Antimatter in the Direct-Action Theory of Fields

One of Feynman's greatest contributions to physics was the interpretation of negative energies as antimatter in quantum field theory. A key component of this interpretation is the Feynman propagator, which seeks to describe the behavior of antimatter at the virtual particle level. Ironically, i...

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Main Author: Ruth E. Kastner
Format: Article
Language:English
Published: Quanta 2016-01-01
Series:Quanta
Online Access:http://quanta.ws/ojs/index.php/quanta/article/view/45
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spelling doaj-b835c38388364ee48e9bd759b1c8d33e2020-11-24T22:57:44ZengQuantaQuanta1314-73742016-01-0151121810.12743/quanta.v5i1.4527Antimatter in the Direct-Action Theory of FieldsRuth E. Kastner0University of MarylandOne of Feynman's greatest contributions to physics was the interpretation of negative energies as antimatter in quantum field theory. A key component of this interpretation is the Feynman propagator, which seeks to describe the behavior of antimatter at the virtual particle level. Ironically, it turns out that one can dispense with the Feynman propagator in a direct-action theory of fields, while still retaining the interpretation of negative energy solutions as antiparticles. Quanta 2016; 5: 12–18.http://quanta.ws/ojs/index.php/quanta/article/view/45
collection DOAJ
language English
format Article
sources DOAJ
author Ruth E. Kastner
spellingShingle Ruth E. Kastner
Antimatter in the Direct-Action Theory of Fields
Quanta
author_facet Ruth E. Kastner
author_sort Ruth E. Kastner
title Antimatter in the Direct-Action Theory of Fields
title_short Antimatter in the Direct-Action Theory of Fields
title_full Antimatter in the Direct-Action Theory of Fields
title_fullStr Antimatter in the Direct-Action Theory of Fields
title_full_unstemmed Antimatter in the Direct-Action Theory of Fields
title_sort antimatter in the direct-action theory of fields
publisher Quanta
series Quanta
issn 1314-7374
publishDate 2016-01-01
description One of Feynman's greatest contributions to physics was the interpretation of negative energies as antimatter in quantum field theory. A key component of this interpretation is the Feynman propagator, which seeks to describe the behavior of antimatter at the virtual particle level. Ironically, it turns out that one can dispense with the Feynman propagator in a direct-action theory of fields, while still retaining the interpretation of negative energy solutions as antiparticles. Quanta 2016; 5: 12–18.
url http://quanta.ws/ojs/index.php/quanta/article/view/45
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