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Volume number51 (4)
Antiferrom...

Antiferromagnetic ground state of molecular π-d system λ-(BEDT-STF)2FeCl4 studied by site-selective magnetization and thermodynamic measurements

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Antiferromagnetic ground state of molecular π-d system λ-(BEDT-STF)2FeCl4 studied by site-selective magnetization and thermodynamic measurements

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info:ndljp/pid/12299133
Material type
記事
Author
Shuhei Fukuokaほか
Publisher
The Chemical Society of Japan
Publication date
2022-02-01
Material Format
Digital
Journal name
Chemistry letters 51(4)
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-
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コレクション : 国立国会図書館デジタルコレクション > 電子書籍・電子雑誌 > 学術機関 > 学協会(Provided by: CiNii Research)

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Material Type
記事
Author/Editor
Shuhei Fukuoka
Atsushi Kawamoto
Publication, Distribution, etc.
Publication Date
2022-02-01
Publication Date (W3CDTF)
2022-02-01
Periodical title
Chemistry letters
No. or year of volume/issue
51(4)
Volume
51(4)
ISSN (Periodical Title)
1348-0715
ISSN-L (Periodical Title)
0366-7022
Text Language Code
eng
Persistent ID (NDL)
info:ndljp/pid/12299133
Collection (Materials For Handicapped People:1)
Collection (particular)
国立国会図書館デジタルコレクション > 電子書籍・電子雑誌 > 学術機関 > 学協会
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Date Accepted (W3CDTF)
2022-06-13T20:11:05+09:00
Date Captured (W3CDTF)
2022-06-03
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application/pdf
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国立国会図書館内限定公開
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Periodical Title (Persistent ID (NDL))
info:ndljp/pid/12299132
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国立国会図書館 : 国立国会図書館デジタルコレクション

Digital

Summary, etc.
コレクション : 国立国会図書館デジタルコレクション > 電子書籍・電子雑誌 > 学術機関 > 学協会
References
Role of the <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:mi>d</mml:mi><mml:mtext>−</mml:mtext><mml:mi>d</mml:mi></mml:mrow></mml:math> interaction in the antiferromagnetic phase of <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mi>λ</mml:mi><mml:mtext>−</mml:mtext><mml:mrow><mml:msub><mml:mrow><mml:mo>(</mml:mo><mml:mi>BEDT</mml:mi><mml:mtext>−</mml:mtext><mml:mi>STF</mml:mi><mml:mo>)</mml:mo></mml:mrow><mml:mn>2</mml:mn></mml:msub><mml:msub><mml:mi>FeCl</mml:mi><mml:mn>4</mml:mn></mml:msub></mml:mrow></mml:math>
Stabilization of Long-Range Order by Additional Anisotropic Spins in Two-Dimensional Isotropic Heisenberg Antiferromagnets —A Possible Model of an Organic Compound with Magnetic Anions—
Antiferromagnetic Ordering in Organic Conductor λ-(BEDT-TTF)<sub>2</sub>GaCl<sub>4</sub> Probed by <sup>13</sup>C NMR
Multistep Development of the Hyperfine Fields in λ-(BEDT-STF)<sub>2</sub>FeCl<sub>4</sub> Studied by Mössbauer Spectroscopy
Magnetic and Electric Properties of Organic Conductors Probed by 13C-NMR Using Selective-Site Substituted Molecules
Antiferromagnetic Insulating Ground State of Molecular π-d System Λ-(BETS)2FeCl4 (BETS = Bis(ethylenedithio)tetraselenafulvalene): A Theoretical and Experimental Review
New BETS Conductors with Magnetic Anions (BETS = bis(ethylenedithio)tetraselenafulvalene)
Temperature-Composition Phase Diagram of the Organic Alloys, λ-BETS2(FeXGa1−X)Cl4, with Mixed Magnetic and Non-Magnetic Anions
Magnetic and Thermal Properties of λ-(BETS)<sub>2</sub>FeCl<sub>4</sub> System –Fe 3<i>d</i> Spin in Antiferromagnetic Insulating Phase–
