Treatment of the two-body Coulomb problem as a short-range potential (original) (raw)

Scattering theory with the Coulomb potential

Journal of Physics: Conference Series, 2009

Basic features of a new surface-integral formulation of scattering theory are outlined. This formulation is valid for both short-range and Coulombic longe-range interactions. New general definitions for the potential scattering amplitude are given. For the Coulombic potentials the generalized amplitude gives the physical on-shell amplitude without recourse to a renormalization procedure. New post and prior forms for the amplitudes of breakup, direct and rearrangement scattering in a Coulomb three-body system are presented.

On the high-energy behaviour of scattering phase shifts for Coulomb-like potentials

Journal of Physics A: Mathematical and General, 1980

We discuss the high-energy behaviour of scattering phase shifts for a large class of spherically symmetric Coulomb-like potentials. Some results which have been known only for short-range potentials are extended to this larger class. In particular, by iterating appropriate Volterra integral equations we derive an asymptotic expression for the phase shifts, which is valid whenever the short-range part of the potential is integrable. When applying our results to the problem of the interference between Coulomb and shortrange interactions we obt64n an estimate for the high-energy behaviour of the Coulombinterference effect in the phase shifts.

The Coulomb problem in nonrelativistic scattering theory

Nuclear Physics A, 1987

Selected papers in the nonrelativistic quantum scattering theory o£ charged particles are reviewed. The emphasis is on the numerical results o£ the past few years and the fundamental theoretical issues they raise. I.

Scattering by potentials with Coulomb Tails

Il Nuovo Cimento A (1971-1996), 1975

An earlier study of the Coulomb partial-wave series and of the connection between screened and unscreened Coulomb potentials is extended to potentials made up of a Coulomb potential plus an arbitrary short-range part y".r-(r). The partial-wave series for the contribution of Y".r-is shown to converge pointwise, for all 8, provided y".r. is 0(,.-3-8) asr-+ 00.

Nonasymptotic analysis of relativistic electron scattering in the Coulomb field

Physical Review A, 2010

It is shown that the conventional Born series for relativistic electron scattering in the Coulomb field cannot be used for calculating the scattering characteristics. The differential cross section at small scattering angles is found on the basis of the Furry-Sommerfeld-Maue solution of the Dirac equation. Propagation of the electron wave packet is considered in order to separate the incident and scattered fluxes. It is shown that the total scattering cross section proves to be finite but depends on the distance r between the scattering center and the observation point. It is also shown that the polarization characteristics of the scattered beam are changed due to the long-range character of the Coulomb potential. The results can be important because Coulomb scattering is often used for normalization of experimental data in high-energy physics.

Analytic properties of three-body continuum Coulomb wave functions

Physical Review A, 2000

We study the analytic properties of the functions known as C3 and ⌽ 2 , used in atomic collision theory for the description of the three-body continuum state. We analyze the bound states for both models obtained by analytic continuation in the case of ion-atom collision. The C3 wave function is an uncorrelated model represented by the product of two-body Coulomb functions and the bound states are found for negative relative energies of electron-target or electron-projectile pairs. On the other hand, the ⌽ 2 model is based on a twovariable hypergeometric function that correlates the electron motion relative to both the target and projectile. We found that only decaying bound states are allowed and the atomic spectra becomes continuous. The bound states of the ⌽ 2 model have a complex energy due to the action of the projectile. Expressions for the wave functions in the different thresholds are given and studied.

Surface-Integral Approach to the Coulomb Few-Body Scattering Problem

19th International Iupap Conference on Few-Body Problems in Physics, 2009

We present main features of a surface-integral approach to the Coulomb few-body scattering problem. This approach is valid for both short-range and Coulombic longe-range interactions. We give new general definitions for the potential scattering amplitude. For the Coulombic potentials the generalized amplitude gives the physical on-shell amplitude without recourse to a renormalization procedure. New post and prior forms for the amplitudes of breakup, direct and rearrangement scattering in a Coulomb three-body system are also presented. The Green's functions and formal solutions of the Schrödinger equation in integral form are not used. Therefore, for the purpose of defining the scattering amplitudes the knowledge of a complicated analytic structure of the Green's function in the complex-energy plane is not required.

Two-body Coulomb problems with sources

Physical Review A, 2010

The two-body Coulomb Schrödinger equation with different types of nonhomogeneities are studied. The particular solution of these nonhomogeneous equations is expressed in closed form in terms of a two-variable hypergeometric function. A particular representation of the latter allows one to study efficiently the solution in the asymptotic limit of large values of the coordinate and hence the associated physics. Simple sources are first considered, and a complete analysis of scattering and bound states is performed. The solutions corresponding to more general (arbitrary) sources are then provided and written in terms of more general hypergeometric functions.

Scattering Amplitude Together with Thermodynamic Properties in the Poschl-Teller Double Ring-Shaped Coulomb Potential

arXiv (Cornell University), 2020

We obtain the exact solution to the Dirac equation with the Pöschl-Teller double ringshaped Coulomb (PTDRSC) potential for any spin-orbit quantum number . The relativistic scattering amplitude for spin 12 particles in the field of this potential has been studied. The wave functions are expressed in terms of the hyper-geometric series of the continuous states on the 2 k  scale. A formula for the phase shifts has also been found. In the nonrelativistic limits, our solution to the Dirac system converges to that of the Schrödinger one. At the high temperature, the partition function is calculated in order to study the behavior of some thermodynamic properties.

Scattering theory for arbitrary potentials

Physical Review A, 2005

The fundamental quantities of potential scattering theory are generalized to accommodate longrange interactions. New definitions for the scattering amplitude and wave operators valid for arbitrary interactions including potentials with a Coulomb tail are presented. It is shown that for the Coulomb potential the generalized amplitude gives the physical on-shell amplitude without recourse to a renormalization procedure.