross sections in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV and cross section ratios to 2.76 and 7 TeV,2257,0.00044306601683650863,,,nan,,NOT SCOAP3 Switzerland
1113276,19582,,,796,"Nardo, G.",Springer/SISSA,Measurement and QCD analysis of double-differential inclusive jet cross sections in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV and cross section ratios to 2.76 and 7 TeV,2257,0.00044306601683650863,,,nan,,NOT SCOAP3 Switzerland
1113277,19582,,,807,"Thyssen, F.",Springer/SISSA,Measurement and QCD analysis of double-differential inclusive jet cross sections in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV and cross section ratios to 2.76 and 7 TeV,2257,0.00044306601683650863,,,nan,,NOT SCOAP3 Switzerland
1113278,19582,,,831,"Zanetti, M.",Springer/SISSA,Measurement and QCD analysis of double-differential inclusive jet cross sections in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV and cross section ratios to 2.76 and 7 TeV,2257,0.00044306601683650863,,,nan,,NOT SCOAP3 Switzerland
1113279,19582,,,863,"Fedi, G.",Springer/SISSA,Measurement and QCD analysis of double-differential inclusive jet cross sections in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV and cross section ratios to 2.76 and 7 TeV,2257,0.00044306601683650863,,,nan,,NOT SCOAP3 Switzerland
1125086,19441,,,162,"Ruiz Vargas, J.",Springer/SISSA,Search for CP violation in t t ¯ $$ t\overline{t} $$ production and decay in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2274,0.00043975373790677223,,,nan,,NOT SCOAP3 Switzerland
1125087,19441,,,718,"Battilana, C.",Springer/SISSA,Search for CP violation in t t ¯ $$ t\overline{t} $$ production and decay in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2274,0.00043975373790677223,,,nan,,NOT SCOAP3 Switzerland
1125088,19441,,,792,"Nardo, G.",Springer/SISSA,Search for CP violation in t t ¯ $$ t\overline{t} $$ production and decay in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2274,0.00043975373790677223,,,nan,,NOT SCOAP3 Switzerland
1125089,19441,,,803,"Thyssen, F.",Springer/SISSA,Search for CP violation in t t ¯ $$ t\overline{t} $$ production and decay in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2274,0.00043975373790677223,,,nan,,NOT SCOAP3 Switzerland
1125090,19441,,,827,"Zanetti, M.",Springer/SISSA,Search for CP violation in t t ¯ $$ t\overline{t} $$ production and decay in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2274,0.00043975373790677223,,,nan,,NOT SCOAP3 Switzerland
1125091,19441,,,858,"Fedi, G.",Springer/SISSA,Search for CP violation in t t ¯ $$ t\overline{t} $$ production and decay in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2274,0.00043975373790677223,,,nan,,NOT SCOAP3 Switzerland
1128411,19368,,,162,"Ruiz Vargas, J.",Springer/SISSA,Search for heavy neutrinos or third-generation leptoquarks in final states with two hadronically decaying τ leptons and two jets in proton-proton collisions at s = 13 $$ \sqrt{s}=13 $$ TeV,2279,0.00043878894251864854,,,nan,,NOT SCOAP3 Switzerland
1128412,19368,,,722,"Battilana, C.",Springer/SISSA,Search for heavy neutrinos or third-generation leptoquarks in final states with two hadronically decaying τ leptons and two jets in proton-proton collisions at s = 13 $$ \sqrt{s}=13 $$ TeV,2279,0.00043878894251864854,,,nan,,NOT SCOAP3 Switzerland
1128413,19368,,,783,"Malberti, M.",Springer/SISSA,Search for heavy neutrinos or third-generation leptoquarks in final states with two hadronically decaying τ leptons and two jets in proton-proton collisions at s = 13 $$ \sqrt{s}=13 $$ TeV,2279,0.00043878894251864854,,,nan,,NOT SCOAP3 Switzerland
1128414,19368,,,790,"Pigazzini, S.",Springer/SISSA,Search for heavy neutrinos or third-generation leptoquarks in final states with two hadronically decaying τ leptons and two jets in proton-proton collisions at s = 13 $$ \sqrt{s}=13 $$ TeV,2279,0.00043878894251864854,,,nan,,NOT SCOAP3 Switzerland
1128415,19368,,,795,"Nardo, G.",Springer/SISSA,Search for heavy neutrinos or third-generation leptoquarks in final states with two hadronically decaying τ leptons and two jets in proton-proton collisions at s = 13 $$ \sqrt{s}=13 $$ TeV,2279,0.00043878894251864854,,,nan,,NOT SCOAP3 Switzerland
1128416,19368,,,806,"Thyssen, F.",Springer/SISSA,Search for heavy neutrinos or third-generation leptoquarks in final states with two hadronically decaying τ leptons and two jets in proton-proton collisions at s = 13 $$ \sqrt{s}=13 $$ TeV,2279,0.00043878894251864854,,,nan,,NOT SCOAP3 Switzerland
1128417,19368,,,830,"Zanetti, M.",Springer/SISSA,Search for heavy neutrinos or third-generation leptoquarks in final states with two hadronically decaying τ leptons and two jets in proton-proton collisions at s = 13 $$ \sqrt{s}=13 $$ TeV,2279,0.00043878894251864854,,,nan,,NOT SCOAP3 Switzerland
1128418,19368,,,861,"Fedi, G.",Springer/SISSA,Search for heavy neutrinos or third-generation leptoquarks in final states with two hadronically decaying τ leptons and two jets in proton-proton collisions at s = 13 $$ \sqrt{s}=13 $$ TeV,2279,0.00043878894251864854,,,nan,,NOT SCOAP3 Switzerland
1133972,19316,,,714,"Battilana, C.",Springer,Search for dark matter and unparticles in events with a Z boson and missing transverse momentum in proton-proton collisions at      <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>13</mn> </math>  $$ \sqrt{s}=13 $$  TeV,2244,0.000445632798573975,,,nan,,NOT SCOAP3 Switzerland
1133973,19316,,,770,"Ciriolo, V.",Springer,Search for dark matter and unparticles in events with a Z boson and missing transverse momentum in proton-proton collisions at      <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>13</mn> </math>  $$ \sqrt{s}=13 $$  TeV,2244,0.000445632798573975,,,nan,,NOT SCOAP3 Switzerland
1133974,19316,,,788,"Nardo, G.",Springer,Search for dark matter and unparticles in events with a Z boson and missing transverse momentum in proton-proton collisions at      <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>13</mn> </math>  $$ \sqrt{s}=13 $$  TeV,2244,0.000445632798573975,,,nan,,NOT SCOAP3 Switzerland
1133975,19316,,,855,"Fedi, G.",Springer,Search for dark matter and unparticles in events with a Z boson and missing transverse momentum in proton-proton collisions at      <math> <msqrt> <mi>s</mi> </msqrt> <mo>=</mo> <mn>13</mn> </math>  $$ \sqrt{s}=13 $$  TeV,2244,0.000445632798573975,,,nan,,NOT SCOAP3 Switzerland
1136808,19291,,,160,"Ruiz Vargas, J.",Springer/SISSA,Measurement of the transverse momentum spectrum of the Higgs boson produced in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV using H → WW decays,2259,0.0004426737494466578,,,nan,,NOT SCOAP3 Switzerland
1136809,19291,,,717,"Battilana, C.",Springer/SISSA,Measurement of the transverse momentum spectrum of the Higgs boson produced in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV using H → WW decays,2259,0.0004426737494466578,,,nan,,NOT SCOAP3 Switzerland
1136810,19291,,,761,"Redapi, L.",Springer/SISSA,Measurement of the transverse momentum spectrum of the Higgs boson produced in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV using H → WW decays,2259,0.0004426737494466578,,,nan,,NOT SCOAP3 Switzerland
1136811,19291,,,776,"Brianza, L.",Springer/SISSA,Measurement of the transverse momentum spectrum of the Higgs boson produced in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV using H → WW decays,2259,0.0004426737494466578,,,nan,,NOT SCOAP3 Switzerland
1136812,19291,,,789,"Pigazzini, S.",Springer/SISSA,Measurement of the transverse momentum spectrum of the Higgs boson produced in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV using H → WW decays,2259,0.0004426737494466578,,,nan,,NOT SCOAP3 Switzerland
1136813,19291,,,794,"Nardo, G.",Springer/SISSA,Measurement of the transverse momentum spectrum of the Higgs boson produced in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV using H → WW decays,2259,0.0004426737494466578,,,nan,,NOT SCOAP3 Switzerland
1136814,19291,,,804,"Thyssen, F.",Springer/SISSA,Measurement of the transverse momentum spectrum of the Higgs boson produced in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV using H → WW decays,2259,0.0004426737494466578,,,nan,,NOT SCOAP3 Switzerland
1136815,19291,,,828,"Zanetti, M.",Springer/SISSA,Measurement of the transverse momentum spectrum of the Higgs boson produced in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV using H → WW decays,2259,0.0004426737494466578,,,nan,,NOT SCOAP3 Switzerland
1136816,19291,,,860,"Fedi, G.",Springer/SISSA,Measurement of the transverse momentum spectrum of the Higgs boson produced in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV using H → WW decays,2259,0.0004426737494466578,,,nan,,NOT SCOAP3 Switzerland
