Coming Full Circle With Quantum Hall Explanations: Difference between revisions
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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 | 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 Schrödinger 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|coming circle quantum hall explanations]] | [[Category:Scientific Paper|coming circle quantum hall explanations]] | ||
[[Category:Quantum Theory]] | [[Category:Quantum Theory]] | ||
Latest revision as of 09:17, 22 July 2026
| Scientific Paper | |
|---|---|
| Title | Coming Full Circle With Quantum Hall Explanations |
| Read in full | Link to paper |
| Author(s) | Evert Jan Post |
| Published | 2008 |
| 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 Schrödinger 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.