Antiferromagnetic ground state of molecular π-d system λ-(BEDT-STF)2FeCl4 studied by site-selective magnetization and thermodynamic measurements
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- Material Type
- 記事
- Author/Editor
- Shuhei FukuokaAtsushi 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
- DOI
- 10.1246/cl.210767
- Persistent ID (NDL)
- info:ndljp/pid/12299133
- Collection
- 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
- Acquisition Basis
- オンライン資料収集制度
- Date Accepted (W3CDTF)
- 2022-06-13T20:11:05+09:00
- Date Captured (W3CDTF)
- 2022-06-03
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- application/pdf
- Access Restrictions
- 国立国会図書館内限定公開
- Service for the Digitized Contents Transmission Service
- 図書館・個人送信対象外
- Availability of remote photoduplication service
- 可
- Periodical Title (URI)
- Periodical Title (Persistent ID (NDL))
- info:ndljp/pid/12299132
- Data Provider (Database)
- 国立国会図書館 : 国立国会図書館デジタルコレクション
- 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
- DOI
- 10.1246/cl.210767
- Related Material (URI)
- 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 NMRMultistep Development of the Hyperfine Fields in λ-(BEDT-STF)<sub>2</sub>FeCl<sub>4</sub> Studied by Mössbauer SpectroscopyMagnetic and Electric Properties of Organic Conductors Probed by 13C-NMR Using Selective-Site Substituted MoleculesAntiferromagnetic Insulating Ground State of Molecular π-d System Λ-(BETS)2FeCl4 (BETS = Bis(ethylenedithio)tetraselenafulvalene): A Theoretical and Experimental ReviewNew 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 AnionsMagnetic 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 AntiferromagnetsEvidence 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> NMRParamagnetic Metal—Antiferromagnetic Insulator Transition in π-d System λ-BETS2FeCl4, BETS = Bis(ethylenedithio)tetraselenafulvaleneSelective 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>]BrThermodynamic 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)2GaCl4New 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 spectroscopyUnconventional 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> NMRThe Electrical Behavior of Charge-Transfer Salts Based on an Unsymmetrical Donor Bis(ethylenedithio)diselenadithiafulvalene (STF): Disorder Effect on the Transport PropertiesParamagnetic 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> SystemSuperconducting Phase in λ-(BEDT-STF)<sub>2</sub>GaCl<sub>4</sub> at High PressuresOn Scaling Relations of Organic Antiferromagnets with Magnetic AnionsSite-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 propertiesPhase 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 6Magnetic-field-induced superconductivity in a two-dimensional organic conductorProton 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 systemField-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)2FeCl4Interplay between chains of localised spins and two-dimensional sheets of organic donors in the synthetically built magnetic multilayerElectrical Conductivity of the Perylene–Bromine ComplexSuperconductivity 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)2FeCl4NMR study of partially deuterated κ-(BEDT-TTF)2Cu[N(CN)2]BrSuperconducting 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 measurementsNuclear Resonance Absorption in Hydrated Crystals: Fine Structure of the Proton LineBandwidth and band filling control in organic conductorsMössbauer 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 anionsGlobal Phase Diagram of the Magnetic Field-Induced Organic Superconductors λ-(BETS)2FexGa1−xCl4Mysterious paramagnetic states of Fe 3d spin in antiferromagnetic insulator of κ-BETS2FeCl4systemGap Symmetry of the Organic Superconductor λ-(BETS)₂GaCl₄ Determined by Magnetic-Field-Angle-Resolved Heat CapacityThermodynamic Investigation on Antiferromagnetic Ordered State of the Molecular π-d System λ-(BEDT-STF)₂FeCl₄Critical Phenomena in Coupled Magnetic Systems : Application to the Organic Antiferromagnet λ-(BETS)₂FeCl₄Mean Field Theory of a Coupled Heisenberg Model and Its Application to an Organic Antiferromagnet with Magnetic AnionsDetailed X-band Studies of the π-d Molecular Conductor λ-(BETS)₂FeCl₄ : Observation of Anomalous Angular Dependence of the g-valueEffects 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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- 国立情報学研究所 : CiNii Research
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- 雑誌記事索引データベースCrossref科学研究費助成事業データベース科学研究費助成事業データベース
- Bibliographic ID (NDL)
- 12299133