1999
DOI: 10.1007/978-3-7091-6798-4_13
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Structure of T- and S-Matrices in Unphysical Sheets and Resonances in Three-Body Systems

Abstract: Abstract. Algorithm, based on explicit representations for the analytic continuation of Faddeev components of the three-body T-matrix in unphysical energy sheets, is employed to study mechanism of disappearance and formation of the Efimov levels of the helium 4 He trimer.

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Cited by 6 publications
(5 citation statements)
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“…Apparently, the most detailed numerical study of the nature of the excited state in the 4 He trimer has been performed in [58] (see also [91] and [92]). Notice that the Aziz et al potential [13] was employed in [58] and the number of the partial-wave Faddeev components was reduced to one.…”
Section: On the Efimov Nature Of The 4 He Trimer Excited Statementioning
confidence: 99%
“…Apparently, the most detailed numerical study of the nature of the excited state in the 4 He trimer has been performed in [58] (see also [91] and [92]). Notice that the Aziz et al potential [13] was employed in [58] and the number of the partial-wave Faddeev components was reduced to one.…”
Section: On the Efimov Nature Of The 4 He Trimer Excited Statementioning
confidence: 99%
“…In the framework of the hyperspherical harmonic method and using complex scaling with model potentials a subthreshold 3n resonance for J π = 1/2 − has been located in [11]. Recently mathematical foundations have been laid on the analytical continuation of the three-body Faddeev equations into unphysical energy sheets [12] and an application thereof to the 4 He trimer appeared in [13].…”
Section: Three-nucleon (3n) Resonances Have Not Yet Been Firmly Estabmentioning
confidence: 99%
“…When the scattering length is large and negative, the virtual state turns into a bound state. We studied this mechanism in detail in [11]. In this limit of the large but negative scattering length the linear dependence is again restored.…”
Section: Figmentioning
confidence: 94%
“…In this case, we study graph surfaces of the real and imaginary parts of the scattering matrix S 0 (z) in the domain of its holomorphy (curve 1 on Fig. 2, see for details [11]). The root lines of the functions Re S 0 (z) and Im S 0 (z) presented in Fig.…”
mentioning
confidence: 99%