Fully electron-transferred donor/acceptor layered frameworks with TCNQ(2-)
In a series of two-dimensional layered frameworks constructed by two electron-donor (D) and one electron-acceptor (A) units (a D2A framework), two-electron transferred systems with D(+)2A(2-) were first synthesized as [{Ru2(R-PhCO2)4}2(TCNQRx)]·n(solv) (R = o-CF3, Rx = H2 (1), R = o-CF3, Rx = Me2 (2...
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Veröffentlicht in: | Inorganic chemistry 2015-02, Vol.54 (4), p.1518-1527 |
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description | In a series of two-dimensional layered frameworks constructed by two electron-donor (D) and one electron-acceptor (A) units (a D2A framework), two-electron transferred systems with D(+)2A(2-) were first synthesized as [{Ru2(R-PhCO2)4}2(TCNQRx)]·n(solv) (R = o-CF3, Rx = H2 (1), R = o-CF3, Rx = Me2 (2), R = o-CF3, Rx = F4 (3), R = o-Me, TCNQRx = BTDA-TCNQ (4), R = p-Me, TCNQRx = BTDA-TCNQ (5), where TCNQ is 7,7,8,8-tetracyano-p-quinodimethane and BTDA-TCNQ is bis[1,2,5]dithiazolotetracyanoquinodimethane). The D(+)2A(2-) system was synthesized by assembling D/A combinations of paddlewheel-type [Ru2(II,II)(R-PhCO2)4] complexes and TCNQRx that possibly caused a large gap between the HOMO of D and the LUMO of A (ΔEH-L(DA)). All compounds were paramagnetic because of quasi-isolated [Ru2(II,III)](+) units with weakly antiferromagnetically coupled S = 3/2 spins via diamagnetic TCNQRx(2-) and/or through the interlayer space. The ionic states of these compounds were determined using the HOMO/LUMO energies and redox potentials of the D and A components in the ionization diagram for ΔEH-L(DA) vs ΔE1/2(DA) (= E1/2(D) - E1/2(A); E1/2 = first redox potential) as well as by previously reported data for the D2A and DA series of [Ru2]/TCNQ, DCNQI materials. The boundary between the one-electron and the two-electron transferred ionic regimes (1e-I and 2e-I, respectively) was not characterized. Therefore, another diagram for ΔEH-L(DA) vs |(2)E1/2(A) - (1)E1/2(A)|, where (2)E1/2(A) and (1)E1/2(A) are the second and first redox potentials of TCNQRx, respectively, was used because the 2e-I regime is dependent on on-site Coulomb repulsion (U = |(2)E1/2(A) - (1)E1/2(A)|) of TCNQRx. This explained the oxidation states of 1-5 and the relationship between ΔEH-L(DA) and U and allowed us to determine whether the ionic regime was 1e-I or 2e-I. These diagrams confirm that a charge-oriented choice of building units is possible even when designing covalently bonded D2A framework systems. |
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The D(+)2A(2-) system was synthesized by assembling D/A combinations of paddlewheel-type [Ru2(II,II)(R-PhCO2)4] complexes and TCNQRx that possibly caused a large gap between the HOMO of D and the LUMO of A (ΔEH-L(DA)). All compounds were paramagnetic because of quasi-isolated [Ru2(II,III)](+) units with weakly antiferromagnetically coupled S = 3/2 spins via diamagnetic TCNQRx(2-) and/or through the interlayer space. The ionic states of these compounds were determined using the HOMO/LUMO energies and redox potentials of the D and A components in the ionization diagram for ΔEH-L(DA) vs ΔE1/2(DA) (= E1/2(D) - E1/2(A); E1/2 = first redox potential) as well as by previously reported data for the D2A and DA series of [Ru2]/TCNQ, DCNQI materials. The boundary between the one-electron and the two-electron transferred ionic regimes (1e-I and 2e-I, respectively) was not characterized. Therefore, another diagram for ΔEH-L(DA) vs |(2)E1/2(A) - (1)E1/2(A)|, where (2)E1/2(A) and (1)E1/2(A) are the second and first redox potentials of TCNQRx, respectively, was used because the 2e-I regime is dependent on on-site Coulomb repulsion (U = |(2)E1/2(A) - (1)E1/2(A)|) of TCNQRx. This explained the oxidation states of 1-5 and the relationship between ΔEH-L(DA) and U and allowed us to determine whether the ionic regime was 1e-I or 2e-I. These diagrams confirm that a charge-oriented choice of building units is possible even when designing covalently bonded D2A framework systems.