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 $L_n^{(1)}(x$). Here we first calculate the $q$th-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 $F_A^{(2q+1)}(\frac{1}{q},...,\frac{1}{q},1)$ by use
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 $L_n^{(1)}(x$). Here we first calculate the $q$th-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 $F_A^{(2q+1)}(\frac{1}{q},...,\frac{1}{q},1)$ by use
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Papers by Juan Omiste