1147192,19191,,,160,"Ruiz Vargas, J.",Springer/SISSA,"Searches for invisible decays of the Higgs boson in pp collisions at s $$ \sqrt{s} $$ = 7 , 8, and 13 TeV",2273,0.0004399472063352398,,,nan,,NOT SCOAP3 Switzerland
1147193,19191,,,721,"Battilana, C.",Springer/SISSA,"Searches for invisible decays of the Higgs boson in pp collisions at s $$ \sqrt{s} $$ = 7 , 8, and 13 TeV",2273,0.0004399472063352398,,,nan,,NOT SCOAP3 Switzerland
1147194,19191,,,784,"Malberti, M.",Springer/SISSA,"Searches for invisible decays of the Higgs boson in pp collisions at s $$ \sqrt{s} $$ = 7 , 8, and 13 TeV",2273,0.0004399472063352398,,,nan,,NOT SCOAP3 Switzerland
1147195,19191,,,791,"Pigazzini, S.",Springer/SISSA,"Searches for invisible decays of the Higgs boson in pp collisions at s $$ \sqrt{s} $$ = 7 , 8, and 13 TeV",2273,0.0004399472063352398,,,nan,,NOT SCOAP3 Switzerland
1147196,19191,,,796,"Nardo, G.",Springer/SISSA,"Searches for invisible decays of the Higgs boson in pp collisions at s $$ \sqrt{s} $$ = 7 , 8, and 13 TeV",2273,0.0004399472063352398,,,nan,,NOT SCOAP3 Switzerland
1147197,19191,,,807,"Thyssen, F.",Springer/SISSA,"Searches for invisible decays of the Higgs boson in pp collisions at s $$ \sqrt{s} $$ = 7 , 8, and 13 TeV",2273,0.0004399472063352398,,,nan,,NOT SCOAP3 Switzerland
1147198,19191,,,831,"Zanetti, M.",Springer/SISSA,"Searches for invisible decays of the Higgs boson in pp collisions at s $$ \sqrt{s} $$ = 7 , 8, and 13 TeV",2273,0.0004399472063352398,,,nan,,NOT SCOAP3 Switzerland
1147199,19191,,,862,"Fedi, G.",Springer/SISSA,"Searches for invisible decays of the Higgs boson in pp collisions at s $$ \sqrt{s} $$ = 7 , 8, and 13 TeV",2273,0.0004399472063352398,,,nan,,NOT SCOAP3 Switzerland
1157755,19092,,,170,"Ruiz Vargas, J.",Springer/SISSA,Measurement of the transverse momentum spectra of weak vector bosons produced in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2300,0.0004347826086956522,,,nan,,NOT SCOAP3 Switzerland
1157756,19092,,,790,"Brianza, L.",Springer/SISSA,Measurement of the transverse momentum spectra of weak vector bosons produced in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2300,0.0004347826086956522,,,nan,,NOT SCOAP3 Switzerland
1157757,19092,,,804,"Pigazzini, S.",Springer/SISSA,Measurement of the transverse momentum spectra of weak vector bosons produced in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2300,0.0004347826086956522,,,nan,,NOT SCOAP3 Switzerland
1157758,19092,,,820,"Thyssen, F.",Springer/SISSA,Measurement of the transverse momentum spectra of weak vector bosons produced in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2300,0.0004347826086956522,,,nan,,NOT SCOAP3 Switzerland
1157759,19092,,,847,"Zanetti, M.",Springer/SISSA,Measurement of the transverse momentum spectra of weak vector bosons produced in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2300,0.0004347826086956522,,,nan,,NOT SCOAP3 Switzerland
1157760,19092,,,878,"Fedi, G.",Springer/SISSA,Measurement of the transverse momentum spectra of weak vector bosons produced in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2300,0.0004347826086956522,,,nan,,NOT SCOAP3 Switzerland
1160653,19061,,,162,"Ruiz Vargas, J.",Springer/SISSA,Search for top quark decays via Higgs-boson-mediated flavor-changing neutral currents in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2257,0.00044306601683650863,,,nan,,NOT SCOAP3 Switzerland
1160654,19061,,,717,"Battilana, C.",Springer/SISSA,Search for top quark decays via Higgs-boson-mediated flavor-changing neutral currents in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2257,0.00044306601683650863,,,nan,,NOT SCOAP3 Switzerland
1160655,19061,,,774,"Brianza, L.",Springer/SISSA,Search for top quark decays via Higgs-boson-mediated flavor-changing neutral currents in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2257,0.00044306601683650863,,,nan,,NOT SCOAP3 Switzerland
1160656,19061,,,787,"Pigazzini, S.",Springer/SISSA,Search for top quark decays via Higgs-boson-mediated flavor-changing neutral currents in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2257,0.00044306601683650863,,,nan,,NOT SCOAP3 Switzerland
1160657,19061,,,792,"Nardo, G.",Springer/SISSA,Search for top quark decays via Higgs-boson-mediated flavor-changing neutral currents in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2257,0.00044306601683650863,,,nan,,NOT SCOAP3 Switzerland
1160658,19061,,,803,"Thyssen, F.",Springer/SISSA,Search for top quark decays via Higgs-boson-mediated flavor-changing neutral currents in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2257,0.00044306601683650863,,,nan,,NOT SCOAP3 Switzerland
1160659,19061,,,827,"Zanetti, M.",Springer/SISSA,Search for top quark decays via Higgs-boson-mediated flavor-changing neutral currents in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2257,0.00044306601683650863,,,nan,,NOT SCOAP3 Switzerland
1160660,19061,,,859,"Fedi, G.",Springer/SISSA,Search for top quark decays via Higgs-boson-mediated flavor-changing neutral currents in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2257,0.00044306601683650863,,,nan,,NOT SCOAP3 Switzerland
1172708,18946,,,160,"Ruiz Vargas, J.",Springer/SISSA,Search for heavy resonances decaying to tau lepton pairs in proton-proton collisions at s = 13 $$ \sqrt{s}=13 $$ TeV,2282,0.00043821209465381246,,,nan,,NOT SCOAP3 Switzerland
1172709,18946,,,723,"Battilana, C.",Springer/SISSA,Search for heavy resonances decaying to tau lepton pairs in proton-proton collisions at s = 13 $$ \sqrt{s}=13 $$ TeV,2282,0.00043821209465381246,,,nan,,NOT SCOAP3 Switzerland
1172710,18946,,,786,"Malberti, M.",Springer/SISSA,Search for heavy resonances decaying to tau lepton pairs in proton-proton collisions at s = 13 $$ \sqrt{s}=13 $$ TeV,2282,0.00043821209465381246,,,nan,,NOT SCOAP3 Switzerland
1172711,18946,,,793,"Pigazzini, S.",Springer/SISSA,Search for heavy resonances decaying to tau lepton pairs in proton-proton collisions at s = 13 $$ \sqrt{s}=13 $$ TeV,2282,0.00043821209465381246,,,nan,,NOT SCOAP3 Switzerland
1172712,18946,,,798,"Nardo, G.",Springer/SISSA,Search for heavy resonances decaying to tau lepton pairs in proton-proton collisions at s = 13 $$ \sqrt{s}=13 $$ TeV,2282,0.00043821209465381246,,,nan,,NOT SCOAP3 Switzerland
1172713,18946,,,809,"Thyssen, F.",Springer/SISSA,Search for heavy resonances decaying to tau lepton pairs in proton-proton collisions at s = 13 $$ \sqrt{s}=13 $$ TeV,2282,0.00043821209465381246,,,nan,,NOT SCOAP3 Switzerland
1172714,18946,,,833,"Zanetti, M.",Springer/SISSA,Search for heavy resonances decaying to tau lepton pairs in proton-proton collisions at s = 13 $$ \sqrt{s}=13 $$ TeV,2282,0.00043821209465381246,,,nan,,NOT SCOAP3 Switzerland
1172715,18946,,,864,"Fedi, G.",Springer/SISSA,Search for heavy resonances decaying to tau lepton pairs in proton-proton collisions at s = 13 $$ \sqrt{s}=13 $$ TeV,2282,0.00043821209465381246,,,nan,,NOT SCOAP3 Switzerland
1181767,18939,,,160,"Ruiz Vargas, J.",Springer/SISSA,Search for anomalous Wtb couplings and flavour-changing neutral currents in t -channel single top quark production in pp collisions at s = 7 $$ \sqrt{s}=7 $$ and 8 TeV,2259,0.0004426737494466578,,,nan,,NOT SCOAP3 Switzerland
1181768,18939,,,718,"Battilana, C.",Springer/SISSA,Search for anomalous Wtb couplings and flavour-changing neutral currents in t -channel single top quark production in pp collisions at s = 7 $$ \sqrt{s}=7 $$ and 8 TeV,2259,0.0004426737494466578,,,nan,,NOT SCOAP3 Switzerland
1181769,18939,,,775,"Brianza, L.",Springer/SISSA,Search for anomalous Wtb couplings and flavour-changing neutral currents in t -channel single top quark production in pp collisions at s = 7 $$ \sqrt{s}=7 $$ and 8 TeV,2259,0.0004426737494466578,,,nan,,NOT SCOAP3 Switzerland
1181770,18939,,,788,"Pigazzini, S.",Springer/SISSA,Search for anomalous Wtb couplings and flavour-changing neutral currents in t -channel single top quark production in pp collisions at s = 7 $$ \sqrt{s}=7 $$ and 8 TeV,2259,0.0004426737494466578,,,nan,,NOT SCOAP3 Switzerland
1181771,18939,,,793,"Nardo, G.",Springer/SISSA,Search for anomalous Wtb couplings and flavour-changing neutral currents in t -channel single top quark production in pp collisions at s = 7 $$ \sqrt{s}=7 $$ and 8 TeV,2259,0.0004426737494466578,,,nan,,NOT SCOAP3 Switzerland
1181772,18939,,,803,"Thyssen, F.",Springer/SISSA,Search for anomalous Wtb couplings and flavour-changing neutral currents in t -channel single top quark production in pp collisions at s = 7 $$ \sqrt{s}=7 $$ and 8 TeV,2259,0.0004426737494466578,,,nan,,NOT SCOAP3 Switzerland
