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Volumn 54, Issue 4, 2001, Pages 502-507

Hall state quantization in a rotating frame

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EID: 0035795492     PISSN: 02955075     EISSN: None     Source Type: Journal    
DOI: 10.1209/epl/i2001-00273-1     Document Type: Article
Times cited : (43)

References (17)
  • 2
    • 0004179874 scopus 로고    scopus 로고
    • John Wiley & Sons
    • We remark that in the literature, e.g. in JACKSON J. D., Classical Electrodynamics, third edition (John Wiley & Sons) 1998, what is called the "electromotive force" is actually an electromotive potential, i.e. a line integral of the electromotive field ε along some path. We prefer, for obvious reasons, to call our ε an electromotive force field. Correspondingly, v × B is called the magnetomotive force field.
    • (1998) Classical Electrodynamics, Third Edition
    • Jackson, J.D.1
  • 11
    • 0007293759 scopus 로고    scopus 로고
    • note
    • The fact that one has lΩ ≫ lφ, for any realizable (i.e. nondestructive) rotation speed, was disregarded in [3], where phase coherence was assumed to hold over the entire sample size, rather than over the distance lφ.
  • 12
    • 0007169950 scopus 로고    scopus 로고
    • note
    • Note that, using this argument for the fractional quantum Hall effect in a rotating sample, the number of particles, not their charge, flowing into (or out of) the region enclosed by Γ, were required to be nonintegral if exactly one quantum of flux is turned on.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.