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Continuum structure in strong electromagnetic fields

[Pages missing ] In this chapter, the Dirac equation for spherically symmetric potentials is closely examined. Analytical solutions are found for a square well potential, the properties of which will be used later when the equation is solved for arbitrary potentials using numerical methods. The star...

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Main Author: O'Connor, Michael
Format: Thesis
Language:English
Published: Not Specified 2024
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access_status_str Open Access
author O'Connor, Michael
author_browse O'Connor, Michael
author_facet O'Connor, Michael
author_sort O'Connor, Michael
collection Thesis
description [Pages missing ] In this chapter, the Dirac equation for spherically symmetric potentials is closely examined. Analytical solutions are found for a square well potential, the properties of which will be used later when the equation is solved for arbitrary potentials using numerical methods. The starting point is the Dirac equation for stationary states. For convenience, the units are chosen such that h=c=l. However, in explicit calculations, these constants are re-introduced using the prescription hc=197 Mev fm. When the coupling constant a is used, its value is taken as 1/137.
format Thesis
id oai:open.uct.ac.za:11427/40477
institution University of Cape Town (South Africa)
language eng
last_indexed 2026-06-10T12:32:45.765Z
license_str Not specified — see source repository
provenance_str_mv Harvested via OAI-PMH from UCTD — University of Cape Town Open Access Repository
publishDate 2024
publishDateRange 2024
publishDateSort 2024
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record_format dspace
source_str UCTD — University of Cape Town Open Access Repository
spelling oai:open.uct.ac.za:11427/40477 Continuum structure in strong electromagnetic fields O'Connor, Michael Physics [Pages missing ] In this chapter, the Dirac equation for spherically symmetric potentials is closely examined. Analytical solutions are found for a square well potential, the properties of which will be used later when the equation is solved for arbitrary potentials using numerical methods. The starting point is the Dirac equation for stationary states. For convenience, the units are chosen such that h=c=l. However, in explicit calculations, these constants are re-introduced using the prescription hc=197 Mev fm. When the coupling constant a is used, its value is taken as 1/137. 2024-07-23T13:13:23Z 2024-07-23T13:13:23Z 1987 2024-07-19T13:54:31Z Thesis / Dissertation Masters MSc http://hdl.handle.net/11427/40477 eng application/pdf Not Specified Not Specified
spellingShingle Physics
O'Connor, Michael
Continuum structure in strong electromagnetic fields
thesis_degree_str Master's
title Continuum structure in strong electromagnetic fields
title_full Continuum structure in strong electromagnetic fields
title_fullStr Continuum structure in strong electromagnetic fields
title_full_unstemmed Continuum structure in strong electromagnetic fields
title_short Continuum structure in strong electromagnetic fields
title_sort continuum structure in strong electromagnetic fields
topic Physics
url http://hdl.handle.net/11427/40477
work_keys_str_mv AT oconnormichael continuumstructureinstrongelectromagneticfields