Muoniated radical formation and spin dynamics in molecular magnetic materials with oxalate ligands
The crystal structure of Na 2T 2(ox) 2(H 2O) 2 with T = Ni ( II ) , Co ( II ) , Fe ( II ) , and Mn(II) consists of isostructural compounds with an anionic transition metal oxalate network with a 2-leg ladder topology. We performed zero external field μ SR , longitudinal-field quenching (LFQ) and avo...
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Veröffentlicht in: | Physica. B, Condensed matter Condensed matter, 2006-03, Vol.374, p.325-327 |
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container_title | Physica. B, Condensed matter |
container_volume | 374 |
creator | Mennerich, C. Scheuermann, R. Luetkens, H. Kühne, H. Broekelmann, M. Bosse, A. Litterst, F.J. Price, D.J. Klauss, H.-H. |
description | The crystal structure of Na
2T
2(ox)
2(H
2O)
2 with
T
=
Ni
(
II
)
,
Co
(
II
)
,
Fe
(
II
)
, and Mn(II) consists of isostructural compounds with an anionic transition metal oxalate network with a 2-leg ladder topology. We performed zero external field
μ
SR
, longitudinal-field quenching (LFQ) and avoided level-crossing (ALC) measurements on the Co-compound of this series. The measurements show that a significant fraction of the implanted muons forms a muoniated radical state by muonium addition to the resonant
π
electron system of the
(
COO
)
2
2
-
group. The LFQ measurements reveal electronic spin fluctuation rates of several GHz. For reference, ALC measurements on the nonmagnetic compounds Li
2(ox)
2 and Na
2(ox)
2 were carried out and the muon hyperfine coupling constant were deduced to 115 and 150
MHz, respectively. |
doi_str_mv | 10.1016/j.physb.2005.11.087 |
format | Article |
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2T
2(ox)
2(H
2O)
2 with
T
=
Ni
(
II
)
,
Co
(
II
)
,
Fe
(
II
)
, and Mn(II) consists of isostructural compounds with an anionic transition metal oxalate network with a 2-leg ladder topology. We performed zero external field
μ
SR
, longitudinal-field quenching (LFQ) and avoided level-crossing (ALC) measurements on the Co-compound of this series. The measurements show that a significant fraction of the implanted muons forms a muoniated radical state by muonium addition to the resonant
π
electron system of the
(
COO
)
2
2
-
group. The LFQ measurements reveal electronic spin fluctuation rates of several GHz. For reference, ALC measurements on the nonmagnetic compounds Li
2(ox)
2 and Na
2(ox)
2 were carried out and the muon hyperfine coupling constant were deduced to 115 and 150
MHz, respectively.</description><identifier>ISSN: 0921-4526</identifier><identifier>EISSN: 1873-2135</identifier><identifier>DOI: 10.1016/j.physb.2005.11.087</identifier><language>eng</language><publisher>Elsevier B.V</publisher><subject>Avoided level crossing muon spin resonance ; Hyperfine interaction ; Molecular magnets ; Spin fluctuation</subject><ispartof>Physica. B, Condensed matter, 2006-03, Vol.374, p.325-327</ispartof><rights>2005 Elsevier B.V.</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c334t-464ba0b5a130c7a14e588d93c3ccf73b86ec33ca2c3aaaffd5a54be2159513f93</citedby><cites>FETCH-LOGICAL-c334t-464ba0b5a130c7a14e588d93c3ccf73b86ec33ca2c3aaaffd5a54be2159513f93</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://dx.doi.org/10.1016/j.physb.2005.11.087$$EHTML$$P50$$Gelsevier$$H</linktohtml><link.rule.ids>314,780,784,3550,27924,27925,45995</link.rule.ids></links><search><creatorcontrib>Mennerich, C.</creatorcontrib><creatorcontrib>Scheuermann, R.</creatorcontrib><creatorcontrib>Luetkens, H.</creatorcontrib><creatorcontrib>Kühne, H.</creatorcontrib><creatorcontrib>Broekelmann, M.</creatorcontrib><creatorcontrib>Bosse, A.</creatorcontrib><creatorcontrib>Litterst, F.J.</creatorcontrib><creatorcontrib>Price, D.J.</creatorcontrib><creatorcontrib>Klauss, H.-H.</creatorcontrib><title>Muoniated radical formation and spin dynamics in molecular magnetic materials with oxalate ligands</title><title>Physica. B, Condensed matter</title><description>The crystal structure of Na
2T
2(ox)
2(H
2O)
2 with
T
=
Ni
(
II
)
,
Co
(
II
)
,
Fe
(
II
)
, and Mn(II) consists of isostructural compounds with an anionic transition metal oxalate network with a 2-leg ladder topology. We performed zero external field
μ
SR
, longitudinal-field quenching (LFQ) and avoided level-crossing (ALC) measurements on the Co-compound of this series. The measurements show that a significant fraction of the implanted muons forms a muoniated radical state by muonium addition to the resonant
π
electron system of the
(
COO
)
2
2
-
group. The LFQ measurements reveal electronic spin fluctuation rates of several GHz. For reference, ALC measurements on the nonmagnetic compounds Li
