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Isostructural Bisdithiazolyl and Bisthiaselenazolyl Radicals: Trends in Bandwidth and Conductivity
Reaction of N-alkylated pyridine-bridged bisdithiazolylium cations [1]+ (R1 = Me, Et; R2 = Ph) with selenium dioxide in acetic acid provides a one-step high-yield synthetic route to bisthiaselenazolylium cations [2]+ (R1 = Me, Et; R2 = Ph). The corresponding radicals 1 and 2 can be prepared by chemi...
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Published in: | Inorganic chemistry 2006-12, Vol.45 (26), p.10958-10966 |
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container_title | Inorganic chemistry |
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creator | Brusso, Jaclyn L Derakhshan, Shahab Itkis, Mikhail E Kleinke, Holger Haddon, Robert C Oakley, Richard T Reed, Robert W Richardson, John F Robertson, Craig M Thompson, Laurence K |
description | Reaction of N-alkylated pyridine-bridged bisdithiazolylium cations [1]+ (R1 = Me, Et; R2 = Ph) with selenium dioxide in acetic acid provides a one-step high-yield synthetic route to bisthiaselenazolylium cations [2]+ (R1 = Me, Et; R2 = Ph). The corresponding radicals 1 and 2 can be prepared by chemical or electrochemical reduction of the cations. Structural analysis of the radicals has been achieved by a combination of single-crystal and powder X-ray diffraction methods. While the two sulfur radicals 1 adopt different space groups (P3121 for R1 = Me and P1̄ for R1 = Et), the two selenium radicals 2 (space groups P3121 for R1 = Me and P3221 for R1 = Et) are isostructural with each other and also with 1 (R1 = Me, R2 = Ph). Variable-temperature magnetic measurements on all four compounds confirm that they are undimerized S = 1/2 systems, with varying degrees of weak intermolecular antiferromagnetic coupling. Variable-temperature electrical conductivity measurements on the two selenium radicals provide conductivities σ(300 K) = 7.4 × 10-6 (R1 = Et) and 3.3 × 10-5 S cm-1 (R1 = Me), with activation energies, E act, of 0.32 (R1 = Et) and 0.29 eV (R1 = Me). The differences in conductivity within the isostructural series is interpreted in terms of their relative solid-state bandwidths, as estimated from Extended Hückel band-structure calculations. |
doi_str_mv | 10.1021/ic061687c |
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The corresponding radicals 1 and 2 can be prepared by chemical or electrochemical reduction of the cations. Structural analysis of the radicals has been achieved by a combination of single-crystal and powder X-ray diffraction methods. While the two sulfur radicals 1 adopt different space groups (P3121 for R1 = Me and P1̄ for R1 = Et), the two selenium radicals 2 (space groups P3121 for R1 = Me and P3221 for R1 = Et) are isostructural with each other and also with 1 (R1 = Me, R2 = Ph). Variable-temperature magnetic measurements on all four compounds confirm that they are undimerized S = 1/2 systems, with varying degrees of weak intermolecular antiferromagnetic coupling. Variable-temperature electrical conductivity measurements on the two selenium radicals provide conductivities σ(300 K) = 7.4 × 10-6 (R1 = Et) and 3.3 × 10-5 S cm-1 (R1 = Me), with activation energies, E act, of 0.32 (R1 = Et) and 0.29 eV (R1 = Me). 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Chem</addtitle><description>Reaction of N-alkylated pyridine-bridged bisdithiazolylium cations [1]+ (R1 = Me, Et; R2 = Ph) with selenium dioxide in acetic acid provides a one-step high-yield synthetic route to bisthiaselenazolylium cations [2]+ (R1 = Me, Et; R2 = Ph). The corresponding radicals 1 and 2 can be prepared by chemical or electrochemical reduction of the cations. Structural analysis of the radicals has been achieved by a combination of single-crystal and powder X-ray diffraction methods. While the two sulfur radicals 1 adopt different space groups (P3121 for R1 = Me and P1̄ for R1 = Et), the two selenium radicals 2 (space groups P3121 for R1 = Me and P3221 for R1 = Et) are isostructural with each other and also with 1 (R1 = Me, R2 = Ph). Variable-temperature magnetic measurements on all four compounds confirm that they are undimerized S = 1/2 systems, with varying degrees of weak intermolecular antiferromagnetic coupling. Variable-temperature electrical conductivity measurements on the two selenium radicals provide conductivities σ(300 K) = 7.4 × 10-6 (R1 = Et) and 3.3 × 10-5 S cm-1 (R1 = Me), with activation energies, E act, of 0.32 (R1 = Et) and 0.29 eV (R1 = Me). The differences in conductivity within the isostructural series is interpreted in terms of their relative solid-state bandwidths, as estimated from Extended Hückel band-structure calculations.