WebM C K A I G Department of Mathematics, Tidewater Community College Virginia Beach, VA 23456, U.S.A. (Received August 1996; accepted October 1996) A b s t r a c t - - U s i n g the first Born approximation, properties of the scattering phase shift are inves- tigated for waves that are scattered by a schematic representation of a large-scale "stellar potential," i.e., … WebExcept at zero energy, σ peaks in the forward direction (θ = 0) and decreases monotonically as θ varies from 0 to π (Fig. 14.18). Note that, within the Born approximation, the differential crosssection is independent of the sign of V_{0} , and gives the same result if the Yukawa potential is attractive (V_{0}\lt 0) or repulsive (V_{0}\gt 0) .
Non-Local Potentials and Two-Body Scattering - JSTOR
WebPhase-equivalent potentials using SUSY transformations M. Majumder, U. Laha Physics Pramana 2024 The approximate phase-equivalent potentials to Manning–Rosen one are constructed using supersymmetric algebra. Using supersymmetric factorisation method, four SUSY transformations… Expand 1 Highly Influenced View 4 excerpts, cites … WebIn this project, we combined two non-periodic potentials (spin-orbit and RF coupling) to generate a periodic lattice potential known as Zeeman lattice. We investigated the lattice dynamics with experiments like Bloch oscillations, band spectroscopy and Kapitza-Dirac scattering. This work shows that the Zeeman lattice provides robust methods for ... how did they make the lightsaber sound
Yukawa potential - Wikipedia
Web12 Apr 2024 · For each of the considered s-wave scattering length, we studied in detail the characteristics of the built RW solutions in the context of BEC system with loss/gain of atoms. We have showed how the solution parameters and parameter \(g\left( t\right) \) of the two-body interatomic interaction can be used for manipulating first- and second-order … Web5 Sep 2014 · Finite potentials will be dealt with Þrst: those for which V(R)=0forR ! Rn, where Rn is the Þnite range of the potential. This excludes Coulomb potentials, which will be dealt with later. We will examine the solutions at positive energy of the time-independent Schrod¬ inger equation with this potential, and show how to Þn d the scattering Webfrom the scattering region are found. The phase-shifts at are independent of energy and for large I to go to zero as (21+ 1)-1. I. INTRODUCTION ... potentials, so for scattering at … how did they make ice cream before freezers