2(ox)
2 and Na
2(ox)
2 were carried out and the muon hyperfine coupling constant were deduced to 115 and 150
MHz, respectively.</description><subject>Avoided level crossing muon spin resonance</subject><subject>Hyperfine interaction</subject><subject>Molecular magnets</subject><subject>Spin fluctuation</subject><issn>0921-4526</issn><issn>1873-2135</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2006</creationdate><recordtype>article</recordtype><recordid>eNp9kE1PwzAMhiMEEmPwC7jkxK0lbpp-HDigiS8JxAXOkZu6W6a2GUkH7N-TMc74Yst-31fyw9gliBQEFNfrdLPahSbNhFApQCqq8ojNoCplkoFUx2wm6gySXGXFKTsLYS1iQQkz1rxs3WhxopZ7bK3BnnfODzhZN3IcWx42duTtbsTBmsDjPLiezLZHzwdcjjRZE4eJvMU-8C87rbj7xj5ueG-XMSGcs5Mu3ujir8_Z-_3d2-IxeX59eFrcPidGynxK8iJvUDQKQQpTIuSkqqqtpZHGdKVsqoKi0GBmJCJ2XatQ5Q1loGoFsqvlnF0dcjfefWwpTHqwwVDf40huG3RWy0JUEqJQHoTGuxA8dXrj7YB-p0HoPU-91r889Z6nBtCRZ3TdHFwUf_i05HUwlkZDrfVkJt06-6__B7HPgi4</recordid><startdate>20060331</startdate><enddate>20060331</enddate><creator>Mennerich, C.</creator><creator>Scheuermann, R.</creator><creator>Luetkens, H.</creator><creator>Kühne, H.</creator><creator>Broekelmann, M.</creator><creator>Bosse, A.</creator><creator>Litterst, F.J.</creator><creator>Price, D.J.</creator><creator>Klauss, H.-H.</creator><general>Elsevier B.V</general><scope>AAYXX</scope><scope>CITATION</scope><scope>7U5</scope><scope>8FD</scope><scope>L7M</scope></search><sort><creationdate>20060331</creationdate><title>Muoniated radical formation and spin dynamics in molecular magnetic materials with oxalate ligands</title><author>Mennerich, C. ; Scheuermann, R. ; Luetkens, H. ; Kühne, H. ; Broekelmann, M. ; Bosse, A. ; Litterst, F.J. ; Price, D.J. ; Klauss, H.-H.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c334t-464ba0b5a130c7a14e588d93c3ccf73b86ec33ca2c3aaaffd5a54be2159513f93</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2006</creationdate><topic>Avoided level crossing muon spin resonance</topic><topic>Hyperfine interaction</topic><topic>Molecular magnets</topic><topic>Spin fluctuation</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Mennerich, C.</creatorcontrib><creatorcontrib>Scheuermann, R.</creatorcontrib><creatorcontrib>Luetkens, H.</creatorcontrib><creatorcontrib>Kühne, H.</creatorcontrib><creatorcontrib>Broekelmann, M.</creatorcontrib><creatorcontrib>Bosse, A.</creatorcontrib><creatorcontrib>Litterst, F.J.</creatorcontrib><creatorcontrib>Price, D.J.</creatorcontrib><creatorcontrib>Klauss, H.-H.</creatorcontrib><collection>CrossRef</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>Technology Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Physica. B, Condensed matter</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Mennerich, C.</au><au>Scheuermann, R.</au><au>Luetkens, H.</au><au>Kühne, H.</au><au>Broekelmann, M.</au><au>Bosse, A.</au><au>Litterst, F.J.</au><au>Price, D.J.</au><au>Klauss, H.-H.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Muoniated radical formation and spin dynamics in molecular magnetic materials with oxalate ligands</atitle><jtitle>Physica. B, Condensed matter</jtitle><date>2006-03-31</date><risdate>2006</risdate><volume>374</volume><spage>325</spage><epage>327</epage><pages>325-327</pages><issn>0921-4526</issn><eissn>1873-2135</eissn><abstract>The crystal structure of Na
2T
2(ox)
2(H
2O)
2 with
T
=
Ni
(
II
)
,
Co
(
II
)
,
Fe
(
II
)
, and Mn(II) consists of isostructural compounds with an anionic transition metal oxalate network with a 2-leg ladder topology. We performed zero external field
μ
SR
, longitudinal-field quenching (LFQ) and avoided level-crossing (ALC) measurements on the Co-compound of this series. The measurements show that a significant fraction of the implanted muons forms a muoniated radical state by muonium addition to the resonant
π
electron system of the
(
COO
)
2
2
-
group. The LFQ measurements reveal electronic spin fluctuation rates of several GHz. For reference, ALC measurements on the nonmagnetic compounds Li
2(ox)
2 and Na
2(ox)
2 were carried out and the muon hyperfine coupling constant were deduced to 115 and 150
MHz, respectively.</abstract><pub>Elsevier B.V</pub><doi>10.1016/j.physb.2005.11.087</doi><tpages>3</tpages></addata></record> |
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language | eng |
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source | Elsevier ScienceDirect Journals Complete |
subjects | Avoided level crossing muon spin resonance Hyperfine interaction Molecular magnets Spin fluctuation |
title | Muoniated radical formation and spin dynamics in molecular magnetic materials with oxalate ligands |
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