Bound state equivalent potentials with the Lagrange mesh method
arXiv:physics/0611146 · doi:10.1103/PhysRevE.75.026705
Abstract
The Lagrange mesh method is a very simple procedure to accurately solve eigenvalue problems starting from a given nonrelativistic or semirelativistic two-body Hamiltonian with local or nonlocal potential. We show in this work that it can be applied to solve the inverse problem, namely, to find the equivalent local potential starting from a particular bound state wave function and the corresponding energy. In order to check the method, we apply it to several cases which are analytically solvable: the nonrelativistic harmonic oscillator and Coulomb potential, the nonlocal Yamaguchi potential and the semirelativistic harmonic oscillator. The potential is accurately computed in each case. In particular, our procedure deals efficiently with both nonrelativistic and semirelativistic kinematics.
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References in corpus (9)
- Glueball masses and Pomeron trajectory in nonperturbative QCD
- A consistent derivation of the quark--antiquark and three quark potentials in a Wilson loop context
- Relativistic Harmonic Oscillator
- Semirelativistic potential model for glueball states
- Auxiliary fields and hadron dynamics
- Sizes of Lightest Glueballs in SU(3) Lattice Gauge Theory
- Lagrange mesh, relativistic flux tube, and rotating string
- A mass formula for light mesons from a potential model
- Local and non-local equivalent potentials for p-12C scattering
Cited by in corpus (7)
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- Hyperspherical-coordinate approach to the spectra and decay widths of hybrid quarkonia
- Effective potential between two transverse gluons from lattice QCD