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<refs>
  <reqdate>2013-06-20</reqdate>
  <reqtime>13:58:36</reqtime>
  <query><![CDATA[SELECT * FROM refs WHERE grp like "%H%" AND ((refid=173)OR(refid=172)) ORDER BY pubyear DESC, refid DESC ;]]></query>
  <ref>
    <refid>173</refid>
    <title><![CDATA[The [Fe(etz)<sub>6</sub>](BF<sub>4</sub>)<sub>2</sub> Spin-Crossover System - Part Two: Hysteresis in the LIESST Regime]]></title>
    <authors>R. Hinek, H. Spiering, P. Gütlich, A. Hauser</authors>
    <author_list>
      <author>Hinek, R.</author>
      <author>Spiering, H.</author>
      <author>Gütlich, P.</author>
      <author>Hauser, A.</author>
    </author_list>
    <journal>Chemistry - A European Journal</journal>
    <journal_abbr>Chem. - Eur. J.</journal_abbr>
    <issn>0947-6539</issn>
    <pubyear>1996</pubyear>
    <vol>2</vol>
    <no>11</no>
    <ppsta>1435</ppsta>
    <ppend>1439</ppend>
    <grp>H</grp>
    <keywords>hysteresis; iron complexes; LIESST; spin crossover; tetrazoles</keywords>
    <keyword_list>
      <keyword>hysteresis</keyword>
      <keyword>iron complexes</keyword>
      <keyword>LIESST</keyword>
      <keyword>spin crossover</keyword>
      <keyword>tetrazoles</keyword>
    </keyword_list>
    <abs_url>http://www3.interscience.wiley.com/journal/112298255/abstract</abs_url>
    <pdf_url>http://www3.interscience.wiley.com/cgi-bin/fulltext/112298255/PDFSTART</pdf_url>
    <abstract><![CDATA[<p>In the [Fe(etz)<sub>6</sub>](BF<sub>4</sub>)<sub>2</sub> spincrossover system the iron(II) complexes occupy two nonequivalent lattice sites, sites A and B. Complexes on site A show a thermal high-spin (HS) &rarr; low-spin (LS) transition at 105 K, whereas complexes on site B remain in the HS state down to 10 K. Complexes on both sites exhibit light-induced spin state conversions (LIESST) at 20 K: LS &rarr; HS on site A with &lambda; = 514.5 nm, and HS &rarr; LS on site B with &lambda; = 820 nm. The relaxation processes subsequent to the HS &rarr; LS conversion on site B reveal a light-induced HS&rarr;LS bistability for the complexes on site B at 70 K. The bistability as well as the absence of a thermal spin transition on site B are attributed to a thermal hysteresis for the B-site complexes with a critical temperature T<sup>&uarr;</sup><sub>c </sub>K on heating. This hysteresis can be interpreted in terms of strong cooperative effects of elastic origin, which, in addition, cause characteristic deviations of the relaxation on site B from first-order kinetics (self-acceleration). In contrast, the HS &rarr; LS relaxation at 60 K on site A after irradiation with &lambda; = 514.5 nm shows an unusual self-retardation.</p>]]></abstract>
    <doi>10.1002/chem.19960021116</doi>
    <unige>2977</unige>
  </ref>
  <ref>
    <refid>172</refid>
    <title><![CDATA[The [Fe(etz)<sub>6</sub>](BF<sub>4</sub>)<sub>2</sub> Spin-Crossover System - Part One: HS-LS Transition on Two Lattice Sites]]></title>
    <authors>R. Hinek, H. Spiering, D. Schollmeyer, P. Gütlich, A. Hauser</authors>
    <author_list>
      <author>Hinek, R.</author>
      <author>Spiering, H.</author>
      <author>Schollmeyer, D.</author>
      <author>Gütlich, P.</author>
      <author>Hauser, A.</author>
    </author_list>
    <journal>Chemistry - A European Journal</journal>
    <journal_abbr>Chem. - Eur. J.</journal_abbr>
    <issn>0947-6539</issn>
    <pubyear>1996</pubyear>
    <vol>2</vol>
    <no>11</no>
    <ppsta>1427</ppsta>
    <ppend>1434</ppend>
    <grp>H</grp>
    <keywords>iron complexes; LIESST; spin crossover; tetrazoles</keywords>
    <keyword_list>
      <keyword>iron complexes</keyword>
      <keyword>LIESST</keyword>
      <keyword>spin crossover</keyword>
      <keyword>tetrazoles</keyword>
    </keyword_list>
    <abs_url>http://www3.interscience.wiley.com/journal/112298254/abstract</abs_url>
    <pdf_url>http://www3.interscience.wiley.com/cgi-bin/fulltext/112298254/PDFSTART</pdf_url>
    <abstract><![CDATA[<p>The [Fe(etz),](BF,), spin-cross-over system (etz = 1-ethyl-1 <sub>H</sub>-tetrazole) crystallizes in space group P<em>1</em>, with the following lattice constants at 298 K: <em>a</em>10.419(3), b=15.709(1), c = 18.890(2) Ċ, &alpha; = 71.223(9), &beta; =77.986(10), and &gamma; = 84.62(1)° V = 2862.0(9) Ċ<sup>3</sup> and <em>Z</em> = 3. Two nonequivalent lattice sites, one without (site A) and one with (site B) inversion symmetry, are observed. The population of the two sites <em>n</em><sub>A</sub>:<em>n</em><sub>B</sub> is 2:l. Iron(II) on site A undergoes a thermal low-spin (LS) &rarr; high-spin (HS) transition with T<sub>1/2</sub>I, = 105 K. whereas that on site B remains in the high-spin state down to cryogenic temperatures. Application of external pressure of up to 1200 bar between 200 and 60 K does not cause formation of the low-spin state on site B. On site A the high-spin state can be populated as a metastable state at 20 K by irradiating the sample with &lambda; = 514.5 nm; on site B a light-induced population of the low-spin state can be achieved with &lambda; = 820 nm.</p>]]></abstract>
    <doi>10.1002/chem.19960021115</doi>
    <unige>2978</unige>
  </ref>
</refs>
