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Volumn 70, Issue 1, 2004, Pages

Feshbach resonances with large background scattering length: Interplay with open-channel resonances

Author keywords

[No Author keywords available]

Indexed keywords

ALKALI METALS; BINDING ENERGY; BOUNDARY CONDITIONS; EIGENVALUES AND EIGENFUNCTIONS; ELECTROMAGNETIC WAVE SCATTERING; ENERGY ABSORPTION; MOLECULAR STRUCTURE;

EID: 19244365258     PISSN: 10502947     EISSN: None     Source Type: Journal    
DOI: 10.1103/PhysRevA.70.012701     Document Type: Article
Times cited : (72)

References (73)
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    • note
    • Note that virtual-state poles can collide on the negative imaginary k axis and move into the third and fourth quadrants of the complex k plane; see, e.g., [37]. However, these poles are located sufficiently far from the real k axis, such that they can be included in the background part of the scattering matrix.
  • 45
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    • note
    • Note that similar behavior was found in the case of dipolemodified s-wave scattering of low-energy electrons from weakly dipolar molecules [40]. However, the physical mechanism responsible for this behavior is different, and the open channel studied in this reference does not contain a potential resonance. Moreover, in contrast to our approach, the work in this reference is based on a phenomenological parametrization of the decay width Γ(E).
  • 48
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    • note
    • n and without a cutoff, the Jost function has a branch point at the origin; see, e.g., [40,43], Within the finite-range approximation the Jost function is an entire function of k.
  • 52
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    • note
    • P 1 is not satisfied. This is related to the fact that the background part summarizes the effect of all distant poles and consists of a sum over these pole contributions. All these contributions are linear in k in the energy domain under consideration and so is their sum.
  • 53
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    • note
    • Note that the energy E can be any (complex) energy in this case, and it is not necessary to include the extra term iδ approaching zero. This small imaginary term only has to be included when calculating the physical scattering states, defined for real and positive energies E (see, for instance, Ref. [44]).
  • 54
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