</description><identifier>EISSN: 1520-510X</identifier><identifier>DOI: 10.1021/ic502513p</identifier><identifier>PMID: 25629292</identifier><language>eng</language><publisher>United States</publisher><ispartof>Inorganic chemistry, 2015-02, Vol.54 (4), p.1518-1527</ispartof><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,776,780,27901,27902</link.rule.ids><backlink>$$Uhttps://www.ncbi.nlm.nih.gov/pubmed/25629292$$D View this record in MEDLINE/PubMed$$Hfree_for_read</backlink></links><search><creatorcontrib>Kosaka, Wataru</creatorcontrib><creatorcontrib>Morita, Takaumi</creatorcontrib><creatorcontrib>Yokoyama, Taiga</creatorcontrib><creatorcontrib>Zhang, Jun</creatorcontrib><creatorcontrib>Miyasaka, Hitoshi</creatorcontrib><title>Fully electron-transferred donor/acceptor layered frameworks with TCNQ(2-)</title><title>Inorganic chemistry</title><addtitle>Inorg Chem</addtitle><description>In a series of two-dimensional layered frameworks constructed by two electron-donor (D) and one electron-acceptor (A) units (a D2A framework), two-electron transferred systems with D(+)2A(2-) were first synthesized as [{Ru2(R-PhCO2)4}2(TCNQRx)]·n(solv) (R = o-CF3, Rx = H2 (1), R = o-CF3, Rx = Me2 (2), R = o-CF3, Rx = F4 (3), R = o-Me, TCNQRx = BTDA-TCNQ (4), R = p-Me, TCNQRx = BTDA-TCNQ (5), where TCNQ is 7,7,8,8-tetracyano-p-quinodimethane and BTDA-TCNQ is bis[1,2,5]dithiazolotetracyanoquinodimethane). The D(+)2A(2-) system was synthesized by assembling D/A combinations of paddlewheel-type [Ru2(II,II)(R-PhCO2)4] complexes and TCNQRx that possibly caused a large gap between the HOMO of D and the LUMO of A (ΔEH-L(DA)). All compounds were paramagnetic because of quasi-isolated [Ru2(II,III)](+) units with weakly antiferromagnetically coupled S = 3/2 spins via diamagnetic TCNQRx(2-) and/or through the interlayer space. The ionic states of these compounds were determined using the HOMO/LUMO energies and redox potentials of the D and A components in the ionization diagram for ΔEH-L(DA) vs ΔE1/2(DA) (= E1/2(D) - E1/2(A); E1/2 = first redox potential) as well as by previously reported data for the D2A and DA series of [Ru2]/TCNQ, DCNQI materials. The boundary between the one-electron and the two-electron transferred ionic regimes (1e-I and 2e-I, respectively) was not characterized. Therefore, another diagram for ΔEH-L(DA) vs |(2)E1/2(A) - (1)E1/2(A)|, where (2)E1/2(A) and (1)E1/2(A) are the second and first redox potentials of TCNQRx, respectively, was used because the 2e-I regime is dependent on on-site Coulomb repulsion (U = |(2)E1/2(A) - (1)E1/2(A)|) of TCNQRx. This explained the oxidation states of 1-5 and the relationship between ΔEH-L(DA) and U and allowed us to determine whether the ionic regime was 1e-I or 2e-I. These diagrams confirm that a charge-oriented choice of building units is possible even when designing covalently bonded D2A framework systems.</description><issn>1520-510X</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2015</creationdate><recordtype>article</recordtype><recordid>eNo1j01Lw0AYhBdBbK0e_AOSYz3E7neSoxTrB0URcvAW3uy-wegmG3cTSv-9FStzGBieGRhCrhi9ZZSzVWsU5YqJ4YTMmeI0VYy-z8h5jJ-U0kJIfUZmXGleHDQnz5vJuX2CDs0YfJ-OAfrYYAhoE-t7H1ZgDA6jD4mDPf7GTYAOdz58xWTXjh9JuX55W_L05oKcNuAiXh59QcrNfbl-TLevD0_ru206cMbGFGUjjcwZ5Eih1kBNlqksKzgv8lraXAkDBdS8YEAFz0wtrJAGwB5aNs_Fgiz_ZofgvyeMY9W10aBz0KOfYsW00lRqnakDen1Ep7pDWw2h7SDsq__74geExFle</recordid><startdate>20150216</startdate><enddate>20150216</enddate><creator>Kosaka, Wataru</creator><creator>Morita, Takaumi</creator><creator>Yokoyama, Taiga</creator><creator>Zhang, Jun</creator><creator>Miyasaka, Hitoshi</creator><scope>NPM</scope><scope>7X8</scope></search><sort><creationdate>20150216</creationdate><title>Fully