1993
DOI: 10.1007/bf01344365
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Green function and scattering amplitudes in many-dimensional space

M. Fabre de la Ripelle

Abstract: Abstract. Methods for solving scattering are studied in many-dimensional space. Green function and scattering amplitudes are given in terms of the required asymptotic behaviour of the wave function. The Born approximation and the optical theorem are derived in many-dimensional space. Phase-shift analyses are performed for hypercentral potentials and for non-hypercentral potentials by use of the hyperspherical adiabatic approximation.

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Cited by 19 publications
(20 citation statements)
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“…Thus, the partial orbital momenta l 1 = l 2 = 0, and the total orbital momentum L = 0. The asymptotic part of the single-channel wave function in the hyperspherical harmonic formalism [49,50] is…”
Section: Wave Functions Of Resonance Statesmentioning
confidence: 99%
“…Thus, the partial orbital momenta l 1 = l 2 = 0, and the total orbital momentum L = 0. The asymptotic part of the single-channel wave function in the hyperspherical harmonic formalism [49,50] is…”
Section: Wave Functions Of Resonance Statesmentioning
confidence: 99%
“…The assumption that antisymmetrization effects between clusters are absent in the asymtptotic region is a natural one. The relative motion problem of the three clusters in the absence of a potential can then be explicitly solved in the Hyperspherical Harmonics (HH) method (see for instance [21][22][23]). It involves the transformation of the Jacobi coordinates q 1 and q 2 to the hyperradius ρ and a set of hyperangles Ω.…”
Section: A Asymptotic Solutions In Coordinate Representationmentioning
confidence: 99%
“…Mass operators of the form (2.7) satisfy all symmetry requirements and are easily diagonalized by means of hyper-spherical harmonics. [4] It is convenient to express the magnitudes r and ρ as functions of the radius R and the auxiliary variable z,…”
Section: The Confining Mass Operatormentioning
confidence: 99%
“…The mass operators considered are sums of a confining term, which depends only on the Jacobi coordinates of the 3-quark system, and a flavor and spin dependent hyperfine correction. The former provides the basic shell structure of the spectrum and is readily diagonalized by means of hyper-spherical harmonics [4]. The latter is built on the observation that a superior description of the baryon spectrum in all flavor generations may be achieved by assuming that the main hyperfine correction should have the flavor-spin structure -i<j λ i · λ j σ i · σ j , which e.g.…”
Section: Introductionmentioning
confidence: 99%