</description><issn>0020-1669</issn><issn>1520-510X</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2006</creationdate><recordtype>article</recordtype><recordid>eNptkLtOwzAUhi0EouUy8AIoC0gMATvxJWGDcqtUcS2CzXLjU9WQJsVOgDKx8po8CQ6tysLko_98_i1_CG0RvE9wRA5MhjnhiciWUJuwCIeM4Mdl1MbYz4TztIXWnHvCGKcx5auoRQQRMWWsjaDrSlfZOqtqq_Lg2DhtqpFRH2U-zQNV6CZqAgc5FPP4VmmTqdwdfn9-BX0LhXaBKYJjj78ZXY1-73XKQvta82qq6QZaGXoeNufnOro_O-13LsLe1Xm3c9QLFSWiCtN4QKJ4wIUinGI2TDPqv0OEEljAIGUURCKACsEAOOc6wUnKgKooSjVRaRSvo91Z78SWLzW4So6NyyDPVQFl7SRPIkYj1oB7MzCzpXMWhnJizVjZqSRYNk7lwqlnt-el9WAM-o-cS_RAOAO8KXhf7JV9llzEgsn-9Z28vHkQSe_xXJ54fmfGq8zJp7K2hXfyz8M_fSWOGA</recordid><startdate>20061225</startdate><enddate>20061225</enddate><creator>Brusso, Jaclyn L</creator><creator>Derakhshan, Shahab</creator><creator>Itkis, Mikhail E</creator><creator>Kleinke, Holger</creator><creator>Haddon, Robert C</creator><creator>Oakley, Richard T</creator><creator>Reed, Robert W</creator><creator>Richardson, John F</creator><creator>Robertson, Craig M</creator><creator>Thompson, Laurence K</creator><general>American Chemical Society</general><scope>BSCLL</scope><scope>NPM</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7X8</scope></search><sort><creationdate>20061225</creationdate><title>Isostructural Bisdithiazolyl and Bisthiaselenazolyl Radicals: Trends in Bandwidth and Conductivity</title><author>Brusso, Jaclyn L ; Derakhshan, Shahab ; Itkis, Mikhail E ; Kleinke, Holger ; Haddon, Robert C ; Oakley, Richard T ; Reed, Robert W ; Richardson, John F ; Robertson, Craig M ; Thompson, Laurence K</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-a417t-93b123b67a16405f9c415217a707eb954e787e4775ee666d80895e4a229d1a923</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2006</creationdate><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Brusso, Jaclyn L</creatorcontrib><creatorcontrib>Derakhshan, Shahab</creatorcontrib><creatorcontrib>Itkis, Mikhail E</creatorcontrib><creatorcontrib>Kleinke, Holger</creatorcontrib><creatorcontrib>Haddon, Robert C</creatorcontrib><creatorcontrib>Oakley, Richard T</creatorcontrib><creatorcontrib>Reed, Robert W</creatorcontrib><creatorcontrib>Richardson, John F</creatorcontrib><creatorcontrib>Robertson, Craig M</creatorcontrib><creatorcontrib>Thompson, Laurence K</creatorcontrib><collection>Istex</collection><collection>PubMed</collection><collection>CrossRef</collection><collection>MEDLINE - Academic</collection><jtitle>Inorganic chemistry</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Brusso, Jaclyn L</au><au>Derakhshan, Shahab</au><au>Itkis, Mikhail E</au><au>Kleinke, Holger</au><au>Haddon, Robert C</au><au>Oakley, Richard T</au><au>Reed, Robert W</au><au>Richardson, John F</au><au>Robertson, Craig M</au><au>Thompson, Laurence K</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Isostructural Bisdithiazolyl and Bisthiaselenazolyl Radicals: Trends in Bandwidth and Conductivity</atitle><jtitle>Inorganic chemistry</jtitle><addtitle>Inorg. Chem</addtitle><date>2006-12-25</date><risdate>2006</risdate><volume>45</volume><issue>26</issue><spage>10958</spage><epage>10966</epage><pages>10958-10966</pages><issn>0020-1669</issn><eissn>1520-510X</eissn><abstract>Reaction of N-alkylated pyridine-bridged bisdithiazolylium cations [1]+ (R1 = Me, Et; R2 = Ph) with selenium dioxide in acetic acid provides a one-step high-yield synthetic route to bisthiaselenazolylium cations [2]+ (R1 = Me, Et; R2 = Ph). The corresponding radicals 1 and 2 can be prepared by chemical or electrochemical reduction of the cations. Structural analysis of the radicals has been achieved by a combination of single-crystal and powder X-ray diffraction methods. While the two sulfur radicals 1 adopt different space groups (P3121 for R1 = Me and P1̄ for R1 = Et), the two selenium radicals 2 (space groups P3121 for R1 = Me and P3221 for R1 = Et) are isostructural with each other and also with 1 (R1 = Me, R2 = Ph). Variable-temperature magnetic measurements on all four compounds confirm that they are undimerized S = 1/2 systems, with varying degrees of weak intermolecular antiferromagnetic coupling. Variable-temperature electrical conductivity measurements on the two selenium radicals provide conductivities σ(300 K) = 7.4 × 10-6 (R1 = Et) and 3.3 × 10-5 S cm-1 (R1 = Me), with activation energies, E act, of 0.32 (R1 = Et) and 0.29 eV (R1 = Me). The differences in conductivity within the isostructural series is interpreted in terms of their relative solid-state bandwidths, as estimated from Extended Hückel band-structure calculations.</abstract><cop>United States</cop><pub>American Chemical Society</pub><pmid>17173455</pmid><doi>10.1021/ic061687c</doi><tpages>9</tpages></addata></record> |
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title | Isostructural Bisdithiazolyl and Bisthiaselenazolyl Radicals: Trends in Bandwidth and Conductivity |
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