메뉴 건너뛰기




Volumn 77, Issue 2, 2008, Pages

Infrared and Raman study of the charge-ordered state in the vicinity of the superconducting state in the organic conductor β-(meso-DMBEDT-TTF) 2PF6

Author keywords

(meso DMBEDT TTF)2PF6; Charge fluctuation; Charge order; High pressure; Organic conductor; Superconductivity

Indexed keywords


EID: 54349122256     PISSN: 00319015     EISSN: 13474073     Source Type: Journal    
DOI: 10.1143/JPSJ.77.024714     Document Type: Article
Times cited : (23)

References (45)
  • 4
    • 54349099797 scopus 로고    scopus 로고
    • M. Itoh, N. Akimoto, H. Yamada, M. Isobe, and Y. Ueda: Proc. Int. Workshop Magnetic Excitations in Strongly Correlated Electrons, J. Phys. Soc. Jpn. 69 (2000) Suppl. B, p. 155.
    • M. Itoh, N. Akimoto, H. Yamada, M. Isobe, and Y. Ueda: Proc. Int. Workshop Magnetic Excitations in Strongly Correlated Electrons, J. Phys. Soc. Jpn. 69 (2000) Suppl. B, p. 155.
  • 23
    • 54349089455 scopus 로고    scopus 로고
    • 1 line converted into pressure is negligible within ±0.1 kbar above 100 K, but it increase to ±0.5 kbar below 50 K.
    • 1 line converted into pressure is negligible within ±0.1 kbar above 100 K, but it increase to ±0.5 kbar below 50 K.
  • 24
    • 54349122588 scopus 로고    scopus 로고
    • Gaussian98, revision A.11. Gaussian Inc.
    • Gaussian98, revision A.11. Gaussian Inc.
  • 31
    • 54349107973 scopus 로고    scopus 로고
    • 1).
    • 1).
  • 32
    • 54349117566 scopus 로고    scopus 로고
    • -1 band below 68 K.
    • -1 band below 68 K.
  • 33
    • 1842584447 scopus 로고    scopus 로고
    • When the EMV interaction is strong, the splitting is mainly governed not by the difference in valence but by the EMV effect. In this case, the high-frequency mode persists at the same position before splitting
    • K. Suzuki, K. Yamamoto, and K. Yakushi: Phys. Rev. B 69 (2004) 085114. When the EMV interaction is strong, the splitting is mainly governed not by the difference in valence but by the EMV effect. In this case, the high-frequency mode persists at the same position before splitting.
    • (2004) Phys. Rev. B , vol.69 , pp. 085114
    • Suzuki, K.1    Yamamoto, K.2    Yakushi, K.3
  • 38
    • 54349104987 scopus 로고    scopus 로고
    • The transfer integral is estimatd from the empirical relation, t ∼ -10S, where S is the overlap integral that is given in ref. 16.
    • The transfer integral is estimatd from the empirical relation, t ∼ -10S, where S is the overlap integral that is given in ref. 16.
  • 41
    • 54349091177 scopus 로고    scopus 로고
    • private communication
    • H. Sawa: private communication.
    • Sawa, H.1
  • 42
  • 44
    • 0034507105 scopus 로고    scopus 로고
    • 2X, has a coexistent region of AF and SC states between the AF phase and SC phase. [S. Lefebvre, P. Wzietek, S. Brown, C. Bourbonnais, D. Jerome, C. Meziere, M. Fourmigue, and P. Batail: Phys. Rev. Lett. 85 (2000) 5420.]
    • 2X, has a coexistent region of AF and SC states between the AF phase and SC phase. [S. Lefebvre, P. Wzietek, S. Brown, C. Bourbonnais, D. Jerome, C. Meziere, M. Fourmigue, and P. Batail: Phys. Rev. Lett. 85 (2000) 5420.]
  • 45


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.