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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Main Author: Mukeru, Bahati
Other Authors: Lekala, Mantile Leslie
Format: Others
Language:en
Published: 2013
Subjects:
Online Access:http://hdl.handle.net/10500/8909
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spelling 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.
collection NDLTD
language en
format Others
sources NDLTD
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
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