Thermodynamic Evidence of <i>d</i>-Wave Superconductivity of the Organic Superconductor λ-(BETS)<sub>2</sub>GaCl<sub>4</sub>
Spin Wave Theory in Two-Dimensional Coupled Antiferromagnets
Evidence of antiferromagnetic fluctuation in the unconventional superconductor <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mi>λ</mml:mi></mml:math> -(BETS) <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:msub><mml:mrow/><mml:mn>2</mml:mn></mml:msub><mml:msub><mml:mi>GaCl</mml:mi><mml:mn>4</mml:mn></mml:msub></mml:mrow></mml:math> by <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mmultiscripts><mml:mi mathvariant="normal">C</mml:mi><mml:mprescripts/><mml:none/><mml:mn>13</mml:mn></mml:mmultiscripts></mml:math> NMR
Paramagnetic Metal—Antiferromagnetic Insulator Transition in π-d System λ-BETS2FeCl4, BETS = Bis(ethylenedithio)tetraselenafulvalene
Selective observation of sublattice magnetization in the molecular <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:mi>π</mml:mi><mml:mo>−</mml:mo><mml:mi>d</mml:mi></mml:mrow></mml:math> system <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:mi>λ</mml:mi><mml:mo>−</mml:mo><mml:msub><mml:mrow><mml:mo>(</mml:mo><mml:mi>BEDT</mml:mi><mml:mo>−</mml:mo><mml:mi>STF</mml:mi><mml:mo>)</mml:mo></mml:mrow><mml:mn>2</mml:mn></mml:msub><mml:msub><mml:mi>FeCl</mml:mi><mml:mn>4</mml:mn></mml:msub></mml:mrow></mml:math> studied by <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mmultiscripts><mml:mi mathvariant="normal">C</mml:mi><mml:mprescripts/><mml:none/><mml:mn>13</mml:mn></mml:mmultiscripts></mml:math> NMR
<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mmultiscripts><mml:mrow><mml:mi mathvariant="normal">C</mml:mi></mml:mrow><mml:mprescripts/><mml:mrow/><mml:mrow><mml:mn>13</mml:mn></mml:mrow><mml:mrow/><mml:mrow/></mml:mmultiscripts></mml:mrow></mml:math>NMR studies of the normal and superconducting states of the organic superconductor κ-(ET<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msub><mml:mrow><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math>Cu[N(CN<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msub><mml:mrow><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math>]Br
<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mmultiscripts><mml:mrow><mml:mi mathvariant="normal">C</mml:mi></mml:mrow><mml:mprescripts/><mml:mrow/><mml:mrow><mml:mn>13</mml:mn></mml:mrow><mml:mrow/><mml:mrow/></mml:mmultiscripts></mml:mrow></mml:math>NMR line-shape studies of the organic superconductor κ-(ET<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msub><mml:mrow><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math>Cu[N(CN<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msub><mml:mrow><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math>]Br
Thermodynamic evidence for the formation of a Fulde-Ferrell-Larkin-Ovchinnikov phase in the organic superconductor <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mi>λ</mml:mi><mml:mo>−</mml:mo><mml:mrow><mml:msub><mml:mrow><mml:mo>(</mml:mo><mml:mi>BETS</mml:mi><mml:mo>)</mml:mo></mml:mrow><mml:mn>2</mml:mn></mml:msub><mml:msub><mml:mi>GaCl</mml:mi><mml:mn>4</mml:mn></mml:msub></mml:mrow></mml:math>
A New Organic Superconductor, λ-(BEDT-TSF)2GaCl4
New Organic Metals Based on BETS Compounds with MX4− Anions (BETS = bis(ethylenedithio)tetraselenafulvalene; M = Ga, Fe, In; X = Cl, Br)
