메뉴 건너뛰기




Volumn 81, Issue 17, 2010, Pages

Superconducting resistive transition in coupled arrays of 4 Å carbon nanotubes

Author keywords

[No Author keywords available]

Indexed keywords


EID: 77955457566     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.81.174530     Document Type: Article
Times cited : (40)

References (55)
  • 2
    • 0001158846 scopus 로고
    • 10.1103/PhysRevLett.17.1133;
    • D. Mermin and H. Wagner, Phys. Rev. Lett. 17, 1133 (1966) 10.1103/PhysRevLett.17.1133
    • (1966) Phys. Rev. Lett. , vol.17 , pp. 1133
    • Mermin, D.1    Wagner, H.2
  • 3
    • 33750016779 scopus 로고
    • 10.1103/PhysRev.158.383
    • P. C. Hohenberg, Phys. Rev. 158, 383 (1967). 10.1103/PhysRev.158.383
    • (1967) Phys. Rev. , vol.158 , pp. 383
    • Hohenberg, P.C.1
  • 10
    • 44049118760 scopus 로고
    • 10.1016/0144-2449(92)90022-H
    • W. M. Meier and D. H. Olson, Zeolites 12, 1 (1992). 10.1016/0144-2449(92) 90022-H
    • (1992) Zeolites , vol.12 , pp. 1
    • Meier, W.M.1    Olson, D.H.2
  • 15
    • 84875846115 scopus 로고    scopus 로고
    • 10.1103/PhysRevB.66.115416
    • H. J. Liu and C. T. Chan, Phys. Rev. B 66, 115416 (2002). 10.1103/PhysRevB.66.115416
    • (2002) Phys. Rev. B , vol.66 , pp. 115416
    • Liu, H.J.1    Chan, C.T.2
  • 16
    • 77955453422 scopus 로고    scopus 로고
    • Both samples shown here differ from the one whose electrical resistance vs temperature was shown in Ref., which reflects the behavior of a 1D (fluctuating) superconducting bundle that presumably acts as the critical link bridging the conducting path
    • Both samples shown here differ from the one whose electrical resistance vs temperature was shown in Ref., which reflects the behavior of a 1D (fluctuating) superconducting bundle that presumably acts as the critical link bridging the conducting path.
  • 17
  • 19
    • 33749159475 scopus 로고    scopus 로고
    • 10.1103/PhysRevB.72.014512
    • T. Z. Qian, W. Q. Ren, and P. Sheng, Phys. Rev. B 72, 014512 (2005). 10.1103/PhysRevB.72.014512
    • (2005) Phys. Rev. B , vol.72 , pp. 014512
    • Qian, T.Z.1    Ren, W.Q.2    Sheng, P.3
  • 23
    • 0001164469 scopus 로고
    • 10.1103/PhysRevB.36.3651
    • A. Kampf and G. Schon, Phys. Rev. B 36, 3651 (1987). 10.1103/PhysRevB.36. 3651
    • (1987) Phys. Rev. B , vol.36 , pp. 3651
    • Kampf, A.1    Schon, G.2
  • 27
  • 33
    • 0001174813 scopus 로고
    • 10.1103/PhysRevB.42.6827
    • H. Q. Ding and M. S. Makivic, Phys. Rev. B 42, 6827 (1990). 10.1103/PhysRevB.42.6827
    • (1990) Phys. Rev. B , vol.42 , pp. 6827
    • Ding, H.Q.1    Makivic, M.S.2
  • 36
    • 77955435368 scopus 로고    scopus 로고
    • As the occupation fraction for the superconducting nanotubes in the transverse plane must be less than 100%, it remains an open possibility that the transition temperature could be dependent on the fraction of superconducting nanotubes in the zeolite pores (Refs.)
    • As the occupation fraction for the superconducting nanotubes in the transverse plane must be less than 100%, it remains an open possibility that the transition temperature could be dependent on the fraction of superconducting nanotubes in the zeolite pores (Refs.).
  • 37
    • 0010652268 scopus 로고
    • 10.1103/PhysRevB.45.2883
    • R. Gupta and C. F. Baillie, Phys. Rev. B 45, 2883 (1992). 10.1103/PhysRevB.45.2883
    • (1992) Phys. Rev. B , vol.45 , pp. 2883
    • Gupta, R.1    Baillie, C.F.2
  • 41
    • 3543099749 scopus 로고
    • 10.1103/PhysRevLett.9.266
    • A. K. Clogston, Phys. Rev. Lett. 9, 266 (1962). 10.1103/PhysRevLett.9.266
    • (1962) Phys. Rev. Lett. , vol.9 , pp. 266
    • Clogston, A.K.1
  • 43
    • 33747876356 scopus 로고
    • 10.1103/PhysRev.135.A550
    • P. Fulde and R. A. Ferrell, Phys. Rev. 135, A550 (1964). 10.1103/PhysRev.135.A550
    • (1964) Phys. Rev. , vol.135 , pp. 550
    • Fulde, P.1    Ferrell, R.A.2
  • 51
    • 42749102953 scopus 로고    scopus 로고
    • 10.1103/PhysRevB.70.014508
    • A. De Martino and R. Egger, Phys. Rev. B 70, 014508 (2004). 10.1103/PhysRevB.70.014508
    • (2004) Phys. Rev. B , vol.70 , pp. 014508
    • De Martino, A.1    Egger, R.2
  • 53
    • 77955433342 scopus 로고    scopus 로고
    • In Refs., the mentioned BKT transition refers to the binding-unbinding transition of quantum phase slips of opposite helicities so that a zero-resistance state becomes possible even in a 1D superconducting wire. This is in contrast to the BKT transition in the transverse plane that mediates a 1D to 3D crossover
    • In Refs., the mentioned BKT transition refers to the binding-unbinding transition of quantum phase slips of opposite helicities so that a zero-resistance state becomes possible even in a 1D superconducting wire. This is in contrast to the BKT transition in the transverse plane that mediates a 1D to 3D crossover.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.