Difference between revisions of "Coming Full Circle With Quantum Hall Explanations"

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==Abstract==
 
==Abstract==
  
The vast majority of attempts at describing how the two quantum Hall effects fit existing theory have started out by viewing the phonemena in a Copenhagen-Schroedinger perspective. In the course of time extraneous adaptations had to be made ranging from fractional charge, composite fermions all the way to a Chern-Simmons 3-forms invoking strings. Yet this step of entering the field now reveals a structural topology not conveyable by statistical Schr?dinger methods. Ironically, the 1- and 2-form components of a physical 3-form used by Kiehn unify integer and fractional effects. More ironic is that this option had already been reported in ref.12 prior to the announced discovery of the fractional effect in 1982.[[Category:Scientific Paper]]
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The vast majority of attempts at describing how the two quantum Hall effects fit existing theory have started out by viewing the phonemena in a Copenhagen-Schroedinger perspective. In the course of time extraneous adaptations had to be made ranging from fractional charge, composite fermions all the way to a Chern-Simmons 3-forms invoking strings. Yet this step of entering the field now reveals a structural topology not conveyable by statistical Schr?dinger methods. Ironically, the 1- and 2-form components of a physical 3-form used by Kiehn unify integer and fractional effects. More ironic is that this option had already been reported in ref.12 prior to the announced discovery of the fractional effect in 1982.
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[[Category:Scientific Paper|coming circle quantum hall explanations]]

Latest revision as of 10:09, 1 January 2017

Scientific Paper
Title Coming Full Circle With Quantum Hall Explanations
Read in full Link to paper
Author(s) Evert Jan Post
Keywords {{{keywords}}}
Published 2008
Journal None
No. of pages 5

Read the full paper here

Abstract

The vast majority of attempts at describing how the two quantum Hall effects fit existing theory have started out by viewing the phonemena in a Copenhagen-Schroedinger perspective. In the course of time extraneous adaptations had to be made ranging from fractional charge, composite fermions all the way to a Chern-Simmons 3-forms invoking strings. Yet this step of entering the field now reveals a structural topology not conveyable by statistical Schr?dinger methods. Ironically, the 1- and 2-form components of a physical 3-form used by Kiehn unify integer and fractional effects. More ironic is that this option had already been reported in ref.12 prior to the announced discovery of the fractional effect in 1982.