메뉴 건너뛰기




Volumn 79, Issue 7, 2009, Pages

Single-walled carbon nanotube weak links in Kondo regime with zero-field splitting

Author keywords

[No Author keywords available]

Indexed keywords


EID: 61949237440     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.79.073404     Document Type: Article
Times cited : (18)

References (37)
  • 17
    • 61949324657 scopus 로고    scopus 로고
    • (reprinted in C. W. J. Beenakker and H. van Houten, arXiv:cond-mat/ 0111505)
    • (reprinted in C. W. J. Beenakker and H. van Houten, arXiv:cond-mat/ 0111505).
  • 21
    • 3242766924 scopus 로고    scopus 로고
    • Quantitive discussion on the slope of NDR has to include the competition of EC and EJ together with MAR current of the Josephson junction. See, e.g. 10.1016/j.ssc.2004.05.031
    • Quantitive discussion on the slope of NDR has to include the competition of EC and EJ together with MAR current of the Josephson junction. See, e.g., E. Vecino, M. R. Buitelaar, A. Martín-Rodero, C. Schönenberger, and A. Levy Yeyati, Solid State Commun. 131, 625 (2004). 10.1016/j.ssc.2004.05.031
    • (2004) Solid State Commun. , vol.131 , pp. 625
    • Vecino, E.1    Buitelaar, M.R.2    Martín-Rodero, A.3    Schönenberger, C.4    Levy Yeyati, A.5
  • 22
    • 0013085021 scopus 로고    scopus 로고
    • This value does not include the effect of finite length of the nanotube, which would suppress the maximum I0 a bit. See, e.g., 10.1103/PhysRevB.65.184507
    • This value does not include the effect of finite length of the nanotube, which would suppress the maximum I0 a bit. See, e.g., A. V. Galaktionov and A. D. Zaikin, Phys. Rev. B 65, 184507 (2002). 10.1103/PhysRevB.65.184507
    • (2002) Phys. Rev. B , vol.65 , pp. 184507
    • Galaktionov, A.V.1    Zaikin, A.D.2
  • 24
    • 61949327543 scopus 로고    scopus 로고
    • When NDR exists, we extract ICM from the local current maximum I CMp and minimum I CMn using ICM = (I CMp - I CMn) /2. Around the Kondo resonance peaks without NDR, ICM is obtained using the averaged voltages, V CMp ̄ and V CMn ̄, respectively, of the I CMp and I CMn peak positions at lower ICM, and taking ICM = I (V CMp ̄) -I (V CMn ̄) /2.
    • When NDR exists, we extract ICM from the local current maximum I CMp and minimum I CMn using ICM = (I CMp - I CMn) /2. Around the Kondo resonance peaks without NDR, ICM is obtained using the averaged voltages, V CMp ̄ and V CMn ̄, respectively, of the I CMp and I CMn peak positions at lower ICM, and taking ICM = I (V CMp ̄) -I (V CMn ̄) /2.
  • 34
    • 11944271804 scopus 로고
    • 10.1103/PhysRevLett.75.1831
    • D. Averin and A. Bardas, Phys. Rev. Lett. 75, 1831 (1995). 10.1103/PhysRevLett.75.1831
    • (1995) Phys. Rev. Lett. , vol.75 , pp. 1831
    • Averin, D.1    Bardas, A.2


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.