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[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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| Format: | Thesis |
| Language: | English |
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2024
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| _version_ | 1867613225160278016 |
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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 |
| publisher | Not Specified |
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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 |