Juan Omiste - Academia.edu (original) (raw)
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Papers by Juan Omiste
International Journal of Quantum Chemistry, 2010
The stationary states of the half-line Coulomb potential are described by quantum-mechanical wave... more The stationary states of the half-line Coulomb potential are described by quantum-mechanical wavefunctions which are controlled by the Laguerre polynomials Ln(1)(xL_n^{(1)}(xLn(1)(x). Here we first calculate the qqqth-order frequency or entropic moments of this quantum system, which is controlled by some entropic functionals of the Laguerre polynomials. These functionals are shown to be equal to a Lauricella function FA(2q+1)(frac1q,...,frac1q,1)F_A^{(2q+1)}(\frac{1}{q},...,\frac{1}{q},1)FA(2q+1)(frac1q,...,frac1q,1) by use
International Journal of Quantum Chemistry, 2010
The stationary states of the half-line Coulomb potential are described by quantum-mechanical wave... more The stationary states of the half-line Coulomb potential are described by quantum-mechanical wavefunctions which are controlled by the Laguerre polynomials Ln(1)(xL_n^{(1)}(xLn(1)(x). Here we first calculate the qqqth-order frequency or entropic moments of this quantum system, which is controlled by some entropic functionals of the Laguerre polynomials. These functionals are shown to be equal to a Lauricella function FA(2q+1)(frac1q,...,frac1q,1)F_A^{(2q+1)}(\frac{1}{q},...,\frac{1}{q},1)FA(2q+1)(frac1q,...,frac1q,1) by use