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Volumn 79, Issue 4, 2009, Pages

Quasi-one-dimensional Fermi surface of (TMTSF)2NO3

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EID: 59749088424     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.79.045115     Document Type: Article
Times cited : (17)

References (34)
  • 1
    • 34848868725 scopus 로고    scopus 로고
    • Series in Materials Science Vol. Springer-Verlag, Berlin
    • A. G. Lebed, Organic Conductors and Superconductors, Series in Materials Science Vol. 100 (Springer-Verlag, Berlin, 2008).
    • (2008) Organic Conductors and Superconductors , vol.100
    • Lebed, A.G.1
  • 2
    • 0000538952 scopus 로고
    • 10.1103/PhysRevB.31.4770
    • P. M. Chaikin, Phys. Rev. B 31, 4770 (1985). 10.1103/PhysRevB.31.4770
    • (1985) Phys. Rev. B , vol.31 , pp. 4770
    • Chaikin, P.M.1
  • 5
    • 53249093496 scopus 로고
    • 10.1143/JPSJ.58.1520
    • K. Yamaji, J. Phys. Soc. Jpn. 58, 1520 (1989). 10.1143/JPSJ.58.1520
    • (1989) J. Phys. Soc. Jpn. , vol.58 , pp. 1520
    • Yamaji, K.1
  • 6
    • 59749097171 scopus 로고    scopus 로고
    • The angular positions θN of the KKY resonance peaks are given as (Ref.) c kF cot θN =π (N- 1 4) -C, where c is the distance between adjacent conducting planes, kF is the wave vector whose projection is on the Fermi surface, and N is the index of resonance. C is a constant depending on the azimuthal angle.
    • The angular positions θN of the KKY resonance peaks are given as (Ref.) c kF cot θN =π (N- 1 4) -C, where c is the distance between adjacent conducting planes, kF is the wave vector whose projection is on the Fermi surface, and N is the index of resonance. C is a constant depending on the azimuthal angle.
  • 10
    • 4243690091 scopus 로고
    • 10.1103/PhysRevLett.50.1005
    • P. M. Grant, Phys. Rev. Lett. 50, 1005 (1983). 10.1103/PhysRevLett.50. 1005
    • (1983) Phys. Rev. Lett. , vol.50 , pp. 1005
    • Grant, P.M.1
  • 18
    • 59749087203 scopus 로고    scopus 로고
    • The Lebed's original suggestion (Ref.) was extended to give the resonance angles θp/q for arbitrary azimuthal plane such as (Refs.) By Bz =cot θp/q sin φ = p q bsinγ csinβsin α -cot α*, regardless of Bx. Here, b, c, β, γ, and α* are lattice parameters and p and q are small integers.
    • The Lebed's original suggestion (Ref.) was extended to give the resonance angles θp/q for arbitrary azimuthal plane such as (Refs.) By Bz =cot θp/q sin φ= p q bsinγ csinβsin α* -cot α*, regardless of Bx. Here, b, c, β, γ, and α* are lattice parameters and p and q are small integers.
  • 23
    • 36148986527 scopus 로고    scopus 로고
    • 10.1103/PhysRevB.76.193103
    • W. Kang, Phys. Rev. B 76, 193103 (2007). 10.1103/PhysRevB.76.193103
    • (2007) Phys. Rev. B , vol.76 , pp. 193103
    • Kang, W.1
  • 33
    • 0000887251 scopus 로고    scopus 로고
    • 10.1103/PhysRevB.57.7423
    • I. J. Lee and M. J. Naughton, Phys. Rev. B 57, 7423 (1998). 10.1103/PhysRevB.57.7423
    • (1998) Phys. Rev. B , vol.57 , pp. 7423
    • Lee, I.J.1    Naughton, M.J.2
  • 34
    • 8644275281 scopus 로고    scopus 로고
    • 10.1103/PhysRevLett.91.187003
    • A. G. Lebed and M. J. Naughton, Phys. Rev. Lett. 91, 187003 (2003). 10.1103/PhysRevLett.91.187003
    • (2003) Phys. Rev. Lett. , vol.91 , pp. 187003
    • Lebed, A.G.1    Naughton, M.J.2


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.