메뉴 건너뛰기




Volumn 78, Issue 20, 2008, Pages

Crossover in charge transport from one-dimensional copper-oxygen chains to two-dimensional ladders in (La,Y)y(Sr,Ca)14-yCu 24O41

Author keywords

[No Author keywords available]

Indexed keywords


EID: 56349128197     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.78.205105     Document Type: Article
Times cited : (4)

References (34)
  • 17
    • 0001288575 scopus 로고    scopus 로고
    • 10.1103/PhysRevB.53.12201
    • M. Matsuda and K. Katsumata, Phys. Rev. B 53, 12201 (1996). 10.1103/PhysRevB.53.12201
    • (1996) Phys. Rev. B , vol.53 , pp. 12201
    • Matsuda, M.1    Katsumata, K.2
  • 21
    • 56349159844 scopus 로고    scopus 로고
    • The main condition to establish AF dimer+CO is that the number of holes in the chains per formula unit is close to 6. This requirement is satisfied according to Ref., while it cannot be reconciled with the hole distribution suggested in Ref..
    • The main condition to establish AF dimer+CO is that the number of holes in the chains per formula unit is close to 6. This requirement is satisfied according to Ref., while it cannot be reconciled with the hole distribution suggested in Ref..
  • 24
    • 56349118233 scopus 로고    scopus 로고
    • http://www.ccp14.ac.uk/tutorial/lmgp/orientexpress.htm
  • 27
    • 56349089076 scopus 로고    scopus 로고
    • The measurement of ac conductivity for y=0.55 and 1.6 was done at 250 and 200 K, respectively, due to too high conductivity values causing too low transmittivity of prepared plane-parallel samples.
    • The measurement of ac conductivity for y=0.55 and 1.6 was done at 250 and 200 K, respectively, due to too high conductivity values causing too low transmittivity of prepared plane-parallel samples.
  • 28
    • 56349111233 scopus 로고    scopus 로고
    • While Drude response is clearly visible at RT for y=0.55 (E∥c) and y=1.6 (E∥a) it is masked by the phonon tail for y=1.6 (E∥c).
    • While Drude response is clearly visible at RT for y=0.55 (E∥c) and y=1.6 (E∥a) it is masked by the phonon tail for y=1.6 (E∥c).
  • 29
    • 56349165408 scopus 로고    scopus 로고
    • We remind that only at low temperatures one standardly expects that due to frozen charge carriers a low-energy phonon contribution prevails over electronic hopping.
    • We remind that only at low temperatures one standardly expects that due to frozen charge carriers a low-energy phonon contribution prevails over electronic hopping.
  • 32
    • 0030188991 scopus 로고    scopus 로고
    • 10.1016/0921-4534(96)00254-7
    • M. Kato, T. Adachi, and Y. Koike, Physica C 265, 107 (1996). 10.1016/0921-4534(96)00254-7
    • (1996) Physica C , vol.265 , pp. 107
    • Kato, M.1    Adachi, T.2    Koike, Y.3


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.