1181773,18939,,,827,"Zanetti, M.",Springer/SISSA,Search for anomalous Wtb couplings and flavour-changing neutral currents in t -channel single top quark production in pp collisions at s = 7 $$ \sqrt{s}=7 $$ and 8 TeV,2259,0.0004426737494466578,,,nan,,NOT SCOAP3 Switzerland
1181774,18939,,,859,"Fedi, G.",Springer/SISSA,Search for anomalous Wtb couplings and flavour-changing neutral currents in t -channel single top quark production in pp collisions at s = 7 $$ \sqrt{s}=7 $$ and 8 TeV,2259,0.0004426737494466578,,,nan,,NOT SCOAP3 Switzerland
1201748,18669,,,160,"Ruiz Vargas, J.",Springer/SISSA,Search for high-mass Zγ resonances in e + e − γ and μ + μ − γ final states in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ and 13 TeV,2271,0.00044033465433729633,,,nan,,NOT SCOAP3 Switzerland
1201749,18669,,,718,"Battilana, C.",Springer/SISSA,Search for high-mass Zγ resonances in e + e − γ and μ + μ − γ final states in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ and 13 TeV,2271,0.00044033465433729633,,,nan,,NOT SCOAP3 Switzerland
1201750,18669,,,781,"Malberti, M.",Springer/SISSA,Search for high-mass Zγ resonances in e + e − γ and μ + μ − γ final states in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ and 13 TeV,2271,0.00044033465433729633,,,nan,,NOT SCOAP3 Switzerland
1201751,18669,,,788,"Pigazzini, S.",Springer/SISSA,Search for high-mass Zγ resonances in e + e − γ and μ + μ − γ final states in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ and 13 TeV,2271,0.00044033465433729633,,,nan,,NOT SCOAP3 Switzerland
1201752,18669,,,793,"Nardo, G.",Springer/SISSA,Search for high-mass Zγ resonances in e + e − γ and μ + μ − γ final states in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ and 13 TeV,2271,0.00044033465433729633,,,nan,,NOT SCOAP3 Switzerland
1201753,18669,,,804,"Thyssen, F.",Springer/SISSA,Search for high-mass Zγ resonances in e + e − γ and μ + μ − γ final states in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ and 13 TeV,2271,0.00044033465433729633,,,nan,,NOT SCOAP3 Switzerland
1201754,18669,,,828,"Zanetti, M.",Springer/SISSA,Search for high-mass Zγ resonances in e + e − γ and μ + μ − γ final states in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ and 13 TeV,2271,0.00044033465433729633,,,nan,,NOT SCOAP3 Switzerland
1201755,18669,,,859,"Fedi, G.",Springer/SISSA,Search for high-mass Zγ resonances in e + e − γ and μ + μ − γ final states in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ and 13 TeV,2271,0.00044033465433729633,,,nan,,NOT SCOAP3 Switzerland
1212095,18422,,,158,"Ruiz Vargas, J.",Springer/SISSA,Measurement of the mass of the top quark in decays with a J/ ψ meson in pp collisions at 8 TeV,2261,0.0004422821760283061,,,nan,,NOT SCOAP3 Switzerland
1212096,18422,,,717,"Battilana, C.",Springer/SISSA,Measurement of the mass of the top quark in decays with a J/ ψ meson in pp collisions at 8 TeV,2261,0.0004422821760283061,,,nan,,NOT SCOAP3 Switzerland
1212097,18422,,,780,"Malberti, M.",Springer/SISSA,Measurement of the mass of the top quark in decays with a J/ ψ meson in pp collisions at 8 TeV,2261,0.0004422821760283061,,,nan,,NOT SCOAP3 Switzerland
1212098,18422,,,788,"Pigazzini, S.",Springer/SISSA,Measurement of the mass of the top quark in decays with a J/ ψ meson in pp collisions at 8 TeV,2261,0.0004422821760283061,,,nan,,NOT SCOAP3 Switzerland
1212099,18422,,,793,"Nardo, G.",Springer/SISSA,Measurement of the mass of the top quark in decays with a J/ ψ meson in pp collisions at 8 TeV,2261,0.0004422821760283061,,,nan,,NOT SCOAP3 Switzerland
1212100,18422,,,803,"Thyssen, F.",Springer/SISSA,Measurement of the mass of the top quark in decays with a J/ ψ meson in pp collisions at 8 TeV,2261,0.0004422821760283061,,,nan,,NOT SCOAP3 Switzerland
1212101,18422,,,827,"Zanetti, M.",Springer/SISSA,Measurement of the mass of the top quark in decays with a J/ ψ meson in pp collisions at 8 TeV,2261,0.0004422821760283061,,,nan,,NOT SCOAP3 Switzerland
1212102,18422,,,859,"Fedi, G.",Springer/SISSA,Measurement of the mass of the top quark in decays with a J/ ψ meson in pp collisions at 8 TeV,2261,0.0004422821760283061,,,nan,,NOT SCOAP3 Switzerland
1214653,18405,,,176,"Ruiz Vargas, J.",Springer/SISSA,Search for dark matter particles in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV using the razor variables,2287,0.00043725404459991256,,,nan,,NOT SCOAP3 Switzerland
1214654,18405,,,795,"Brianza, L.",Springer/SISSA,Search for dark matter particles in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV using the razor variables,2287,0.00043725404459991256,,,nan,,NOT SCOAP3 Switzerland
1214655,18405,,,824,"Thyssen, F.",Springer/SISSA,Search for dark matter particles in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV using the razor variables,2287,0.00043725404459991256,,,nan,,NOT SCOAP3 Switzerland
1214656,18405,,,850,"Zanetti, M.",Springer/SISSA,Search for dark matter particles in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV using the razor variables,2287,0.00043725404459991256,,,nan,,NOT SCOAP3 Switzerland
1214657,18405,,,881,"Fedi, G.",Springer/SISSA,Search for dark matter particles in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV using the razor variables,2287,0.00043725404459991256,,,nan,,NOT SCOAP3 Switzerland
1218050,18383,,,159,"Ruiz Vargas, J.",Springer/SISSA,Search for dark matter in proton-proton collisions at 8 TeV with missing transverse momentum and vector boson tagged jets,2267,0.0004411116012351125,,,nan,,NOT SCOAP3 Switzerland
1218051,18383,,,719,"Battilana, C.",Springer/SISSA,Search for dark matter in proton-proton collisions at 8 TeV with missing transverse momentum and vector boson tagged jets,2267,0.0004411116012351125,,,nan,,NOT SCOAP3 Switzerland
1218052,18383,,,789,"Pigazzini, S.",Springer/SISSA,Search for dark matter in proton-proton collisions at 8 TeV with missing transverse momentum and vector boson tagged jets,2267,0.0004411116012351125,,,nan,,NOT SCOAP3 Switzerland
1218053,18383,,,794,"Nardo, G.",Springer/SISSA,Search for dark matter in proton-proton collisions at 8 TeV with missing transverse momentum and vector boson tagged jets,2267,0.0004411116012351125,,,nan,,NOT SCOAP3 Switzerland
1218054,18383,,,804,"Thyssen, F.",Springer/SISSA,Search for dark matter in proton-proton collisions at 8 TeV with missing transverse momentum and vector boson tagged jets,2267,0.0004411116012351125,,,nan,,NOT SCOAP3 Switzerland
1218055,18383,,,828,"Zanetti, M.",Springer/SISSA,Search for dark matter in proton-proton collisions at 8 TeV with missing transverse momentum and vector boson tagged jets,2267,0.0004411116012351125,,,nan,,NOT SCOAP3 Switzerland
1218056,18383,,,860,"Fedi, G.",Springer/SISSA,Search for dark matter in proton-proton collisions at 8 TeV with missing transverse momentum and vector boson tagged jets,2267,0.0004411116012351125,,,nan,,NOT SCOAP3 Switzerland
1233310,18207,,,160,"Ruiz Vargas, J.",Springer/SISSA,"Search for new physics in final states with two opposite-sign, same-flavor leptons, jets, and missing transverse momentum in pp collisions at s = 13 $$ \sqrt{s}=13 $$ TeV",2257,0.00044306601683650863,,,nan,,NOT SCOAP3 Switzerland
1233311,18207,,,718,"Battilana, C.",Springer/SISSA,"Search for new physics in final states with two opposite-sign, same-flavor leptons, jets, and missing transverse momentum in pp collisions at s = 13 $$ \sqrt{s}=13 $$ TeV",2257,0.00044306601683650863,,,nan,,NOT SCOAP3 Switzerland
1233312,18207,,,775,"Brianza, L.",Springer/SISSA,"Search for new physics in final states with two opposite-sign, same-flavor leptons, jets, and missing transverse momentum in pp collisions at s = 13 $$ \sqrt{s}=13 $$ TeV",2257,0.00044306601683650863,,,nan,,NOT SCOAP3 Switzerland
1233313,18207,,,788,"Pigazzini, S.",Springer/SISSA,"Search for new physics in final states with two opposite-sign, same-flavor leptons, jets, and missing transverse momentum in pp collisions at s = 13 $$ \sqrt{s}=13 $$ TeV",2257,0.00044306601683650863,,,nan,,NOT SCOAP3 Switzerland
1233314,18207,,,793,"Nardo, G.",Springer/SISSA,"Search for new physics in final states with two opposite-sign, same-flavor leptons, jets, and missing transverse momentum in pp collisions at s = 13 $$ \sqrt{s}=13 $$ TeV",2257,0.00044306601683650863,,,nan,,NOT SCOAP3 Switzerland
1233315,18207,,,803,"Thyssen, F.",Springer/SISSA,"Search for new physics in final states with two opposite-sign, same-flavor leptons, jets, and missing transverse momentum in pp collisions at s = 13 $$ \sqrt{s}=13 $$ TeV",2257,0.00044306601683650863,,,nan,,NOT SCOAP3 Switzerland
