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Volumn 61, Issue 16, 2000, Pages 10929-10940

Coulomb interactions and delocalization in quantum Hall constrictions

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EID: 16344387698     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.61.10929     Document Type: Article
Times cited : (19)

References (50)
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    • See, for example, V. J. Emery, in Highly Conducting One-Dimensional Solids, edited by J. T. Devreese, R. P. Evrard, and V. E. van Doren (Plenum Press, New York, 1979), p. 247.
    • (1979) Highly Conducting One-Dimensional Solids , pp. 247
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  • 38
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    • The issues of zero-mode quantization are easily resolved in the Hamiltonian formalism. In particular, it was used in a similar problem by Y. Oreg and A. M. Finkel’stein, Phys. Rev. Lett. 74, 3668 (1995). However, with nonlocal interactions in complicated geometries, we find it more convenient to use the path integral formalism.
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    • Oreg, Y.1    Finkel’stein, A.2
  • 40
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    • As a result, the zero-mode quantization is identical to that in the Hamiltonian formalism. Thus, the action (2) produces the same finite-size correlation functions as obtained previously, e.g., by V. L. Pokrovsky and L. P. Pryadko, Phys. Rev. Lett. 72, 124 (1994).
    • (1994) Phys. Rev. Lett. , vol.72 , pp. 124
    • Pokrovsky, V.1    Pryadko, L.2


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.