1997
DOI: 10.1007/s002200050152
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Asymptotics of Rydberg States for the Hydrogen Atom

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Cited by 13 publications
(22 citation statements)
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“…Related heuristic arguments can be found in [28,7]. In the case q = 0 this equivalence is closely related to the Segal-Bargmann transform in appropriate holomorphic spaces which, in one form or another, plays an important role in the semiclassical analysis performed in [34,36,33,35]. Let us comment in more detail on this relation.…”
Section: 3mentioning
confidence: 84%
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“…Related heuristic arguments can be found in [28,7]. In the case q = 0 this equivalence is closely related to the Segal-Bargmann transform in appropriate holomorphic spaces which, in one form or another, plays an important role in the semiclassical analysis performed in [34,36,33,35]. Let us comment in more detail on this relation.…”
Section: 3mentioning
confidence: 84%
“…In our analysis generalized coherent states and associated anti-Wick ΨDOs closely related to the Bargmann representation and the Segal-Bargmann transform appear again in a natural way (see Section 2), although their role is different from the one of their counterparts in [33,36,35]. Although this paper is inspired by [37,33,36,35], much of our construction (see Section 4) is based on the analysis of [22]. In [22] it was proven that for V ∈ C ∞ 0 (R 2 ) the trace in the l.h.s.…”
Section: Semiclassical Interpretation Consider the Classical Hamiltomentioning
confidence: 90%
“…Next, in section 5, we take the semiclassical limit N → ∞ of this last trace by using the Stone-Weierstrass Theorem, the coherent states for the hydrogen atom introduced in [18], and the stationary phase method in order to estimate the expected value of − B 2 hL 3 m , m ∈ N * , between coherent states. We use decay properties of coherent states shown in [18] but, in addition, we need to estimate decay of their derivatives. Finally, an alternate proof of Theorem 1.3 is presented in section 7.…”
Section: Contentsmentioning
confidence: 99%
“…It can be shown that for α ∈ A given, the state D (N +1) 2 Ψ α,N is highly concentrated along the classical orbit in configuration space associated to α by the inverse of the Moser map and the classical flow of the Kepler problem on the energy surface Σ(−1/2). See references [18] and [20] for details. Let us denote byẼ N,j , j = 1, .…”
Section: A Semiclassical Trace Identity For Zeeman Eigenvalue Clustersmentioning
confidence: 99%
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