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Volumn 247, Issue 11-12, 2010, Pages 2968-2973

1D goes 2D: A Berezinskii-Kosterlitz-Thouless transition in superconducting arrays of 4-Angstrom carbon nanotubes

Author keywords

1D to 3D crossover; Berezinskii Kosterlitz Thouless transition; Nanotubes; Superconductivity

Indexed keywords

CURRENT VOLTAGE CHARACTERISTICS; DROPS; ELECTRON ENERGY ANALYZERS; NANOTUBES; SUPERCONDUCTIVITY; ZEOLITES;

EID: 78649707769     PISSN: 03701972     EISSN: 15213951     Source Type: Journal    
DOI: 10.1002/pssb.201000151     Document Type: Article
Times cited : (2)

References (39)
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    • Sov. Phys. JETP, 34, 610, 1972).
    • V. L. Berezinskii, Sov. Phys. JETP 32, 493 (1971); Sov. Phys. JETP 34, 610 (1972).
    • (1971) Sov. Phys. JETP , vol.32 , pp. 493
    • Berezinskii, V.L.1
  • 12
    • 84878988852 scopus 로고    scopus 로고
    • The samples were prepared in the same manner as that described in [3].
    • The samples were prepared in the same manner as that described in [3].
  • 13
    • 84878999131 scopus 로고    scopus 로고
    • This sample differs from the one whose electrical resistance vs. temperature was shown [3], which reflects the behavior of a 1D (fluctuating) superconducting bundle that presumably acts as the critical link bridging the conducting path.
    • This sample differs from the one whose electrical resistance vs. temperature was shown [3], which reflects the behavior of a 1D (fluctuating) superconducting bundle that presumably acts as the critical link bridging the conducting path.
  • 18
    • 0004255870 scopus 로고    scopus 로고
    • Introduction to Superconductivity
    • second ed. MGH, New York, chap. 4.
    • M. Tinkham, Introduction to Superconductivity, second ed. (MGH, New York, 1996), chap. 4.
    • (1996)
    • Tinkham, M.1
  • 30
    • 84878996975 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 [38,39] of superconducting nanotubes in the zeolite pores.
    • 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 [38, 39] of superconducting nanotubes in the zeolite pores.
  • 35
    • 84878988326 scopus 로고    scopus 로고
    • In references [14-17], 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 references [14-17], 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.
  • 39
    • 0001399398 scopus 로고
    • Phys. Rev. Lett., 11, 104 1963).
    • V. Ambegaokar and A. Baratoff, Phys. Rev. Lett. 10, 486 (1963); Phys. Rev. Lett. 11, 104 (E) (1963).
    • (1963) Phys. Rev. Lett. , vol.10 , Issue.E , pp. 486
    • Ambegaokar, V.1    Baratoff, A.2


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.