2000
DOI: 10.1142/s0217732300000141
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Schrödinger Quantum Modes on the Taub–nut Background

Abstract: The Schrödinger equation is investigated in the Euclidean Taub-NUT geometry. The bound states are degenerate and an extra degeneracy is due to the conserved Runge-Lenz vector. The existence of the extra conserved quantities, quadratic in four-velocities implies the possibility of separating variables in two different coordinate systems. The eigenvalues and the eigenvectors are given in both cases in explicit, closed form.Pacs 04.62.+v *

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Cited by 24 publications
(94 citation statements)
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“…Although the existence of the global solution (26), (30) (with E fixed by (31)) still requires an existence proof, this agrees with the closed form solution known for C = D = 1 [11]. The expansion (30) has only one free coefficient, which is fixed by the normalization condition (14).…”
Section: Numerical Solutionssupporting
confidence: 73%
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“…Although the existence of the global solution (26), (30) (with E fixed by (31)) still requires an existence proof, this agrees with the closed form solution known for C = D = 1 [11]. The expansion (30) has only one free coefficient, which is fixed by the normalization condition (14).…”
Section: Numerical Solutionssupporting
confidence: 73%
“…The radial equation (13) is similar to those of the non-relativistic quantum mechanics apart the term ρ ′′ /ρ . Unfortunately, there is only one solution of the equation (13) known in closed form, corresponding to a GPS monopole background [11] 1 . However, one can analyze the properties of the general solutions by using a combination of analytical and numerical methods, which is enough for most purposes.…”
Section: The Klein-gordon Equationmentioning
confidence: 99%
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“…Moreover, the Taub-NUT geometry possesses four Killing-Yano tensors, f (i) (iϭ1,2,3) and f Y , of valence 2, related to the hidden symmetries of the Taub-NUT geometry reflected by the existence of the nontrivial Stäckel-Killing tensors k (i) . 2,4,7,14 In this Kaluza-Klein geometry there is a pentad gauge fixing 15 where the massless Dirac field, , satisfies a simple gauge-covariant Dirac equation, D " ϭ0, where D " ϭi␥ 0 ‫ץ‬ t ϪD " s . 16,5,7,9 In the standard representation of the Dirac matrices ͓with diagonal ␥ 0 ͑Ref.…”
Section: Preliminariesmentioning
confidence: 99%
“…Moreover, the motion of well-separated monopole-monopole interactions is described approximately by the geodesics of this space [30][31][32][33]. The Euclidean Taub-NUT background contains also interesting specific features of the quantum theory in the case of the scalar fields [34] as well as for Dirac fields of spin-1 2 fermions [35][36][37]. There exist large algebras of conserved observables in both cases [38].…”
mentioning
confidence: 99%