Bound states for A-body nuclear systems
In this work we calculate the binding energies and root-mean-square radii for A−body nuclear bound state systems, where A ≥ 3. To study three−body systems, we employ the three−dimensional differential Faddeev equations with nucleon-nucleon semi-realistic potentials. The equations are solved numer...
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ndltd-netd.ac.za-oai-union.ndltd.org-unisa-oai-umkn-dsp01.int.unisa.ac.za-10500-89092016-04-16T04:08:18Z Bound states for A-body nuclear systems Mukeru, Bahati Lekala, Mantile Leslie Three−dimensional differential Faddeev equations Potential Harmonic basis Coupled differential equations Orthogonal collocation procedure Eigenvalue equation Restarted Arnoldi Algorithm Renormalized Numerov Method Closed shell nuclei 539.70151535 Bound states (Quantum mechanics) Three-body problem Nuclear physics Mathematical physics Differential equations In this work we calculate the binding energies and root-mean-square radii for A−body nuclear bound state systems, where A ≥ 3. To study three−body systems, we employ the three−dimensional differential Faddeev equations with nucleon-nucleon semi-realistic potentials. The equations are solved numerically. For this purpose, the equations are transformed into an eigenvalue equation via the orthogonal collocation procedure using triquintic Hermite splines. The resulting eigenvalue equation is solved using the Restarted Arnoldi Algorithm. Ground state binding energies of the 3H nucleus are determined. For A > 3, the Potential Harmonic Expansion Method is employed. Using this method, the Schr¨odinger equation is transformed into coupled Faddeev-like equations. The Faddeevlike amplitudes are expanded on the potential harmonic basis. To transform the resulting coupled differential equations into an eigenvalue equation, we employ again the orthogonal collocation procedure followed by the Gauss-Jacobi quadrature. The corresponding eigenvalue equation is solved using the Renormalized Numerov Method to obtain ground state binding energies and root-mean-square radii of closed shell nuclei 4He, 8Be, 12C, 16O and 40Ca. Physics M. Sc. (Physics) 2013-04-11T11:59:24Z 2013-04-11T11:59:24Z 2012-03 Dissertation http://hdl.handle.net/10500/8909 en University of South Africa 1 online resource (ix, 71 leaves) : col. ill. |
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en |
format |
Others
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topic |
Three−dimensional differential Faddeev equations Potential Harmonic basis Coupled differential equations Orthogonal collocation procedure Eigenvalue equation Restarted Arnoldi Algorithm Renormalized Numerov Method Closed shell nuclei 539.70151535 Bound states (Quantum mechanics) Three-body problem Nuclear physics Mathematical physics Differential equations |
spellingShingle |
Three−dimensional differential Faddeev equations Potential Harmonic basis Coupled differential equations Orthogonal collocation procedure Eigenvalue equation Restarted Arnoldi Algorithm Renormalized Numerov Method Closed shell nuclei 539.70151535 Bound states (Quantum mechanics) Three-body problem Nuclear physics Mathematical physics Differential equations Mukeru, Bahati Bound states for A-body nuclear systems |
description |
In this work we calculate the binding energies and root-mean-square radii for A−body
nuclear bound state systems, where A ≥ 3. To study three−body systems, we employ
the three−dimensional differential Faddeev equations with nucleon-nucleon semi-realistic
potentials. The equations are solved numerically. For this purpose, the equations are
transformed into an eigenvalue equation via the orthogonal collocation procedure using
triquintic Hermite splines. The resulting eigenvalue equation is solved using the Restarted
Arnoldi Algorithm. Ground state binding energies of the 3H nucleus are determined.
For A > 3, the Potential Harmonic Expansion Method is employed. Using this method,
the Schr¨odinger equation is transformed into coupled Faddeev-like equations. The Faddeevlike
amplitudes are expanded on the potential harmonic basis. To transform the resulting
coupled differential equations into an eigenvalue equation, we employ again the orthogonal
collocation procedure followed by the Gauss-Jacobi quadrature. The corresponding
eigenvalue equation is solved using the Renormalized Numerov Method to obtain ground
state binding energies and root-mean-square radii of closed shell nuclei 4He, 8Be, 12C, 16O
and 40Ca. === Physics === M. Sc. (Physics) |
author2 |
Lekala, Mantile Leslie |
author_facet |
Lekala, Mantile Leslie Mukeru, Bahati |
author |
Mukeru, Bahati |
author_sort |
Mukeru, Bahati |
title |
Bound states for A-body nuclear systems |
title_short |
Bound states for A-body nuclear systems |
title_full |
Bound states for A-body nuclear systems |
title_fullStr |
Bound states for A-body nuclear systems |
title_full_unstemmed |
Bound states for A-body nuclear systems |
title_sort |
bound states for a-body nuclear systems |
publishDate |
2013 |
url |
http://hdl.handle.net/10500/8909 |
work_keys_str_mv |
AT mukerubahati boundstatesforabodynuclearsystems |
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1718224672283164672 |