M. Hirata

activity

19972021

most citedObservation of an anisotropic Dirac cone reshaping and ferrimagnetic spin polarization in an organic conductor

138 citations · 491 across the 18 of their papers we have counts for

collaborators

Showing cond-mat.mtrl-sciShow all

3 papers · 1 filter

cond-mat.mtrl-sci2020★ 3 cited

Magnetic-Field Dependence of Novel Gap Behavior Related to the Quantum-Size Effect

Tomonori Okuno, Yuta Kinoshita, Satoshi Matsuzaki +6

$^{195}$ Pt-NMR measurements of Pt nanoparticles with a mean diameter of 4.0 nm were performed in a high magnetic field of approximately $μ_{0} H = 23.3$ T to investigate the low-temp…

cond-mat.mtrl-sci2012★ 9 cited

Electron Correlations in the Quasi-Two-Dimensional Organic Conductor $θ$ -(BEDT-TTF) $_{2}$ I $_{3}$ investigated by $^{13}$ C NMR

Michihiro Hirata, Kazuya Miyagawa, Kazushi Kanoda +1

We report a $^{13}$ C-NMR study on the ambient-pressure metallic phase of the layered organic conductor $θ$ -(BEDT-TTF) $_{2}$ I $_{3}$ [BEDT-TTF: bisethylenedithio-tetrathiafulvalene],…

cond-mat.mtrl-sci2011★ 30 cited

$^{13}$ C NMR Study on the Charge-Disproportionated Conducting State in the Quasi-Two-Dimensional Organic Conductor $α$ -(BEDT-TTF) $_{2}$ I $_{3}$

Michihiro Hirata, Kyohei Ishikawa, Kazuya Miyagawa +1

The conducting state of the quasi-two-dimensional organic conductor, $α$ -(BEDT-TTF) $_{2}$ I $_{3}$ , at ambient pressure is investigated with $^{13}$ C NMR measurements, which separate the…

Magnetic-Field Dependence of Novel Gap Behavior Related to the Quantum-Size Effect

Electron Correlations in the Quasi-Two-Dimensional Organic Conductor θ-(BEDT-TTF)2​I3​ investigated by 13C NMR

13C NMR Study on the Charge-Disproportionated Conducting State in the Quasi-Two-Dimensional Organic Conductor α-(BEDT-TTF)2​I3​

Electron Correlations in the Quasi-Two-Dimensional Organic Conductor $θ$ -(BEDT-TTF) $_{2}$ I $_{3}$ investigated by $^{13}$ C NMR

$^{13}$ C NMR Study on the Charge-Disproportionated Conducting State in the Quasi-Two-Dimensional Organic Conductor $α$ -(BEDT-TTF) $_{2}$ I $_{3}$