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Volumn 80, Issue 24, 2009, Pages

Hartman effect and spin precession in graphene

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EID: 77954756348     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.80.245433     Document Type: Article
Times cited : (25)

References (23)
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  • 9
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  • 10
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    • The effect discovered by Hartman is superluminality in the L→∞ limit. Since the term "superluminality" is inappropriate for graphene, where all velocities remain well below the speed of light, we avoid this term and speak of the Hartman effect also for finite L
    • The effect discovered by Hartman is superluminality in the L → ∞ limit. Since the term "superluminality" is inappropriate for graphene, where all velocities remain well below the speed of light, we avoid this term and speak of the Hartman effect also for finite L.
  • 11
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    • 10.1016/j.physrep.2006.09.002
    • H. Winful, Phys. Rep. 436, 1 (2006). 10.1016/j.physrep.2006.09.002
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    • Winful, H.1
  • 12
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    • M. I. Katsnelson, Eur. Phys. J. B 51, 157 (2006). 10.1140/epjb/e2006- 00203-1
    • (2006) Eur. Phys. J. B , vol.51 , pp. 157
    • Katsnelson, M.I.1
  • 13
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    • 10.1103/PhysRev.98.145
    • E. P. Wigner, Phys. Rev. 98, 145 (1955). 10.1103/PhysRev.98.145
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  • 14
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    • 10.1103/PhysRev.118.349
    • F. T. Smith, Phys. Rev. 118, 349 (1960). 10.1103/PhysRev.118.349
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    • Smith, F.T.1
  • 15
    • 77954692509 scopus 로고    scopus 로고
    • ) can then be measured as the ratio V3 / V1
    • ) can then be measured as the ratio V 3 / V 1.
  • 23
    • 0038685027 scopus 로고
    • 10.1103/PhysRevB.27.6178
    • M. Büttiker, Phys. Rev. B 27, 6178 (1983). 10.1103/PhysRevB.27.6178
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    • Büttiker, M.1


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.