2012
DOI: 10.1103/physreva.86.052709
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Integral relations and the adiabatic expansion method for1+2reactions above the breakup threshold: Helium trimers with soft-core potentials

Abstract: The integral relations formalism introduced in [P. Barletta et al., Phys. Rev. Lett. 103, 090402 (2009); C. Romero-Redondo et al., Phys. Rev. A 83, 022705 (2011)] and designed to describe 1 + N reactions is extended here to collision energies above the threshold for the target breakup. These two relations are completely general, and in this work they are used together with the adiabatic expansion method for the description of 1 + 2 reactions. The neutron-deuteron breakup, for which benchmark calculations are … Show more

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Cited by 15 publications
(18 citation statements)
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“…To this aim, we make use of the adiabatic expansion method as discussed in Refs. [21,22] for energies below the dimer breakup threshold and recently extended to energies above that threshold [23]. As it is well known, the adiabatic expansion method is a very powerful method used to describe bound states [24].…”
Section: A Elastic and Breakup Cross Sectionsmentioning
confidence: 99%
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“…To this aim, we make use of the adiabatic expansion method as discussed in Refs. [21,22] for energies below the dimer breakup threshold and recently extended to energies above that threshold [23]. As it is well known, the adiabatic expansion method is a very powerful method used to describe bound states [24].…”
Section: A Elastic and Breakup Cross Sectionsmentioning
confidence: 99%
“…[23], where the inelasticity (|S 11 |) and the real part of the phase shift [Re(δ)] have been calculated at selected energies for increasing values of K max (grand-angular quantum number associated to the last adiabatic term included in the expansion of the scattering wave function). The conclusion was that the use of the integral relations produces a pattern of convergence similar to a bound-state calculation.…”
Section: A Elastic and Breakup Cross Sectionsmentioning
confidence: 99%
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“…In the adiabatic hyper-spherical representation of this mass imbalanced three-body system, it happens that the coupling between the lowest adiabatic channel, which asymptotically goes to the atom-dimer channel, with the breakup channels is weak (see e.g. [24]). In addition, asymptotically the lowest adiabatic hyper-spherical potential is attractive, while the breakup channels have a barrier around ρ ∼ |a HL |.…”
mentioning
confidence: 99%
“…[23], which was extended to energies above the breakup threshold in Ref. [24]. The Gaussian potential with r 0 being the interaction range is given by…”
mentioning
confidence: 99%