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<refs>
  <reqdate>2013-05-20</reqdate>
  <reqtime>02:23:40</reqtime>
  <query><![CDATA[SELECT * FROM refs WHERE grp like "%H%" AND ((refid=639)OR(refid=1193)) ORDER BY pubyear DESC, refid DESC ;]]></query>
  <ref>
    <refid>1193</refid>
    <title><![CDATA[Effect of External Pressure on the Excitation Energy Transfer from [Cr(ox)3]<sup>3-</sup> to [Cr(bpy)3]<sup>3+</sup> in [Rh<sub>1-x</sub>Cr<sub>x</sub>(bpy)<sub>3</sub>][NaM<sub>1-y</sub>Cr<sub>y</sub>(ox)<sub>3</sub>]ClO<sub>4</sub>]]></title>
    <authors>Mia Milos, Prodipta Pal, and Andreas Hauser</authors>
    <author_list>
      <author>Milos, Mia</author>
      <author>Pal, Prodipta</author>
      <author>Hauser, Andreas</author>
    </author_list>
    <journal>ChemPhysChem</journal>
    <journal_abbr>ChemPhysChem</journal_abbr>
    <issn>1439-4235</issn>
    <pubyear>2010</pubyear>
    <vol>11</vol>
    <no>14</no>
    <ppsta>3161</ppsta>
    <ppend>3166</ppend>
    <grp>H</grp>
    <keywords><![CDATA[[Cr(bpy)3]3+; [Cr(ox)3]3&#8722;; 3D oxalate networks; excitation energy transfer; high pressures]]></keywords>
    <keyword_list>
      <keyword>[Cr(bpy)3]3+</keyword>
      <keyword>[Cr(ox)3]3&#8722</keyword>
      <keyword>3D oxalate networks</keyword>
      <keyword>excitation energy transfer</keyword>
      <keyword>high pressures</keyword>
    </keyword_list>
    <abs_url>http://onlinelibrary.wiley.com/doi/10.1002/cphc.201000324/abstract</abs_url>
    <html_url>http://onlinelibrary.wiley.com/doi/10.1002/cphc.201000324/full</html_url>
    <pdf_url>http://onlinelibrary.wiley.com/doi/10.1002/cphc.201000324/pdf</pdf_url>
    <abstract><![CDATA[<p>Resonant excitation energy transfer from [Cr(ox)3]<sup>3- </sup>to [Cr(bpy)3]<sup>3+</sup> in the doped 3D oxalate networks [Rh<sub>1-x</sub>Cr<sub>x</sub>(bpy)<sub>3</sub>][NaM<sup>III</sup><sub>1-y</sub>Cr<sub>y</sub>(ox)<sub>3</sub>]ClO<sub>4</sub> (ox=C<sub>2</sub>O<sub>4</sub><sup>-</sup>, bpy=2,2&rsquo;-bipyridine, M=Al,Rh) is due to two types of interaction, namely super exchange coupling and electric dipole&ndash;dipole interaction. The energy transfer probability for both mechanisms is proportional to the spectral overlap of the <sup>2</sup>E&rarr;<sup>4</sup>A<sub>2 </sub>emission of the [Cr(ox)<sub>3</sub>]<sup>3- </sup>donor and the <sup>4</sup>A<sub>2</sub>&rarr;<sup>2</sup>T<sub>1</sub> absorption of the [Cr(bpy)<sub>3</sub>]<sup>3+</sup> acceptor.The spin-flip transitions of (pseudo-)octahedral Cr<sup>3+</sup> are known to shift to lower energy with increasing pressure. Because the shift rates of the two transitions in question differ, the spectral overlap between the donor emission and the acceptor absorption is a function of applied pressure. For [Rh<sub>1-x</sub>Cr<sub>x</sub>(bpy)<sub>3</sub>][Na-M<sub>1-y</sub>Cr<sub>y</sub>(ox)<sub>3</sub>]ClO<sub>4</sub> the spectral overlap is thus substantially reduced on increasing pressure from 0 to 2.5 GPa. As a result, the energy transfer probability decreases with increasing pressure as evidenced by a decrease in the relative emission intensity from the [Cr(bpy)<sub>3</sub>]<sup>3+</sup> acceptor.</p>]]></abstract>
    <flags>P392</flags>
    <doi>10.1002/cphc.201000324</doi>
    <unige>14715</unige>
    <pdf>http://www.unige.ch/sciences/chifi/publis/refs_pdf/ref01193.pdf</pdf>
  </ref>
  <ref>
    <refid>639</refid>
    <title>Photophysical properties of three-dimensional transition metal tris-oxalate network structures</title>
    <authors>Andreas Hauser, Marianne E. von Arx, Vaughan S. Langford, Sélim Kairouani, Ueli Oetliker, Anne Pillonnet</authors>
    <author_list>
      <author>Hauser, Andreas</author>
      <author>Von Arx, Marianne E.</author>
      <author>Langford, Vaughan S.</author>
      <author>Kairouani, Sélim</author>
      <author>Oetliker, Ueli</author>
      <author>Pillonnet, Anne</author>
    </author_list>
    <journal>Topics in Current Chemistry, Transition Metal and Rare Earth Compounds. Excited States, Transitions, and Interactions, Vol III</journal>
    <journal_abbr>Top. Cur. Chem. , Transition Metal Rare Earth Compd. Excited States, Trans. , Interactions, Vol III</journal_abbr>
    <editor>(ed. H. Yersin), Springer, Berlin</editor>
    <pubyear>2004</pubyear>
    <vol>241</vol>
    <grp>H</grp>
    <keywords><![CDATA[oxalate networks ; [Cr(ox)3]3- ; [Cr(bpy)3]3+ ; 2E state ; resonant energy transfer ; phonon-assisted energy transfer ; Förster transfer ; Exchange interaction]]></keywords>
    <keyword_list>
      <keyword>oxalate networks</keyword>
      <keyword>[Cr(ox)3]3-</keyword>
      <keyword>[Cr(bpy)3]3+</keyword>
      <keyword>2E state</keyword>
      <keyword>resonant energy transfer</keyword>
      <keyword>phonon-assisted energy transfer</keyword>
      <keyword>Förster transfer</keyword>
      <keyword>Exchange interaction</keyword>
    </keyword_list>
    <abstract><![CDATA[<p>Excitation energy transfer processes play an important role in many areas of physics, chemistry and biology. The three-dimensional oxalate networks of composition [MIII(bpy)3][MIMIII(ox)3]ClO4 (bpy=2,2-bipyridine, ox=oxalate, MI=alkali ion) allow for a variety of combinations of different transition metal ions. The combination with chromium(III) on both the tris-bipyridine as well as the tris-oxalate site constitutes a model system in which it is possible to differentiate unambiguously between energy transfer from [Cr(ox)3]3&ndash; to [Cr(bpy)3]3+ due to dipole-dipole interaction on the one hand and exchange interaction on the other hand. Furthermore it is possible to just as unambiguously differentiate between the common temperature dependent phonon-assisted energy migration within the 2E state of [Cr(ox)3]3&ndash;, and a unique resonant process.</p>]]></abstract>
    <doi>10.1007/b96860</doi>
    <unige>3941</unige>
  </ref>
</refs>