1233316,18207,,,827,"Zanetti, M.",Springer/SISSA,"Search for new physics in final states with two opposite-sign, same-flavor leptons, jets, and missing transverse momentum in pp collisions at s = 13 $$ \sqrt{s}=13 $$ TeV",2257,0.00044306601683650863,,,nan,,NOT SCOAP3 Switzerland
1233317,18207,,,859,"Fedi, G.",Springer/SISSA,"Search for new physics in final states with two opposite-sign, same-flavor leptons, jets, and missing transverse momentum in pp collisions at s = 13 $$ \sqrt{s}=13 $$ TeV",2257,0.00044306601683650863,,,nan,,NOT SCOAP3 Switzerland
1252893,18098,,,175,"Ruiz Vargas, J.",Springer/SISSA,Measurement of electroweak production of a W boson and two forward jets in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2284,0.00043782837127845885,,,nan,,NOT SCOAP3 Switzerland
1252894,18098,,,791,"Brianza, L.",Springer/SISSA,Measurement of electroweak production of a W boson and two forward jets in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2284,0.00043782837127845885,,,nan,,NOT SCOAP3 Switzerland
1252895,18098,,,820,"Thyssen, F.",Springer/SISSA,Measurement of electroweak production of a W boson and two forward jets in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2284,0.00043782837127845885,,,nan,,NOT SCOAP3 Switzerland
1252896,18098,,,846,"Zanetti, M.",Springer/SISSA,Measurement of electroweak production of a W boson and two forward jets in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2284,0.00043782837127845885,,,nan,,NOT SCOAP3 Switzerland
1252897,18098,,,877,"Fedi, G.",Springer/SISSA,Measurement of electroweak production of a W boson and two forward jets in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2284,0.00043782837127845885,,,nan,,NOT SCOAP3 Switzerland
1268788,17893,,,159,"Ruiz Vargas, J.",Springer/SISSA,Decomposing transverse momentum balance contributions for quenched jets in PbPb collisions at s N N = 2.76 $$ \sqrt{s_{\mathrm{N}\;\mathrm{N}}}=2.76 $$ TeV,2264,0.00044169611307420494,,,nan,,NOT SCOAP3 Switzerland
1268789,17893,,,717,"Battilana, C.",Springer/SISSA,Decomposing transverse momentum balance contributions for quenched jets in PbPb collisions at s N N = 2.76 $$ \sqrt{s_{\mathrm{N}\;\mathrm{N}}}=2.76 $$ TeV,2264,0.00044169611307420494,,,nan,,NOT SCOAP3 Switzerland
1268790,17893,,,787,"Pigazzini, S.",Springer/SISSA,Decomposing transverse momentum balance contributions for quenched jets in PbPb collisions at s N N = 2.76 $$ \sqrt{s_{\mathrm{N}\;\mathrm{N}}}=2.76 $$ TeV,2264,0.00044169611307420494,,,nan,,NOT SCOAP3 Switzerland
1268791,17893,,,792,"Nardo, G.",Springer/SISSA,Decomposing transverse momentum balance contributions for quenched jets in PbPb collisions at s N N = 2.76 $$ \sqrt{s_{\mathrm{N}\;\mathrm{N}}}=2.76 $$ TeV,2264,0.00044169611307420494,,,nan,,NOT SCOAP3 Switzerland
1268792,17893,,,802,"Thyssen, F.",Springer/SISSA,Decomposing transverse momentum balance contributions for quenched jets in PbPb collisions at s N N = 2.76 $$ \sqrt{s_{\mathrm{N}\;\mathrm{N}}}=2.76 $$ TeV,2264,0.00044169611307420494,,,nan,,NOT SCOAP3 Switzerland
1268793,17893,,,826,"Zanetti, M.",Springer/SISSA,Decomposing transverse momentum balance contributions for quenched jets in PbPb collisions at s N N = 2.76 $$ \sqrt{s_{\mathrm{N}\;\mathrm{N}}}=2.76 $$ TeV,2264,0.00044169611307420494,,,nan,,NOT SCOAP3 Switzerland
1268794,17893,,,858,"Fedi, G.",Springer/SISSA,Decomposing transverse momentum balance contributions for quenched jets in PbPb collisions at s N N = 2.76 $$ \sqrt{s_{\mathrm{N}\;\mathrm{N}}}=2.76 $$ TeV,2264,0.00044169611307420494,,,nan,,NOT SCOAP3 Switzerland
1271336,17868,,,166,"Ahuja, S.",Springer/SISSA,Erratum to: Search for third-generation scalar leptoquarks in the tτ channel in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2282,0.00043821209465381246,,,nan,,NOT SCOAP3 Switzerland
1271337,17868,,,174,"Romero Abad, D.",Springer/SISSA,Erratum to: Search for third-generation scalar leptoquarks in the tτ channel in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2282,0.00043821209465381246,,,nan,,NOT SCOAP3 Switzerland
1271338,17868,,,175,"Ruiz Vargas, J.",Springer/SISSA,Erratum to: Search for third-generation scalar leptoquarks in the tτ channel in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2282,0.00043821209465381246,,,nan,,NOT SCOAP3 Switzerland
1271339,17868,,,741,"Battilana, C.",Springer/SISSA,Erratum to: Search for third-generation scalar leptoquarks in the tτ channel in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2282,0.00043821209465381246,,,nan,,NOT SCOAP3 Switzerland
1271340,17868,,,884,"Fedi, G.",Springer/SISSA,Erratum to: Search for third-generation scalar leptoquarks in the tτ channel in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2282,0.00043821209465381246,,,nan,,NOT SCOAP3 Switzerland
1291998,17672,,,174,"Ruiz Vargas, J.",Springer/SISSA,Phenomenological MSSM interpretation of CMS searches in pp collisions at s = 7 $$ \sqrt{s}=7 $$ and 8 TeV,2290,0.0004366812227074236,,,nan,,NOT SCOAP3 Switzerland
1291999,17672,,,793,"Brianza, L.",Springer/SISSA,Phenomenological MSSM interpretation of CMS searches in pp collisions at s = 7 $$ \sqrt{s}=7 $$ and 8 TeV,2290,0.0004366812227074236,,,nan,,NOT SCOAP3 Switzerland
1292000,17672,,,807,"Pigazzini, S.",Springer/SISSA,Phenomenological MSSM interpretation of CMS searches in pp collisions at s = 7 $$ \sqrt{s}=7 $$ and 8 TeV,2290,0.0004366812227074236,,,nan,,NOT SCOAP3 Switzerland
1292001,17672,,,823,"Thyssen, F.",Springer/SISSA,Phenomenological MSSM interpretation of CMS searches in pp collisions at s = 7 $$ \sqrt{s}=7 $$ and 8 TeV,2290,0.0004366812227074236,,,nan,,NOT SCOAP3 Switzerland
1292002,17672,,,849,"Zanetti, M.",Springer/SISSA,Phenomenological MSSM interpretation of CMS searches in pp collisions at s = 7 $$ \sqrt{s}=7 $$ and 8 TeV,2290,0.0004366812227074236,,,nan,,NOT SCOAP3 Switzerland
1292003,17672,,,880,"Fedi, G.",Springer/SISSA,Phenomenological MSSM interpretation of CMS searches in pp collisions at s = 7 $$ \sqrt{s}=7 $$ and 8 TeV,2290,0.0004366812227074236,,,nan,,NOT SCOAP3 Switzerland
1320239,17399,,,162,"Ruiz Vargas, J.",Springer/SISSA,Search for new physics with the M T2 variable in all-jets final states produced in pp collisions at s = 13 $$ \sqrt{s}=13 $$ TeV,2270,0.0004405286343612335,,,nan,,NOT SCOAP3 Switzerland
1320240,17399,,,730,"Battilana, C.",Springer/SISSA,Search for new physics with the M T2 variable in all-jets final states produced in pp collisions at s = 13 $$ \sqrt{s}=13 $$ TeV,2270,0.0004405286343612335,,,nan,,NOT SCOAP3 Switzerland
1320241,17399,,,787,"Brianza, L.",Springer/SISSA,Search for new physics with the M T2 variable in all-jets final states produced in pp collisions at s = 13 $$ \sqrt{s}=13 $$ TeV,2270,0.0004405286343612335,,,nan,,NOT SCOAP3 Switzerland
1320242,17399,,,800,"Pigazzini, S.",Springer/SISSA,Search for new physics with the M T2 variable in all-jets final states produced in pp collisions at s = 13 $$ \sqrt{s}=13 $$ TeV,2270,0.0004405286343612335,,,nan,,NOT SCOAP3 Switzerland
1320243,17399,,,805,"Nardo, G.",Springer/SISSA,Search for new physics with the M T2 variable in all-jets final states produced in pp collisions at s = 13 $$ \sqrt{s}=13 $$ TeV,2270,0.0004405286343612335,,,nan,,NOT SCOAP3 Switzerland
1320244,17399,,,816,"Thyssen, F.",Springer/SISSA,Search for new physics with the M T2 variable in all-jets final states produced in pp collisions at s = 13 $$ \sqrt{s}=13 $$ TeV,2270,0.0004405286343612335,,,nan,,NOT SCOAP3 Switzerland
1320245,17399,,,841,"Zanetti, M.",Springer/SISSA,Search for new physics with the M T2 variable in all-jets final states produced in pp collisions at s = 13 $$ \sqrt{s}=13 $$ TeV,2270,0.0004405286343612335,,,nan,,NOT SCOAP3 Switzerland
1320246,17399,,,873,"Fedi, G.",Springer/SISSA,Search for new physics with the M T2 variable in all-jets final states produced in pp collisions at s = 13 $$ \sqrt{s}=13 $$ TeV,2270,0.0004405286343612335,,,nan,,NOT SCOAP3 Switzerland
1352665,17130,,,174,"Romero Abad, D.",Springer/SISSA,Erratum to: Search for direct pair production of scalar top quarks in the single- and dilepton channels in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2285,0.000437636761487965,,,nan,,NOT SCOAP3 Switzerland
1352666,17130,,,175,"Ruiz Vargas, J.",Springer/SISSA,Erratum to: Search for direct pair production of scalar top quarks in the single- and dilepton channels in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2285,0.000437636761487965,,,nan,,NOT SCOAP3 Switzerland
1352667,17130,,,791,"Brianza, L.",Springer/SISSA,Erratum to: Search for direct pair production of scalar top quarks in the single- and dilepton channels in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2285,0.000437636761487965,,,nan,,NOT SCOAP3 Switzerland