Modification of local electronic state by BEDT-STF doping to<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mi>κ</mml:mi></mml:math>-(BEDT-TTF)<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:msub><mml:mrow/><mml:mn>2</mml:mn></mml:msub><mml:msub><mml:mrow><mml:mi>Cu</mml:mi><mml:mo>[</mml:mo><mml:mi mathvariant="normal">N</mml:mi><mml:mo>(</mml:mo><mml:mi>CN</mml:mi><mml:mo>)</mml:mo></mml:mrow><mml:mn>2</mml:mn></mml:msub><mml:mrow><mml:mo>]</mml:mo><mml:mi>Br</mml:mi></mml:mrow></mml:mrow></mml:math>salt studied by<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mmultiscripts><mml:mi mathvariant="normal">C</mml:mi><mml:mprescripts/><mml:none/><mml:mn>13</mml:mn></mml:mmultiscripts></mml:math>NMR spectroscopy
Unconventional superconductivity in <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mi>λ</mml:mi></mml:math> -(BETS) <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:msub><mml:mrow/><mml:mn>2</mml:mn></mml:msub><mml:msub><mml:mi>GaCl</mml:mi><mml:mn>4</mml:mn></mml:msub></mml:mrow></mml:math> probed by <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mmultiscripts><mml:mi mathvariant="normal">C</mml:mi><mml:mprescripts/><mml:none/><mml:mn>13</mml:mn></mml:mmultiscripts></mml:math> NMR
The Electrical Behavior of Charge-Transfer Salts Based on an Unsymmetrical Donor Bis(ethylenedithio)diselenadithiafulvalene (STF): Disorder Effect on the Transport Properties
Paramagnetic Metal–Antiferromagnetic Insulator Transition of λ-BETS<sub>2</sub>Fe<sub><i>x</i></sub>Ga<sub>1-<i>x</i></sub>Cl<sub>4</sub> System
Superconducting Phase in λ-(BEDT-STF)<sub>2</sub>GaCl<sub>4</sub> at High Pressures
On Scaling Relations of Organic Antiferromagnets with Magnetic Anions
Site-specific <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mmultiscripts><mml:mi mathvariant="normal">C</mml:mi><mml:mprescripts/><mml:none/><mml:mn>13</mml:mn></mml:mmultiscripts></mml:math> NMR study on the locally distorted triangular lattice of the organic conductor <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mi>κ</mml:mi><mml:mo>−</mml:mo><mml:mrow><mml:msub><mml:mrow><mml:mo>(</mml:mo><mml:mi>BEDT</mml:mi><mml:mo>−</mml:mo><mml:mi>TTF</mml:mi><mml:mo>)</mml:mo></mml:mrow><mml:mn>2</mml:mn></mml:msub><mml:msub><mml:mi>Cu</mml:mi><mml:mn>2</mml:mn></mml:msub><mml:msub><mml:mrow><mml:mo>(</mml:mo><mml:mi>CN</mml:mi><mml:mo>)</mml:mo></mml:mrow><mml:mn>3</mml:mn></mml:msub></mml:mrow></mml:math>
Magnetic field–temperature phase diagram of the quasi-two-dimensional organic superconductor<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>λ</mml:mi><mml:mo>−</mml:mo><mml:mo>(</mml:mo><mml:mi mathvariant="normal">BETS</mml:mi><mml:mrow><mml:msub><mml:mrow><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant="normal">GaCl</mml:mi></mml:mrow><mml:mrow><mml:mn>4</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math>studied via thermal conductivity
(BEDT-TTF)2GaCl4: Structure, electrical and magnetic properties
Phase diagram and anomalous constant resistivity state of a magnetic organic superconducting alloy, λ-(BETS)<sub>2</sub>FexGa<sub>1−x</sub>Cl<sub>4</sub>
Superconductivity in a synthetic organic conductor (TMTSF)2PF 6
Magnetic-field-induced superconductivity in a two-dimensional organic conductor
Proton NMR measurements of the local magnetic field in the paramagnetic metal and antiferromagnetic insulator phases of<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mi>λ</mml:mi><mml:mtext>−</mml:mtext><mml:mo>(</mml:mo><mml:mi>BETS</mml:mi><mml:msub><mml:mo>)</mml:mo><mml:mn>2</mml:mn></mml:msub><mml:msub><mml:mi>FeCl</mml:mi><mml:mn>4</mml:mn></mml:msub></mml:mrow></mml:math>
Possible highT c superconductivity in the Ba?La?Cu?O system
