TY - JOUR
T1 - Charge ordering and π-d interaction in electron-doped 3/4-filling molecular system a''-(BEDT-TTF)2Rb2xCo(SCN)4(x = 0.6)
AU - Iguchi, Satoshi
AU - Yamada, Syuhei
AU - Kobayashi, Ryota
AU - Morita, Koutaro
AU - Kudo, Yuki
AU - Kurosu, Megumi
AU - Yoneyama, Naoki
AU - Ikemoto, Yuka
AU - Moriwaki, Taro
AU - Sasaki, Takahiko
N1 - Funding Information:
Acknowledgements This study was partly supported by JSPS KAKENHI Grant Nos. 16K05430, 18H04298, 19H01833, and 20H05144. The optical measurements in the far-infrared region were performed at the BL43IR of SPring-8 with the approval of JASRI (Proposal Nos. 2016A0073 and 2018A0073). The measurements at high magnetic fields were supported by the High Field Laboratory for Superconducting Materials (Project Nos. 16H0412, 18H0405, and 19H0411), Institute for Materials Research, Tohoku University.
Funding Information:
This study was partly supported by JSPS KAKENHI Grant Nos. 16K05430, 18H04298, 19H01833, and 20H05144. The optical measurements in the far-infrared region were performed at the BL43IR of SPring- 8 with the approval of JASRI (Proposal Nos. 2016A0073 and 2018A0073). The measurements at high magnetic fields were supported by the High Field Laboratory for Superconducting Materials (Project Nos. 16H0412, 18H0405, and 19H0411), Institute for Materials Research, Tohoku University.
Publisher Copyright:
© 2021 The Physical Society of Japan.
PY - 2021/7/1
Y1 - 2021/7/1
N2 - We have investigated a newly found a''-phase bis(ethylenedithio)tetrathiafulvalene (BEDT-TTF) molecular arrangement system, namely, a''-(BEDT-TTF)2Rb2xCo(SCN)4 (a''-Rb2xCo), with localized S = 3/2 Co2+ spins. From X-ray structural analyses, we found that owing to the nonstoichiometric ratio of Rb ions (x = 0.6), this compound takes an intermediate value of p-electron band filling between those of a''-(BEDT-TTF)2CsHg(SCN)4 and a''-(BEDTTTF) 2K1.4Co(SCN)4. a''-Rb2xCo (x = 0.6) is a paramagnetic metal at room temperature and exhibits a first-order transition to an insulating state at 100 K, which is the lowest among the three compounds. The results of the twodimensional optical conductivity spectra and peak splitting of charge-sensitive ν27 molecular vibrational modes indicate the phase transition to a state with a gap of 600 cm-1, which is attributed to charge ordering consisting of at least four differently charged BEDT-TTF molecules. The π-spin susceptibility suddenly decreases at the transition temperature, and another anomaly can be seen at about 40 K. Given that π-spin disappears at 100K (i.e., formation of a spin-singlet state), it is difficult to systematically explain other physical properties as a whole at low temperatures. However, by simply assuming the presence of p spins, we can account for all the observed results without contradiction. We also discuss anomalies in the dielectricity of p electrons under magnetic fields mediated by p-d interactions and the spincharge coupling.
AB - We have investigated a newly found a''-phase bis(ethylenedithio)tetrathiafulvalene (BEDT-TTF) molecular arrangement system, namely, a''-(BEDT-TTF)2Rb2xCo(SCN)4 (a''-Rb2xCo), with localized S = 3/2 Co2+ spins. From X-ray structural analyses, we found that owing to the nonstoichiometric ratio of Rb ions (x = 0.6), this compound takes an intermediate value of p-electron band filling between those of a''-(BEDT-TTF)2CsHg(SCN)4 and a''-(BEDTTTF) 2K1.4Co(SCN)4. a''-Rb2xCo (x = 0.6) is a paramagnetic metal at room temperature and exhibits a first-order transition to an insulating state at 100 K, which is the lowest among the three compounds. The results of the twodimensional optical conductivity spectra and peak splitting of charge-sensitive ν27 molecular vibrational modes indicate the phase transition to a state with a gap of 600 cm-1, which is attributed to charge ordering consisting of at least four differently charged BEDT-TTF molecules. The π-spin susceptibility suddenly decreases at the transition temperature, and another anomaly can be seen at about 40 K. Given that π-spin disappears at 100K (i.e., formation of a spin-singlet state), it is difficult to systematically explain other physical properties as a whole at low temperatures. However, by simply assuming the presence of p spins, we can account for all the observed results without contradiction. We also discuss anomalies in the dielectricity of p electrons under magnetic fields mediated by p-d interactions and the spincharge coupling.
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U2 - 10.7566/JPSJ.90.074701
DO - 10.7566/JPSJ.90.074701
M3 - Article
AN - SCOPUS:85107998787
SN - 0031-9015
VL - 90
JO - Journal of the Physical Society of Japan
JF - Journal of the Physical Society of Japan
IS - 7
M1 - 074701
ER -