electron-transferred donor/acceptor layered frameworks with TCNQ(2-)</title><author>Kosaka, Wataru ; Morita, Takaumi ; Yokoyama, Taiga ; Zhang, Jun ; Miyasaka, Hitoshi</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-p211t-e4f4c481a8e0ab6a0c7757792298b4d853ca9ab291a0327cb3d34caad4c4d883</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2015</creationdate><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Kosaka, Wataru</creatorcontrib><creatorcontrib>Morita, Takaumi</creatorcontrib><creatorcontrib>Yokoyama, Taiga</creatorcontrib><creatorcontrib>Zhang, Jun</creatorcontrib><creatorcontrib>Miyasaka, Hitoshi</creatorcontrib><collection>PubMed</collection><collection>MEDLINE - Academic</collection><jtitle>Inorganic chemistry</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Kosaka, Wataru</au><au>Morita, Takaumi</au><au>Yokoyama, Taiga</au><au>Zhang, Jun</au><au>Miyasaka, Hitoshi</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Fully electron-transferred donor/acceptor layered frameworks with TCNQ(2-)</atitle><jtitle>Inorganic chemistry</jtitle><addtitle>Inorg Chem</addtitle><date>2015-02-16</date><risdate>2015</risdate><volume>54</volume><issue>4</issue><spage>1518</spage><epage>1527</epage><pages>1518-1527</pages><eissn>1520-510X</eissn><abstract>In a series of two-dimensional layered frameworks constructed by two electron-donor (D) and one electron-acceptor (A) units (a D2A framework), two-electron transferred systems with D(+)2A(2-) were first synthesized as [{Ru2(R-PhCO2)4}2(TCNQRx)]·n(solv) (R = o-CF3, Rx = H2 (1), R = o-CF3, Rx = Me2 (2), R = o-CF3, Rx = F4 (3), R = o-Me, TCNQRx = BTDA-TCNQ (4), R = p-Me, TCNQRx = BTDA-TCNQ (5), where TCNQ is 7,7,8,8-tetracyano-p-quinodimethane and BTDA-TCNQ is bis[1,2,5]dithiazolotetracyanoquinodimethane). The D(+)2A(2-) system was synthesized by assembling D/A combinations of paddlewheel-type [Ru2(II,II)(R-PhCO2)4] complexes and TCNQRx that possibly caused a large gap between the HOMO of D and the LUMO of A (ΔEH-L(DA)). All compounds were paramagnetic because of quasi-isolated [Ru2(II,III)](+) units with weakly antiferromagnetically coupled S = 3/2 spins via diamagnetic TCNQRx(2-) and/or through the interlayer space. The ionic states of these compounds were determined using the HOMO/LUMO energies and redox potentials of the D and A components in the ionization diagram for ΔEH-L(DA) vs ΔE1/2(DA) (= E1/2(D) - E1/2(A); E1/2 = first redox potential) as well as by previously reported data for the D2A and DA series of [Ru2]/TCNQ, DCNQI materials. The boundary between the one-electron and the two-electron transferred ionic regimes (1e-I and 2e-I, respectively) was not characterized. Therefore, another diagram for ΔEH-L(DA) vs |(2)E1/2(A) - (1)E1/2(A)|, where (2)E1/2(A) and (1)E1/2(A) are the second and first redox potentials of TCNQRx, respectively, was used because the 2e-I regime is dependent on on-site Coulomb repulsion (U = |(2)E1/2(A) - (1)E1/2(A)|) of TCNQRx. This explained the oxidation states of 1-5 and the relationship between ΔEH-L(DA) and U and allowed us to determine whether the ionic regime was 1e-I or 2e-I. These diagrams confirm that a charge-oriented choice of building units is possible even when designing covalently bonded D2A framework systems.</abstract><cop>United States</cop><pmid>25629292</pmid><doi>10.1021/ic502513p</doi><tpages>10</tpages></addata></record> |
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title | Fully electron-transferred donor/acceptor layered frameworks with TCNQ(2-) |
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