Field-induced metal-insulator transition in partially deuterated<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mi>κ</mml:mi><mml:mtext>−</mml:mtext><mml:msub><mml:mrow><mml:mo>(</mml:mo><mml:mi>BEDT</mml:mi><mml:mtext>−</mml:mtext><mml:mi>TTF</mml:mi><mml:mo>)</mml:mo></mml:mrow><mml:mn>2</mml:mn></mml:msub><mml:mi mathvariant="normal">Cu</mml:mi><mml:mrow><mml:mo>[</mml:mo><mml:mi mathvariant="normal">N</mml:mi><mml:msub><mml:mrow><mml:mo>(</mml:mo><mml:mi mathvariant="normal">C</mml:mi><mml:mi mathvariant="normal">N</mml:mi><mml:mo>)</mml:mo></mml:mrow><mml:mn>2</mml:mn></mml:msub><mml:mo>]</mml:mo></mml:mrow><mml:mi mathvariant="normal">Br</mml:mi></mml:mrow></mml:math>
Specific heat studies for λ-(BEDT-TSF)2FeCl4
Interplay between chains of localised spins and two-dimensional sheets of organic donors in the synthetically built magnetic multilayer
Electrical Conductivity of the Perylene–Bromine Complex
Superconductivity in the Presence of Strong Pauli Paramagnetism: Ce<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant="normal">Cu</mml:mi></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant="normal">Si</mml:mi></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math>
Magnetic anisotropy of organic conductor λ-(BETS)2FeCl4
NMR study of partially deuterated κ-(BEDT-TTF)2Cu[N(CN)2]Br
Superconducting phase diagram and FFLO signature in<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mi>λ</mml:mi></mml:mrow></mml:math>-(BETS)<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msub><mml:mrow/><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math>GaCl<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msub><mml:mrow/><mml:mrow><mml:mn>4</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math>from rf penetration depth measurements
Nuclear Resonance Absorption in Hydrated Crystals: Fine Structure of the Proton Line
Bandwidth and band filling control in organic conductors
Mössbauer spectroscopy and magnetic transition of<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mi>λ</mml:mi><mml:mtext>−</mml:mtext><mml:msub><mml:mrow><mml:mrow><mml:mo>(</mml:mo><mml:mrow><mml:mtext>BETS</mml:mtext></mml:mrow><mml:mo>)</mml:mo></mml:mrow></mml:mrow><mml:mn>2</mml:mn></mml:msub><mml:msub><mml:mrow><mml:mtext>FeCl</mml:mtext></mml:mrow><mml:mn>4</mml:mn></mml:msub></mml:mrow></mml:math>
A New Ambient Pressure Organic Superconductor Based on BEDT-TTF with TC Higher than 10 K (TC=10.4 K)
Estimation of πd-interaction in organic conductors including magnetic anions
Global Phase Diagram of the Magnetic Field-Induced Organic Superconductors λ-(BETS)2FexGa1−xCl4
Mysterious paramagnetic states of Fe 3d spin in antiferromagnetic insulator of κ-BETS2FeCl4system
Gap Symmetry of the Organic Superconductor λ-(BETS)₂GaCl₄ Determined by Magnetic-Field-Angle-Resolved Heat Capacity
Thermodynamic Investigation on Antiferromagnetic Ordered State of the Molecular π-d System λ-(BEDT-STF)₂FeCl₄
Critical Phenomena in Coupled Magnetic Systems : Application to the Organic Antiferromagnet λ-(BETS)₂FeCl₄
Mean Field Theory of a Coupled Heisenberg Model and Its Application to an Organic Antiferromagnet with Magnetic Anions
Detailed X-band Studies of the π-d Molecular Conductor λ-(BETS)₂FeCl₄ : Observation of Anomalous Angular Dependence of the g-value
Effects of Anion Substitution on Unconventional Antiferromagnetic Ground State of Molecular π-d System λ-(BEDT-STF)₂Fe[x]Ga[1-x]Cl₄
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Bibliographic ID (NDL)
12299133