1352668,17130,,,820,"Thyssen, F.",Springer/SISSA,Erratum to: Search for direct pair production of scalar top quarks in the single- and dilepton channels in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2285,0.000437636761487965,,,nan,,NOT SCOAP3 Switzerland
1352669,17130,,,847,"Zanetti, M.",Springer/SISSA,Erratum to: Search for direct pair production of scalar top quarks in the single- and dilepton channels in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2285,0.000437636761487965,,,nan,,NOT SCOAP3 Switzerland
1352670,17130,,,877,"Fedi, G.",Springer/SISSA,Erratum to: Search for direct pair production of scalar top quarks in the single- and dilepton channels in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2285,0.000437636761487965,,,nan,,NOT SCOAP3 Switzerland
1358300,17108,,,170,"Ruiz Vargas, J.",Springer/SISSA,Search for Higgs boson off-shell production in proton-proton collisions at 7 and 8 TeV and derivation of constraints on its total decay width,2299,0.00043497172683775554,,,nan,,NOT SCOAP3 Switzerland
1358301,17108,,,789,"Brianza, L.",Springer/SISSA,Search for Higgs boson off-shell production in proton-proton collisions at 7 and 8 TeV and derivation of constraints on its total decay width,2299,0.00043497172683775554,,,nan,,NOT SCOAP3 Switzerland
1358302,17108,,,803,"Pigazzini, S.",Springer/SISSA,Search for Higgs boson off-shell production in proton-proton collisions at 7 and 8 TeV and derivation of constraints on its total decay width,2299,0.00043497172683775554,,,nan,,NOT SCOAP3 Switzerland
1358303,17108,,,819,"Thyssen, F.",Springer/SISSA,Search for Higgs boson off-shell production in proton-proton collisions at 7 and 8 TeV and derivation of constraints on its total decay width,2299,0.00043497172683775554,,,nan,,NOT SCOAP3 Switzerland
1358304,17108,,,845,"Zanetti, M.",Springer/SISSA,Search for Higgs boson off-shell production in proton-proton collisions at 7 and 8 TeV and derivation of constraints on its total decay width,2299,0.00043497172683775554,,,nan,,NOT SCOAP3 Switzerland
1358305,17108,,,877,"Fedi, G.",Springer/SISSA,Search for Higgs boson off-shell production in proton-proton collisions at 7 and 8 TeV and derivation of constraints on its total decay width,2299,0.00043497172683775554,,,nan,,NOT SCOAP3 Switzerland
1367130,17087,,,175,"Ruiz Vargas, J.",Springer/SISSA,Search for s channel single top quark production in pp collisions at s = 7 $$ \sqrt{s}=7 $$ and 8 TeV,2285,0.000437636761487965,,,nan,,NOT SCOAP3 Switzerland
1367131,17087,,,790,"Brianza, L.",Springer/SISSA,Search for s channel single top quark production in pp collisions at s = 7 $$ \sqrt{s}=7 $$ and 8 TeV,2285,0.000437636761487965,,,nan,,NOT SCOAP3 Switzerland
1367132,17087,,,819,"Thyssen, F.",Springer/SISSA,Search for s channel single top quark production in pp collisions at s = 7 $$ \sqrt{s}=7 $$ and 8 TeV,2285,0.000437636761487965,,,nan,,NOT SCOAP3 Switzerland
1367133,17087,,,846,"Zanetti, M.",Springer/SISSA,Search for s channel single top quark production in pp collisions at s = 7 $$ \sqrt{s}=7 $$ and 8 TeV,2285,0.000437636761487965,,,nan,,NOT SCOAP3 Switzerland
1367134,17087,,,877,"Fedi, G.",Springer/SISSA,Search for s channel single top quark production in pp collisions at s = 7 $$ \sqrt{s}=7 $$ and 8 TeV,2285,0.000437636761487965,,,nan,,NOT SCOAP3 Switzerland
1386842,16970,,,178,"Romero Abad, D.",Springer/SISSA,Azimuthal decorrelation of jets widely separated in rapidity in pp collisions at s = 7 $$ \sqrt{s}=7 $$ TeV,2311,0.00043271311120726956,,,nan,,NOT SCOAP3 Switzerland
1386843,16970,,,179,"Ruiz Vargas, J.",Springer/SISSA,Azimuthal decorrelation of jets widely separated in rapidity in pp collisions at s = 7 $$ \sqrt{s}=7 $$ TeV,2311,0.00043271311120726956,,,nan,,NOT SCOAP3 Switzerland
1386844,16970,,,805,"Brianza, L.",Springer/SISSA,Azimuthal decorrelation of jets widely separated in rapidity in pp collisions at s = 7 $$ \sqrt{s}=7 $$ TeV,2311,0.00043271311120726956,,,nan,,NOT SCOAP3 Switzerland
1386845,16970,,,834,"Thyssen, F.",Springer/SISSA,Azimuthal decorrelation of jets widely separated in rapidity in pp collisions at s = 7 $$ \sqrt{s}=7 $$ TeV,2311,0.00043271311120726956,,,nan,,NOT SCOAP3 Switzerland
1386846,16970,,,860,"Zanetti, M.",Springer/SISSA,Azimuthal decorrelation of jets widely separated in rapidity in pp collisions at s = 7 $$ \sqrt{s}=7 $$ TeV,2311,0.00043271311120726956,,,nan,,NOT SCOAP3 Switzerland
1386847,16970,,,894,"Fedi, G.",Springer/SISSA,Azimuthal decorrelation of jets widely separated in rapidity in pp collisions at s = 7 $$ \sqrt{s}=7 $$ TeV,2311,0.00043271311120726956,,,nan,,NOT SCOAP3 Switzerland
1389398,16953,,,177,"Ruiz Vargas, J.",Springer/SISSA,Evidence for exclusive γγ → W + W − production and constraints on anomalous quartic gauge couplings in pp collisions at s = 7 $$ \sqrt{s}=7 $$ and 8 TeV,2282,0.00043821209465381246,,,nan,,NOT SCOAP3 Switzerland
1389399,16953,,,790,"Brianza, L.",Springer/SISSA,Evidence for exclusive γγ → W + W − production and constraints on anomalous quartic gauge couplings in pp collisions at s = 7 $$ \sqrt{s}=7 $$ and 8 TeV,2282,0.00043821209465381246,,,nan,,NOT SCOAP3 Switzerland
1389400,16953,,,819,"Thyssen, F.",Springer/SISSA,Evidence for exclusive γγ → W + W − production and constraints on anomalous quartic gauge couplings in pp collisions at s = 7 $$ \sqrt{s}=7 $$ and 8 TeV,2282,0.00043821209465381246,,,nan,,NOT SCOAP3 Switzerland
1389401,16953,,,846,"Zanetti, M.",Springer/SISSA,Evidence for exclusive γγ → W + W − production and constraints on anomalous quartic gauge couplings in pp collisions at s = 7 $$ \sqrt{s}=7 $$ and 8 TeV,2282,0.00043821209465381246,,,nan,,NOT SCOAP3 Switzerland
1389402,16953,,,876,"Fedi, G.",Springer/SISSA,Evidence for exclusive γγ → W + W − production and constraints on anomalous quartic gauge couplings in pp collisions at s = 7 $$ \sqrt{s}=7 $$ and 8 TeV,2282,0.00043821209465381246,,,nan,,NOT SCOAP3 Switzerland
1394212,16982,,,159,"Ruiz Vargas, J.",Springer/SISSA,Search for supersymmetry in pp collisions at s = 13 $$ \sqrt{s}=13 $$ TeV in the single-lepton final state using the sum of masses of large-radius jets,2258,0.0004428697962798937,,,nan,,NOT SCOAP3 Switzerland
1394213,16982,,,718,"Battilana, C.",Springer/SISSA,Search for supersymmetry in pp collisions at s = 13 $$ \sqrt{s}=13 $$ TeV in the single-lepton final state using the sum of masses of large-radius jets,2258,0.0004428697962798937,,,nan,,NOT SCOAP3 Switzerland
1394214,16982,,,775,"Brianza, L.",Springer/SISSA,Search for supersymmetry in pp collisions at s = 13 $$ \sqrt{s}=13 $$ TeV in the single-lepton final state using the sum of masses of large-radius jets,2258,0.0004428697962798937,,,nan,,NOT SCOAP3 Switzerland
1394215,16982,,,788,"Pigazzini, S.",Springer/SISSA,Search for supersymmetry in pp collisions at s = 13 $$ \sqrt{s}=13 $$ TeV in the single-lepton final state using the sum of masses of large-radius jets,2258,0.0004428697962798937,,,nan,,NOT SCOAP3 Switzerland
1394216,16982,,,793,"Nardo, G.",Springer/SISSA,Search for supersymmetry in pp collisions at s = 13 $$ \sqrt{s}=13 $$ TeV in the single-lepton final state using the sum of masses of large-radius jets,2258,0.0004428697962798937,,,nan,,NOT SCOAP3 Switzerland
1394217,16982,,,804,"Thyssen, F.",Springer/SISSA,Search for supersymmetry in pp collisions at s = 13 $$ \sqrt{s}=13 $$ TeV in the single-lepton final state using the sum of masses of large-radius jets,2258,0.0004428697962798937,,,nan,,NOT SCOAP3 Switzerland
1394218,16982,,,828,"Zanetti, M.",Springer/SISSA,Search for supersymmetry in pp collisions at s = 13 $$ \sqrt{s}=13 $$ TeV in the single-lepton final state using the sum of masses of large-radius jets,2258,0.0004428697962798937,,,nan,,NOT SCOAP3 Switzerland
1394219,16982,,,860,"Fedi, G.",Springer/SISSA,Search for supersymmetry in pp collisions at s = 13 $$ \sqrt{s}=13 $$ TeV in the single-lepton final state using the sum of masses of large-radius jets,2258,0.0004428697962798937,,,nan,,NOT SCOAP3 Switzerland
1419060,16939,,,3006,"Ruiz Vargas, J.",Springer/SISSA,Measurements of the Higgs boson production and decay rates and constraints on its couplings from a combined ATLAS and CMS analysis of the LHC pp collision data at s = 7 $$ \sqrt{s}=7 $$ and 8 TeV,5112,0.00019561815336463224,,,nan,,NOT SCOAP3 Switzerland
1419061,16939,,,3573,"Battilana, C.",Springer/SISSA,Measurements of the Higgs boson production and decay rates and constraints on its couplings from a combined ATLAS and CMS analysis of the LHC pp collision data at s = 7 $$ \sqrt{s}=7 $$ and 8 TeV,5112,0.00019561815336463224,,,nan,,NOT SCOAP3 Switzerland
