The alternative to the incompressible fractional charge in the quantum Hall effect: Comments on Laughlin and Schrieffer's papers

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dc.creatorShrivastava, Keshav N.
dc.date2002-10-10
dc.date.accessioned2026-07-07T02:47:41Z
dc.date.available2026-07-07T02:47:41Z
dc.descriptionLaughlin has found "exactly" the wave function which is ascribed to an excitation of fractional charge, such as e/3. We find that the exactness of the wave function is not destroyed by changing the charge to some other quantity such as the magnetic field. Thus e/3 and H can be replaced by e and H/3. Therefore, the wave function need not belong to quasiparticles of charge e/3.
dc.description8 pages TeX
dc.identifierhttps://arxiv.org/abs/cond-mat/0210238
dc.identifierhttp://arxiv.org/abs/cond-mat/0210238
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/20103
dc.subjectMesoscale and Nanoscale Physics
dc.subjectStatistical Mechanics
dc.titleThe alternative to the incompressible fractional charge in the quantum Hall effect: Comments on Laughlin and Schrieffer's papers
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