A representation for Jost solutions and an efficient method for solving the spectral problem on the half line (original) (raw)

2019, Mathematical Methods in the Applied Sciences

For the one‐dimensional Schrödinger equation with short‐range potential on a half‐line x>0, the knowledge of the Jost solution e(ρ,x)∼eiρx, Imρ ≥ 0, x→∞ allows one to solve corresponding spectral problems. In the present work, a new series representation for e(ρ,x) is derived with the aid of the Levin formula for the Jost solution and a recently proposed Fourier‐Laguerre series expansion of the integral kernel from the Levin formula. The representation for e(ρ,x) has the form , where, for the coefficients bn(x), a simple recurrent integration procedure is obtained and the parameter belongs to the unit disk. An analogous representation is derived for the derivative of the Jost solution as well.With the aid of the series representations, numerical solution of the classical spectral problem on the half‐line becomes an easy task. Indeed, computation of the eigenvalues reduces to finding zeros of a polynomial for z∈(−1,1). For computing corresponding normalizing constants, a simple fo...

A canonical approach for computing the eigenvalues of the Schrödinger equation for double-well potentials

Canadian Journal of Physics, 2000

The problem of obtaining the eigenvalues of the Schrödinger equation for a double-well potential function is considered. By replacing the differential Schrödinger equation by a Volterra integral equation the wave function will be given by [Formula: see text] where the coefficients ai are obtained from the boundary conditions and the fi are two well-defined canonical functions. Using these canonical functions, we define an eigenvalue function F(E) = 0; its roots E1, E2, ... are the eigenvalues of the corresponding double-well potential. The numerical application to analytical potentials (either symmetric or asymmetric) and to a numerical potential of the (2)1 [Formula: see text] state of the molecule Na2 shows the validity and the high accuracy of the present formulation. PACS No.: 03.65Ge

A Fourier-Bessel Expansion for Solving Radial Schrödinger Equation in Two Dimensions

1997

The spectrum of the two-dimensional Schrodinger equation for polynomial oscillators ¨ bounded by infinitely high potentials, where the eigenvalue problem is defined on a w . finite interval r g 0, L , is variationally studied. The wave function is expanded into a FourierBessel series, and matrix elements in terms of integrals involving Bessel functions are evaluated analytically. Numerical results presented accurate to 30 digits show that, by the time L approaches a critical value, the low-lying state energies behave almost as if the potentials were unbounded.

On The Exact and JWKB Solution of 1D Quantum Harmonic Oscillator by Mathematica

Although being the fundamental semiclassical approximation method mainly used in quantum mechanics and optical waveguides, JWKB method along with the application of the associated JWKB asymptotic matching rules is known to give exact solutions for the Quantum Harmonic Oscillator (QHO). Asymptotically matched JWKB solutions are typically accurate or exact in the entire domain except for a narrow domain around the classical turning points where potential energy equals the total energy of the related quantum mechanical system. So, one has to cope with this diverging behavior at the classical turning points since it prohibits us from using continuity relations at the related boundaries to determine the required JWKB coefficients. Here, a computational diagram and related mathematica codes to surmount the problem by applying parity matching for even and odd JWKB solutions rather than boundary continuities are being presented. In effect, JWKB coefficients as well as the conversion factor for the dimensionless form of the Schrodingers equation, which is common to both exact and JWKB solutions, is being successfully obtained. Content from this work may be used under the terms of the Creative Commons Attribution 3.0 licence. Any further distribution of this work must maintain attribution to the author(s) and the title of the work, journal citation and DOI.

Direct computation of the spectral function

Proceedings of the American Mathematical Society, 1995

We would like to find an explicit formula for the spectral function of the following Sturm-Liouville problem: \[ { L f ≡ − d 2 d x 2 f ( x ) + q ( x ) f ( x ) , x ≥ 0 , f ′ ( 0 ) − m f ( 0 ) = 0. \left \{ {\begin {array}{*{20}{c}} {Lf \equiv - \frac {{{d^2}}}{{d{x^2}}}f(x) + q(x)f(x),\quad x \geq 0,} \hfill \\ {f’(0) - mf(0) = 0.} \hfill \\ \end {array} } \right . \] A simple operational calculus argument will help us obtain an explicit formula for the transmutation kernel. The expression of the spectral function is then obtained through the nonlinear integral equation found in the Gelfand-Levitan theory.

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