1419062,16939,,,3630,"Brianza, L.",Springer/SISSA,Measurements of the Higgs boson production and decay rates and constraints on its couplings from a combined ATLAS and CMS analysis of the LHC pp collision data at s = 7 $$ \sqrt{s}=7 $$ and 8 TeV,5112,0.00019561815336463224,,,nan,,NOT SCOAP3 Switzerland
1419063,16939,,,3643,"Pigazzini, S.",Springer/SISSA,Measurements of the Higgs boson production and decay rates and constraints on its couplings from a combined ATLAS and CMS analysis of the LHC pp collision data at s = 7 $$ \sqrt{s}=7 $$ and 8 TeV,5112,0.00019561815336463224,,,nan,,NOT SCOAP3 Switzerland
1419064,16939,,,3648,"Nardo, G.",Springer/SISSA,Measurements of the Higgs boson production and decay rates and constraints on its couplings from a combined ATLAS and CMS analysis of the LHC pp collision data at s = 7 $$ \sqrt{s}=7 $$ and 8 TeV,5112,0.00019561815336463224,,,nan,,NOT SCOAP3 Switzerland
1419065,16939,,,3659,"Thyssen, F.",Springer/SISSA,Measurements of the Higgs boson production and decay rates and constraints on its couplings from a combined ATLAS and CMS analysis of the LHC pp collision data at s = 7 $$ \sqrt{s}=7 $$ and 8 TeV,5112,0.00019561815336463224,,,nan,,NOT SCOAP3 Switzerland
1419066,16939,,,3684,"Zanetti, M.",Springer/SISSA,Measurements of the Higgs boson production and decay rates and constraints on its couplings from a combined ATLAS and CMS analysis of the LHC pp collision data at s = 7 $$ \sqrt{s}=7 $$ and 8 TeV,5112,0.00019561815336463224,,,nan,,NOT SCOAP3 Switzerland
1419067,16939,,,3716,"Fedi, G.",Springer/SISSA,Measurements of the Higgs boson production and decay rates and constraints on its couplings from a combined ATLAS and CMS analysis of the LHC pp collision data at s = 7 $$ \sqrt{s}=7 $$ and 8 TeV,5112,0.00019561815336463224,,,nan,,NOT SCOAP3 Switzerland
1424068,16700,,,170,"Ruiz Vargas, J.",Springer/SISSA,Measurement of the t t ¯ $$ \mathrm{t}\overline{\mathrm{t}} $$ production cross section in the e μ channel in proton-proton collisions at s = 7 $$ \sqrt{s}=7 $$ and 8 TeV,2302,0.0004344048653344917,,,nan,,NOT SCOAP3 Switzerland
1424069,16700,,,793,"Brianza, L.",Springer/SISSA,Measurement of the t t ¯ $$ \mathrm{t}\overline{\mathrm{t}} $$ production cross section in the e μ channel in proton-proton collisions at s = 7 $$ \sqrt{s}=7 $$ and 8 TeV,2302,0.0004344048653344917,,,nan,,NOT SCOAP3 Switzerland
1424070,16700,,,807,"Pigazzini, S.",Springer/SISSA,Measurement of the t t ¯ $$ \mathrm{t}\overline{\mathrm{t}} $$ production cross section in the e μ channel in proton-proton collisions at s = 7 $$ \sqrt{s}=7 $$ and 8 TeV,2302,0.0004344048653344917,,,nan,,NOT SCOAP3 Switzerland
1424071,16700,,,823,"Thyssen, F.",Springer/SISSA,Measurement of the t t ¯ $$ \mathrm{t}\overline{\mathrm{t}} $$ production cross section in the e μ channel in proton-proton collisions at s = 7 $$ \sqrt{s}=7 $$ and 8 TeV,2302,0.0004344048653344917,,,nan,,NOT SCOAP3 Switzerland
1424072,16700,,,849,"Zanetti, M.",Springer/SISSA,Measurement of the t t ¯ $$ \mathrm{t}\overline{\mathrm{t}} $$ production cross section in the e μ channel in proton-proton collisions at s = 7 $$ \sqrt{s}=7 $$ and 8 TeV,2302,0.0004344048653344917,,,nan,,NOT SCOAP3 Switzerland
1424073,16700,,,881,"Fedi, G.",Springer/SISSA,Measurement of the t t ¯ $$ \mathrm{t}\overline{\mathrm{t}} $$ production cross section in the e μ channel in proton-proton collisions at s = 7 $$ \sqrt{s}=7 $$ and 8 TeV,2302,0.0004344048653344917,,,nan,,NOT SCOAP3 Switzerland
1462722,16358,,,174,"Romero Abad, D.",Springer/SISSA,Search for direct pair production of scalar top quarks in the single- and dilepton channels in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2285,0.000437636761487965,,,nan,,NOT SCOAP3 Switzerland
1462723,16358,,,175,"Ruiz Vargas, J.",Springer/SISSA,Search for direct pair production of scalar top quarks in the single- and dilepton channels in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2285,0.000437636761487965,,,nan,,NOT SCOAP3 Switzerland
1462724,16358,,,791,"Brianza, L.",Springer/SISSA,Search for direct pair production of scalar top quarks in the single- and dilepton channels in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2285,0.000437636761487965,,,nan,,NOT SCOAP3 Switzerland
1462725,16358,,,820,"Thyssen, F.",Springer/SISSA,Search for direct pair production of scalar top quarks in the single- and dilepton channels in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2285,0.000437636761487965,,,nan,,NOT SCOAP3 Switzerland
1462726,16358,,,847,"Zanetti, M.",Springer/SISSA,Search for direct pair production of scalar top quarks in the single- and dilepton channels in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2285,0.000437636761487965,,,nan,,NOT SCOAP3 Switzerland
1462727,16358,,,877,"Fedi, G.",Springer/SISSA,Search for direct pair production of scalar top quarks in the single- and dilepton channels in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2285,0.000437636761487965,,,nan,,NOT SCOAP3 Switzerland
1469891,16322,,,176,"Romero Abad, D.",Springer/SISSA,Search for the associated production of a Higgs boson with a single top quark in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2307,0.00043346337234503684,,,nan,,NOT SCOAP3 Switzerland
1469892,16322,,,177,"Ruiz Vargas, J.",Springer/SISSA,Search for the associated production of a Higgs boson with a single top quark in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2307,0.00043346337234503684,,,nan,,NOT SCOAP3 Switzerland
1469893,16322,,,800,"Brianza, L.",Springer/SISSA,Search for the associated production of a Higgs boson with a single top quark in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2307,0.00043346337234503684,,,nan,,NOT SCOAP3 Switzerland
1469894,16322,,,829,"Thyssen, F.",Springer/SISSA,Search for the associated production of a Higgs boson with a single top quark in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2307,0.00043346337234503684,,,nan,,NOT SCOAP3 Switzerland
1469895,16322,,,855,"Zanetti, M.",Springer/SISSA,Search for the associated production of a Higgs boson with a single top quark in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2307,0.00043346337234503684,,,nan,,NOT SCOAP3 Switzerland
1469896,16322,,,888,"Fedi, G.",Springer/SISSA,Search for the associated production of a Higgs boson with a single top quark in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2307,0.00043346337234503684,,,nan,,NOT SCOAP3 Switzerland
1564190,15437,,,173,"Ruiz Vargas, J.",Springer/SISSA,Search for heavy Majorana neutrinos in e ± e ± + jets and e ± μ ± + jets events in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2292,0.0004363001745200698,,,nan,,NOT SCOAP3 Switzerland
1564191,15437,,,789,"Brianza, L.",Springer/SISSA,Search for heavy Majorana neutrinos in e ± e ± + jets and e ± μ ± + jets events in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2292,0.0004363001745200698,,,nan,,NOT SCOAP3 Switzerland
1564192,15437,,,803,"Pigazzini, S.",Springer/SISSA,Search for heavy Majorana neutrinos in e ± e ± + jets and e ± μ ± + jets events in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2292,0.0004363001745200698,,,nan,,NOT SCOAP3 Switzerland
1564193,15437,,,819,"Thyssen, F.",Springer/SISSA,Search for heavy Majorana neutrinos in e ± e ± + jets and e ± μ ± + jets events in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2292,0.0004363001745200698,,,nan,,NOT SCOAP3 Switzerland
1564194,15437,,,845,"Zanetti, M.",Springer/SISSA,Search for heavy Majorana neutrinos in e ± e ± + jets and e ± μ ± + jets events in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2292,0.0004363001745200698,,,nan,,NOT SCOAP3 Switzerland
1564195,15437,,,877,"Fedi, G.",Springer/SISSA,Search for heavy Majorana neutrinos in e ± e ± + jets and e ± μ ± + jets events in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2292,0.0004363001745200698,,,nan,,NOT SCOAP3 Switzerland
1572999,15239,,,174,"Romero Abad, D.",Springer/SISSA,Measurement of top quark polarisation in t -channel single top quark production,2299,0.00043497172683775554,,,nan,,NOT SCOAP3 Switzerland
1573000,15239,,,175,"Ruiz Vargas, J.",Springer/SISSA,Measurement of top quark polarisation in t -channel single top quark production,2299,0.00043497172683775554,,,nan,,NOT SCOAP3 Switzerland
1573001,15239,,,803,"Brianza, L.",Springer/SISSA,Measurement of top quark polarisation in t -channel single top quark production,2299,0.00043497172683775554,,,nan,,NOT SCOAP3 Switzerland
1573002,15239,,,832,"Thyssen, F.",Springer/SISSA,Measurement of top quark polarisation in t -channel single top quark production,2299,0.00043497172683775554,,,nan,,NOT SCOAP3 Switzerland
