GCM Solver (Ver. 3.0): A Mathematica Notebook for Diagonalization of the Geometric Collective Model (Bohr Hamiltonian) with Generalized Gneuss–Greiner Potential
The program diagonalizes the Geometric Collective Model (Bohr Hamiltonian) with generalized Gneuss–Greiner potential with terms up to the sixth power in β . In nuclear physics, the Bohr–Mottelson model with later extensions into the rotovibrational Collective model...
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| Format: | Article |
| Language: | English |
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MDPI AG
2018-08-01
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| Series: | Computation |
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| Online Access: | http://www.mdpi.com/2079-3197/6/3/48 |
| _version_ | 1819089374747295744 |
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| author | Fabrizio Ferrari-Ruffino Lorenzo Fortunato |
| author_facet | Fabrizio Ferrari-Ruffino Lorenzo Fortunato |
| author_sort | Fabrizio Ferrari-Ruffino |
| collection | DOAJ |
| description | The program diagonalizes the Geometric Collective Model (Bohr Hamiltonian) with generalized Gneuss–Greiner potential with terms up to the sixth power in β . In nuclear physics, the Bohr–Mottelson model with later extensions into the rotovibrational Collective model is an important theoretical tool with predictive power and it represents a fundamental step in the education of a nuclear physicist. Nuclear spectroscopists might find it useful for fitting experimental data, reproducing spectra, EM transitions and moments and trying theoretical predictions, while students might find it useful for learning about connections between the nuclear shape and its quantum origin. Matrix elements for the kinetic energy operator and for scalar invariants as β 2 and β 3 cos ( 3 γ ) have been calculated in a truncated five-dimensional harmonic oscillator basis with a different program, checked with three different methods and stored in a matrix library for the lowest values of angular momentum. These matrices are called by the program that uses them to write generalized Hamiltonians as linear combinations of certain simple operators. Energy levels and eigenfunctions are obtained as outputs of the diagonalization of these Hamiltonian operators. |
| first_indexed | 2024-12-21T22:06:55Z |
| format | Article |
| id | doaj.art-59abd9019af641bba700830e3a696fe1 |
| institution | Directory Open Access Journal |
| issn | 2079-3197 |
| language | English |
| last_indexed | 2024-12-21T22:06:55Z |
| publishDate | 2018-08-01 |
| publisher | MDPI AG |
| record_format | Article |
| series | Computation |
| spelling | doaj.art-59abd9019af641bba700830e3a696fe12022-12-21T18:48:40ZengMDPI AGComputation2079-31972018-08-01634810.3390/computation6030048computation6030048GCM Solver (Ver. 3.0): A Mathematica Notebook for Diagonalization of the Geometric Collective Model (Bohr Hamiltonian) with Generalized Gneuss–Greiner PotentialFabrizio Ferrari-Ruffino0Lorenzo Fortunato1Dipartimento di Fisica e Astronomia “G.Galilei”, University Padova, via Marzolo 8, I-35131 Padova, ItalyINFN-Sez.Padova, via Marzolo 8, I-35131 Padova, ItalyThe program diagonalizes the Geometric Collective Model (Bohr Hamiltonian) with generalized Gneuss–Greiner potential with terms up to the sixth power in β . In nuclear physics, the Bohr–Mottelson model with later extensions into the rotovibrational Collective model is an important theoretical tool with predictive power and it represents a fundamental step in the education of a nuclear physicist. Nuclear spectroscopists might find it useful for fitting experimental data, reproducing spectra, EM transitions and moments and trying theoretical predictions, while students might find it useful for learning about connections between the nuclear shape and its quantum origin. Matrix elements for the kinetic energy operator and for scalar invariants as β 2 and β 3 cos ( 3 γ ) have been calculated in a truncated five-dimensional harmonic oscillator basis with a different program, checked with three different methods and stored in a matrix library for the lowest values of angular momentum. These matrices are called by the program that uses them to write generalized Hamiltonians as linear combinations of certain simple operators. Energy levels and eigenfunctions are obtained as outputs of the diagonalization of these Hamiltonian operators.http://www.mdpi.com/2079-3197/6/3/48Bohr Hamiltoniancollective modelquadrupoleBohr–Mottelson modelFrankfurt model |
| spellingShingle | Fabrizio Ferrari-Ruffino Lorenzo Fortunato GCM Solver (Ver. 3.0): A Mathematica Notebook for Diagonalization of the Geometric Collective Model (Bohr Hamiltonian) with Generalized Gneuss–Greiner Potential Computation Bohr Hamiltonian collective model quadrupole Bohr–Mottelson model Frankfurt model |
| title | GCM Solver (Ver. 3.0): A Mathematica Notebook for Diagonalization of the Geometric Collective Model (Bohr Hamiltonian) with Generalized Gneuss–Greiner Potential |
| title_full | GCM Solver (Ver. 3.0): A Mathematica Notebook for Diagonalization of the Geometric Collective Model (Bohr Hamiltonian) with Generalized Gneuss–Greiner Potential |
| title_fullStr | GCM Solver (Ver. 3.0): A Mathematica Notebook for Diagonalization of the Geometric Collective Model (Bohr Hamiltonian) with Generalized Gneuss–Greiner Potential |
| title_full_unstemmed | GCM Solver (Ver. 3.0): A Mathematica Notebook for Diagonalization of the Geometric Collective Model (Bohr Hamiltonian) with Generalized Gneuss–Greiner Potential |
| title_short | GCM Solver (Ver. 3.0): A Mathematica Notebook for Diagonalization of the Geometric Collective Model (Bohr Hamiltonian) with Generalized Gneuss–Greiner Potential |
| title_sort | gcm solver ver 3 0 a mathematica notebook for diagonalization of the geometric collective model bohr hamiltonian with generalized gneuss greiner potential |
| topic | Bohr Hamiltonian collective model quadrupole Bohr–Mottelson model Frankfurt model |
| url | http://www.mdpi.com/2079-3197/6/3/48 |
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