28 research outputs found

    Supersymmetry,Shape Invariance and Exactly Solvable Noncentral Potentials

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    Using the ideas of supersymmetry and shape invariance we show that the eigenvalues and eigenfunctions of a wide class of noncentral potentials can be obtained in a closed form by the operator method. This generalization considerably extends the list of exactly solvable potentials for which the solution can be obtained algebraically in a simple and elegant manner. As an illustration, we discuss in detail the example of the potential V(r,θ,ϕ)=ω24r2+δr2+Cr2sin2θ+Dr2cos2θ+Fr2sin2θsin2αϕ+Gr2sin2θcos2αϕV(r,\theta,\phi)={\omega^2\over 4}r^2 + {\delta\over r^2}+{C\over r^2 sin^2\theta}+{D\over r^2 cos^2\theta} + {F\over r^2 sin^2\theta sin^2 \alpha\phi} +{G\over r^2 sin^2\theta cos^2\alpha\phi} with 7 parameters.Other algebraically solvable examples are also given.Comment: 16 page

    The two-body problem of ultra-cold atoms in a harmonic trap

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    We consider two bosonic atoms interacting with a short-range potential and trapped in a spherically symmetric harmonic oscillator. The problem is exactly solvable and is relevant for the study of ultra-cold atoms. We show that the energy spectrum is universal, irrespective of the shape of the interaction potential, provided its range is much smaller than the oscillator length.Comment: Final version accepted for publication in Am. Journ. Phy

    The Fermionic Density-functional at Feshbach Resonance

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    We consider a dilute gas of neutral unpolarized fermionic atoms at zero temperature.The atoms interact via a short range (tunable) attractive interaction. We demonstrate analytically a curious property of the gas at unitarity. Namely, the correlation energy of the gas, evaluated by second order perturbation theory, has the same density dependence as the first order exchange energy, and the two almost exactly cancel each other at Feshbach resonance irrespective of the shape of the potential, provided (μrs)>>1(\mu r_s) >> 1. Here (μ)−1(\mu)^{-1} is the range of the two-body potential, and rsr_s is defined through the number density n=3/(4πrs3)n=3/(4\pi r_s^3). The implications of this result for universality is discussed.Comment: Five pages, one table. accepted for publication in PR
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