1573003,15239,,,858,"Zanetti, M.",Springer/SISSA,Measurement of top quark polarisation in t -channel single top quark production,2299,0.00043497172683775554,,,nan,,NOT SCOAP3 Switzerland
1573004,15239,,,889,"Fedi, G.",Springer/SISSA,Measurement of top quark polarisation in t -channel single top quark production,2299,0.00043497172683775554,,,nan,,NOT SCOAP3 Switzerland
1582212,15129,,,175,"Romero Abad, D.",Springer/SISSA,Search for anomalous single top quark production in association with a photon in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2307,0.00043346337234503684,,,nan,,NOT SCOAP3 Switzerland
1582213,15129,,,176,"Ruiz Vargas, J.",Springer/SISSA,Search for anomalous single top quark production in association with a photon in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2307,0.00043346337234503684,,,nan,,NOT SCOAP3 Switzerland
1582214,15129,,,799,"Brianza, L.",Springer/SISSA,Search for anomalous single top quark production in association with a photon in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2307,0.00043346337234503684,,,nan,,NOT SCOAP3 Switzerland
1582215,15129,,,828,"Thyssen, F.",Springer/SISSA,Search for anomalous single top quark production in association with a photon in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2307,0.00043346337234503684,,,nan,,NOT SCOAP3 Switzerland
1582216,15129,,,854,"Zanetti, M.",Springer/SISSA,Search for anomalous single top quark production in association with a photon in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2307,0.00043346337234503684,,,nan,,NOT SCOAP3 Switzerland
1582217,15129,,,888,"Fedi, G.",Springer/SISSA,Search for anomalous single top quark production in association with a photon in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2307,0.00043346337234503684,,,nan,,NOT SCOAP3 Switzerland
1588703,15100,,,166,"Ahuja, S.",Springer/SISSA,Erratum to: Comparison of the Z/γ * + jets to γ + jets cross sections in pp collisions at s = 8 $$ \sqrt{s}=8 $$,2289,0.00043687199650502403,,,nan,,NOT SCOAP3 Switzerland
1588704,15100,,,175,"Romero Abad, D.",Springer/SISSA,Erratum to: Comparison of the Z/γ * + jets to γ + jets cross sections in pp collisions at s = 8 $$ \sqrt{s}=8 $$,2289,0.00043687199650502403,,,nan,,NOT SCOAP3 Switzerland
1588705,15100,,,176,"Ruiz Vargas, J.",Springer/SISSA,Erratum to: Comparison of the Z/γ * + jets to γ + jets cross sections in pp collisions at s = 8 $$ \sqrt{s}=8 $$,2289,0.00043687199650502403,,,nan,,NOT SCOAP3 Switzerland
1588706,15100,,,742,"Battilana, C.",Springer/SISSA,Erratum to: Comparison of the Z/γ * + jets to γ + jets cross sections in pp collisions at s = 8 $$ \sqrt{s}=8 $$,2289,0.00043687199650502403,,,nan,,NOT SCOAP3 Switzerland
1588707,15100,,,828,"Thyssen, F.",Springer/SISSA,Erratum to: Comparison of the Z/γ * + jets to γ + jets cross sections in pp collisions at s = 8 $$ \sqrt{s}=8 $$,2289,0.00043687199650502403,,,nan,,NOT SCOAP3 Switzerland
1588708,15100,,,852,"Zanetti, M.",Springer/SISSA,Erratum to: Comparison of the Z/γ * + jets to γ + jets cross sections in pp collisions at s = 8 $$ \sqrt{s}=8 $$,2289,0.00043687199650502403,,,nan,,NOT SCOAP3 Switzerland
1588709,15100,,,886,"Fedi, G.",Springer/SISSA,Erratum to: Comparison of the Z/γ * + jets to γ + jets cross sections in pp collisions at s = 8 $$ \sqrt{s}=8 $$,2289,0.00043687199650502403,,,nan,,NOT SCOAP3 Switzerland
1591278,15049,,,174,"Romero Abad, D.",Springer/SISSA,Measurement of differential and integrated fiducial cross sections for Higgs boson production in the four-lepton decay channel in pp collisions at s = 7 $$ \sqrt{s}=7 $$ and 8 TeV,2302,0.0004344048653344917,,,nan,,NOT SCOAP3 Switzerland
1591279,15049,,,175,"Ruiz Vargas, J.",Springer/SISSA,Measurement of differential and integrated fiducial cross sections for Higgs boson production in the four-lepton decay channel in pp collisions at s = 7 $$ \sqrt{s}=7 $$ and 8 TeV,2302,0.0004344048653344917,,,nan,,NOT SCOAP3 Switzerland
1591280,15049,,,801,"Brianza, L.",Springer/SISSA,Measurement of differential and integrated fiducial cross sections for Higgs boson production in the four-lepton decay channel in pp collisions at s = 7 $$ \sqrt{s}=7 $$ and 8 TeV,2302,0.0004344048653344917,,,nan,,NOT SCOAP3 Switzerland
1591281,15049,,,830,"Thyssen, F.",Springer/SISSA,Measurement of differential and integrated fiducial cross sections for Higgs boson production in the four-lepton decay channel in pp collisions at s = 7 $$ \sqrt{s}=7 $$ and 8 TeV,2302,0.0004344048653344917,,,nan,,NOT SCOAP3 Switzerland
1591282,15049,,,856,"Zanetti, M.",Springer/SISSA,Measurement of differential and integrated fiducial cross sections for Higgs boson production in the four-lepton decay channel in pp collisions at s = 7 $$ \sqrt{s}=7 $$ and 8 TeV,2302,0.0004344048653344917,,,nan,,NOT SCOAP3 Switzerland
1591283,15049,,,888,"Fedi, G.",Springer/SISSA,Measurement of differential and integrated fiducial cross sections for Higgs boson production in the four-lepton decay channel in pp collisions at s = 7 $$ \sqrt{s}=7 $$ and 8 TeV,2302,0.0004344048653344917,,,nan,,NOT SCOAP3 Switzerland
1605562,14863,,,175,"Romero Abad, D.",Springer/SISSA,Search for excited leptons in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2306,0.0004336513443191674,,,nan,,NOT SCOAP3 Switzerland
1605563,14863,,,176,"Ruiz Vargas, J.",Springer/SISSA,Search for excited leptons in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2306,0.0004336513443191674,,,nan,,NOT SCOAP3 Switzerland
1605564,14863,,,799,"Brianza, L.",Springer/SISSA,Search for excited leptons in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2306,0.0004336513443191674,,,nan,,NOT SCOAP3 Switzerland
1605565,14863,,,828,"Thyssen, F.",Springer/SISSA,Search for excited leptons in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2306,0.0004336513443191674,,,nan,,NOT SCOAP3 Switzerland
1605566,14863,,,854,"Zanetti, M.",Springer/SISSA,Search for excited leptons in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2306,0.0004336513443191674,,,nan,,NOT SCOAP3 Switzerland
1605567,14863,,,888,"Fedi, G.",Springer/SISSA,Search for excited leptons in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2306,0.0004336513443191674,,,nan,,NOT SCOAP3 Switzerland
1641638,14516,,,173,"Romero Abad, D.",Springer/SISSA,Correlations between jets and charged particles in PbPb and pp collisions at s N N = 2.76 $$ \sqrt{s_{\mathrm{NN}}}=2.76 $$ TeV,2272,0.00044014084507042255,,,nan,,NOT SCOAP3 Switzerland
1641639,14516,,,174,"Ruiz Vargas, J.",Springer/SISSA,Correlations between jets and charged particles in PbPb and pp collisions at s N N = 2.76 $$ \sqrt{s_{\mathrm{NN}}}=2.76 $$ TeV,2272,0.00044014084507042255,,,nan,,NOT SCOAP3 Switzerland
1641640,14516,,,791,"Brianza, L.",Springer/SISSA,Correlations between jets and charged particles in PbPb and pp collisions at s N N = 2.76 $$ \sqrt{s_{\mathrm{NN}}}=2.76 $$ TeV,2272,0.00044014084507042255,,,nan,,NOT SCOAP3 Switzerland
1641641,14516,,,820,"Thyssen, F.",Springer/SISSA,Correlations between jets and charged particles in PbPb and pp collisions at s N N = 2.76 $$ \sqrt{s_{\mathrm{NN}}}=2.76 $$ TeV,2272,0.00044014084507042255,,,nan,,NOT SCOAP3 Switzerland
1641642,14516,,,846,"Zanetti, M.",Springer/SISSA,Correlations between jets and charged particles in PbPb and pp collisions at s N N = 2.76 $$ \sqrt{s_{\mathrm{NN}}}=2.76 $$ TeV,2272,0.00044014084507042255,,,nan,,NOT SCOAP3 Switzerland
1641643,14516,,,877,"Fedi, G.",Springer/SISSA,Correlations between jets and charged particles in PbPb and pp collisions at s N N = 2.76 $$ \sqrt{s_{\mathrm{NN}}}=2.76 $$ TeV,2272,0.00044014084507042255,,,nan,,NOT SCOAP3 Switzerland
1644174,14551,,,167,"Ahuja, S.",Springer/SISSA,Search for a massive resonance decaying into a Higgs boson and a W or Z boson in hadronic final states in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2275,0.00043956043956043956,,,nan,,NOT SCOAP3 Switzerland
1644175,14551,,,175,"Romero Abad, D.",Springer/SISSA,Search for a massive resonance decaying into a Higgs boson and a W or Z boson in hadronic final states in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2275,0.00043956043956043956,,,nan,,NOT SCOAP3 Switzerland
1644176,14551,,,176,"Ruiz Vargas, J.",Springer/SISSA,Search for a massive resonance decaying into a Higgs boson and a W or Z boson in hadronic final states in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2275,0.00043956043956043956,,,nan,,NOT SCOAP3 Switzerland
1644177,14551,,,734,"Battilana, C.",Springer/SISSA,Search for a massive resonance decaying into a Higgs boson and a W or Z boson in hadronic final states in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2275,0.00043956043956043956,,,nan,,NOT SCOAP3 Switzerland
