scholarly journals New System-Specific Coherent States by Supersymmetric Quantum Mechanics for Bound State Calculations

10.5772/54010 ◽  
2013 ◽  
Author(s):  
Chia-Chun Chou ◽  
Mason T. ◽  
Bernhard G. ◽  
Donald J.
Author(s):  
Jean Vignon Hounguevou ◽  
Daniel Sabi Takou ◽  
Gabriel Y. H. Avossevou

In this paper, we study coherent states for a quantum Pauli model through supersymmetric quantum mechanics (SUSYQM) method. From the point of view of canonical quantization, the construction of these coherent states is based on the very important differential operators in SUSYQM call factorization operators. The connection between classical and quantum theory is given by using the geometric properties of these states.


2020 ◽  
Vol 23 (3) ◽  
Author(s):  
F. Bagarello

Abstract We propose an extended version of supersymmetric quantum mechanics which can be useful if the Hamiltonian of the physical system under investigation is not Hermitian. The method is based on the use of two, in general different, superpotentials. Bi-coherent states of the Gazeau-Klauder type are constructed and their properties are analyzed. Some examples are also discussed, including an application to the Black-Scholes equation, one of the most important equations in Finance.


2004 ◽  
Vol 326 (5-6) ◽  
pp. 315-321 ◽  
Author(s):  
Ying He ◽  
Zhuangqi Cao ◽  
Qishun Shen

2012 ◽  
Vol 45 (50) ◽  
pp. 505302 ◽  
Author(s):  
Chia-Chun Chou ◽  
Mason T Biamonte ◽  
Bernhard G Bodmann ◽  
Donald J Kouri

1985 ◽  
Vol 150 (1-3) ◽  
pp. 159-162 ◽  
Author(s):  
Alain Comtet ◽  
AndréD. Bandrauk ◽  
David K. Campbell

2003 ◽  
Vol 18 (12) ◽  
pp. 853-857
Author(s):  
SUBIR K. BOSE ◽  
AXEL SCHULZE-HALBERG

We improve a result obtained in Ref. 2: In the context of supersymmetric quantum mechanics we present a certain superpotential that yields a trial function we use for the calculation of variational quantum bound state energies of the screened Coulomb potential. We show that for small screening parameters our trial function yields better approximations for the energies than the trial function used in Ref. 2.


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