1996
DOI: 10.1103/revmodphys.68.1015
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Multichannel Rydberg spectroscopy of complex atoms

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Cited by 470 publications
(600 citation statements)
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References 461 publications
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“…are radially outgoing/incoming Coulomb spherical waves, as defined in 16 and σ l = arg(Γ(l + 1 − i/k)) is the Coulomb phase shift. To find d q k , it is now necessary to find the superposition ψ k = A lm ( k)ψ E;lm whose outgoing component matches the outgoing component of e i k· x .…”
Section: Scattering States and Ramifications For Molecular Tomographymentioning
confidence: 99%
“…are radially outgoing/incoming Coulomb spherical waves, as defined in 16 and σ l = arg(Γ(l + 1 − i/k)) is the Coulomb phase shift. To find d q k , it is now necessary to find the superposition ψ k = A lm ( k)ψ E;lm whose outgoing component matches the outgoing component of e i k· x .…”
Section: Scattering States and Ramifications For Molecular Tomographymentioning
confidence: 99%
“…Every such threshold has an infinite number of Rydberg levels converging to it. For this reason, the transformed S does not yet represent the physical scattering matrix (Aymar et al 1996). In fact, it represents the actual scattering matrix S phys only in energy ranges where all of the channels |s are open for electron escape, i.e.…”
Section: Mqdt-rft Methodsmentioning
confidence: 99%
“…When at least one channel is closed, the physical scattering matrix S phys is obtained from S using the standard MQDT channel-elimination formula (see Eq. (2.50) in Aymar et al (1996) or Eq. (38) in Kokoouline and Greene (2004) ).…”
Section: Mqdt-rft Methodsmentioning
confidence: 99%
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“…In most systems, several Rydberg series are present in the same energy range, which most likely interact together. Such situations are described with the Multichannel Quantum Defect Theory (MQDT) [1,2,3], which involves quantum defects for each of the p channels and coupling parameters between them, constituting the so-called Y-matrix with dimension p × p [1].…”
Section: Introductionmentioning
confidence: 99%