1644178,14551,,,843,"Zanetti, M.",Springer/SISSA,Search for a massive resonance decaying into a Higgs boson and a W or Z boson in hadronic final states in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2275,0.00043956043956043956,,,nan,,NOT SCOAP3 Switzerland
1644179,14551,,,876,"Fedi, G.",Springer/SISSA,Search for a massive resonance decaying into a Higgs boson and a W or Z boson in hadronic final states in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2275,0.00043956043956043956,,,nan,,NOT SCOAP3 Switzerland
1650615,14436,,,167,"Ahuja, S.",Springer/SISSA,Search for W′ → tb in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2283,0.0004380201489268506,,,nan,,NOT SCOAP3 Switzerland
1650616,14436,,,175,"Romero Abad, D.",Springer/SISSA,Search for W′ → tb in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2283,0.0004380201489268506,,,nan,,NOT SCOAP3 Switzerland
1650617,14436,,,176,"Ruiz Vargas, J.",Springer/SISSA,Search for W′ → tb in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2283,0.0004380201489268506,,,nan,,NOT SCOAP3 Switzerland
1650618,14436,,,737,"Battilana, C.",Springer/SISSA,Search for W′ → tb in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2283,0.0004380201489268506,,,nan,,NOT SCOAP3 Switzerland
1650619,14436,,,847,"Zanetti, M.",Springer/SISSA,Search for W′ → tb in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2283,0.0004380201489268506,,,nan,,NOT SCOAP3 Switzerland
1650620,14436,,,880,"Fedi, G.",Springer/SISSA,Search for W′ → tb in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2283,0.0004380201489268506,,,nan,,NOT SCOAP3 Switzerland
1678222,13641,,,726,,Institute of Physics Publishing/Chinese Academy of Sciences,"Study of the production of and hadrons in pp collisions and first measurement of the branching fractionSupported by CERN and national agencies: CAPES, CNPq, FAPERJ and FINEP (Brazil); NSFC (China); CNRS/IN2P3 (France); BMBF, DFG, HGF and MPG (Germany); INFN (Italy); FOM and NWO (The Netherlands); MNiSW and NCN (Poland); MEN/IFA (Romania); MinES and FANO (Russia); MinECo (Spain); SNSF and SER (Switzerland); NASU (Ukraine); STFC (United Kingdom); NSF (USA). The Tier1 computing centres are supported by IN2P3 (France), KIT and BMBF (Germany), INFN (Italy), NWO and SURF (The Netherlands), PIC (Spain), GridPP (United Kingdom). Individual groups or members have received support from EPLANET, Marie Skłodowska-Curie Actions and ERC (European Union), Conseil général de Haute-Savoie, Labex ENIGMASS and OCEVU, Région Auvergne (France), RFBR (Russia), XuntaGal and GENCAT (Spain), Royal Society and Royal Commission for the Exhibition of 1851 (United Kingdom).",727,0.001375515818431912,,,nan,,NOT SCOAP3 Switzerland
1680798,13697,,,178,"Romero Abad, D.",Springer/SISSA,Search for the production of an excited bottom quark decaying to tW in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2318,0.0004314063848144953,,,nan,,NOT SCOAP3 Switzerland
1680799,13697,,,179,"Ruiz Vargas, J.",Springer/SISSA,Search for the production of an excited bottom quark decaying to tW in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2318,0.0004314063848144953,,,nan,,NOT SCOAP3 Switzerland
1680800,13697,,,804,"Brianza, L.",Springer/SISSA,Search for the production of an excited bottom quark decaying to tW in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2318,0.0004314063848144953,,,nan,,NOT SCOAP3 Switzerland
1680801,13697,,,833,"Thyssen, F.",Springer/SISSA,Search for the production of an excited bottom quark decaying to tW in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2318,0.0004314063848144953,,,nan,,NOT SCOAP3 Switzerland
1680802,13697,,,859,"Zanetti, M.",Springer/SISSA,Search for the production of an excited bottom quark decaying to tW in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2318,0.0004314063848144953,,,nan,,NOT SCOAP3 Switzerland
1680803,13697,,,893,"Fedi, G.",Springer/SISSA,Search for the production of an excited bottom quark decaying to tW in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2318,0.0004314063848144953,,,nan,,NOT SCOAP3 Switzerland
1691004,13501,,,175,"Romero Abad, D.",Springer/SISSA,Observation of top quark pairs produced in association with a vector boson in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2307,0.00043346337234503684,,,nan,,NOT SCOAP3 Switzerland
1691005,13501,,,176,"Ruiz Vargas, J.",Springer/SISSA,Observation of top quark pairs produced in association with a vector boson in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2307,0.00043346337234503684,,,nan,,NOT SCOAP3 Switzerland
1691006,13501,,,800,"Brianza, L.",Springer/SISSA,Observation of top quark pairs produced in association with a vector boson in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2307,0.00043346337234503684,,,nan,,NOT SCOAP3 Switzerland
1691007,13501,,,829,"Thyssen, F.",Springer/SISSA,Observation of top quark pairs produced in association with a vector boson in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2307,0.00043346337234503684,,,nan,,NOT SCOAP3 Switzerland
1691008,13501,,,855,"Zanetti, M.",Springer/SISSA,Observation of top quark pairs produced in association with a vector boson in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2307,0.00043346337234503684,,,nan,,NOT SCOAP3 Switzerland
1691009,13501,,,889,"Fedi, G.",Springer/SISSA,Observation of top quark pairs produced in association with a vector boson in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2307,0.00043346337234503684,,,nan,,NOT SCOAP3 Switzerland
1699100,13448,,,175,"Romero Abad, D.",Springer/SISSA,Search for a very light NMSSM Higgs boson produced in decays of the 125 GeV scalar boson and decaying into τ leptons in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2309,0.00043308791684711995,,,nan,,NOT SCOAP3 Switzerland
1699101,13448,,,176,"Ruiz Vargas, J.",Springer/SISSA,Search for a very light NMSSM Higgs boson produced in decays of the 125 GeV scalar boson and decaying into τ leptons in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2309,0.00043308791684711995,,,nan,,NOT SCOAP3 Switzerland
1699102,13448,,,799,"Brianza, L.",Springer/SISSA,Search for a very light NMSSM Higgs boson produced in decays of the 125 GeV scalar boson and decaying into τ leptons in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2309,0.00043308791684711995,,,nan,,NOT SCOAP3 Switzerland
1699103,13448,,,828,"Thyssen, F.",Springer/SISSA,Search for a very light NMSSM Higgs boson produced in decays of the 125 GeV scalar boson and decaying into τ leptons in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2309,0.00043308791684711995,,,nan,,NOT SCOAP3 Switzerland
1699104,13448,,,854,"Zanetti, M.",Springer/SISSA,Search for a very light NMSSM Higgs boson produced in decays of the 125 GeV scalar boson and decaying into τ leptons in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2309,0.00043308791684711995,,,nan,,NOT SCOAP3 Switzerland
1699105,13448,,,888,"Fedi, G.",Springer/SISSA,Search for a very light NMSSM Higgs boson produced in decays of the 125 GeV scalar boson and decaying into τ leptons in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV,2309,0.00043308791684711995,,,nan,,NOT SCOAP3 Switzerland
1726291,13350,,,174,"Romero Abad, D.",Springer/SISSA,Measurement of transverse momentum relative to dijet systems in PbPb and pp collisions at s N N = 2.76 $$ \sqrt{s_{\mathrm{NN}}}=2.76 $$ TeV,2302,0.0004344048653344917,,,nan,,NOT SCOAP3 Switzerland
1726292,13350,,,175,"Ruiz Vargas, J.",Springer/SISSA,Measurement of transverse momentum relative to dijet systems in PbPb and pp collisions at s N N = 2.76 $$ \sqrt{s_{\mathrm{NN}}}=2.76 $$ TeV,2302,0.0004344048653344917,,,nan,,NOT SCOAP3 Switzerland
1726293,13350,,,802,"Brianza, L.",Springer/SISSA,Measurement of transverse momentum relative to dijet systems in PbPb and pp collisions at s N N = 2.76 $$ \sqrt{s_{\mathrm{NN}}}=2.76 $$ TeV,2302,0.0004344048653344917,,,nan,,NOT SCOAP3 Switzerland
1726294,13350,,,831,"Thyssen, F.",Springer/SISSA,Measurement of transverse momentum relative to dijet systems in PbPb and pp collisions at s N N = 2.76 $$ \sqrt{s_{\mathrm{NN}}}=2.76 $$ TeV,2302,0.0004344048653344917,,,nan,,NOT SCOAP3 Switzerland
1726295,13350,,,858,"Zanetti, M.",Springer/SISSA,Measurement of transverse momentum relative to dijet systems in PbPb and pp collisions at s N N = 2.76 $$ \sqrt{s_{\mathrm{NN}}}=2.76 $$ TeV,2302,0.0004344048653344917,,,nan,,NOT SCOAP3 Switzerland
1726296,13350,,,889,"Fedi, G.",Springer/SISSA,Measurement of transverse momentum relative to dijet systems in PbPb and pp collisions at s N N = 2.76 $$ \sqrt{s_{\mathrm{NN}}}=2.76 $$ TeV,2302,0.0004344048653344917,,,nan,,NOT SCOAP3 Switzerland
