2004
DOI: 10.1142/s0217732304013799
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Bound State Wave Functions Through the Quantum Hamilton–jacobi Formalism

Abstract: The bound state wave functions for a wide class of exactly solvable potentials are found utilizing the quantum Hamilton-Jacobi formalism of Leacock and Padgett. It is shown that, exploiting the singularity structure of the quantum momentum function, until now used only for obtaining the bound state energies, one can straightforwardly find both the eigenvalues and the corresponding eigenfunctions. After demonstrating the working of this approach through a few solvable examples, we consider Hamiltonians, which e… Show more

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Cited by 50 publications
(71 citation statements)
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“…Even though this approach appears similar to the familiar WKB scheme, it is worth pointing out that Eq. (13) reproduces the exact quantized energy eigenvalues [10]. Let us now apply the above formalism of quantum cosmology, as an example, to the flat FLRW minisuperspace model with perfect fluid as the matter field.…”
Section: Introductionmentioning
confidence: 90%
“…Even though this approach appears similar to the familiar WKB scheme, it is worth pointing out that Eq. (13) reproduces the exact quantized energy eigenvalues [10]. Let us now apply the above formalism of quantum cosmology, as an example, to the flat FLRW minisuperspace model with perfect fluid as the matter field.…”
Section: Introductionmentioning
confidence: 90%
“…From the above equation we can see that q ℓ has a simple pole at the origin along with 2ℓ fixed poles corresponding to the zeros of ξ ℓ (x 2 ; g). An important feature of all known ES models studied has been that the point at infinity is an isolated singularity [10]. The consequence of this is that the QMF has finite number of moving poles.…”
Section: Deformed Radial Oscillator Potentialsmentioning
confidence: 99%
“…The advantage of this method is that it is possible to determine the energy eigenvalues without having to solve for the eigenfunctions. In this formalism, singularity structure of the quantum momentum function There is a boundary condition in the limit QMF which is used to determine physically acceptable solutions for the QMF [29][30][31][32][33][34][35][36][37]. In the applications, Ranjani and her collaborators applied the QHJ formalism, to Hamiltonians with Khare-Mandal potential and Scarf potential, characterized by discrete parity and time reversal (PT) symmetries [31].…”
Section: Introductionmentioning
confidence: 99%