Three-body breakup within the fully discretized Faddeev equations
Ol'ga Andreevna Rubtsova, V. N. Pomerantsev, Vladimir Iosifovich Kukulin, Amand Faessler
Abstract
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Ol'ga Andreevna Rubtsova, V. N. Pomerantsev, Vladimir Iosifovich Kukulin, Amand Faessler
Abstract
Open-access reader
A novel approach is developed to find the three-body breakup amplitudes and cross sections within the modified Faddeev equation framework. The method is based on the latticelike discretization of the three-body continuum with a three-body stationary wave-packet basis in momentum space. The approach makes it possible to simplify drastically all the three- and few-body breakup calculations due to discrete representation for the few-body continuum and lattice representation for all the scattering operators entering the integral equation kernels. As a result, the few-body breakup can be treated as a particular case of multichannel scattering in which part of the channels represents the true few-body continuum states. As an illustration for the novel approach, an accurate calculations for the three-body breakup process $n+d\ensuremath{\rightarrow}n+n+p$ with nonlocal and local $NN$ interactions are calculated. The results obtained reproduce nicely the benchmark calculation results using the traditional Faddeev scheme which requires much more tedious and time-consuming calculations.
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A novel approach is developed to find the three-body breakup amplitudes and cross sections within the modified Faddeev equation framework. The method is based on the latticelike discretization of the three-body continuum with a three-body stationary wave-packet basis in momentum space. The approach makes it possible to simplify drastically all the three- and few-body breakup calculations due to discrete representation for the few-body continuum and lattice representation for all the scattering operators entering the integral equation kernels. As a result, the few-body breakup can be treated as a particular case of multichannel scattering in which part of the channels represents the true few-body continuum states. As an illustration for the novel approach, an accurate calculations for the three-body breakup process $n+d\ensuremath{\rightarrow}n+n+p$ with nonlocal and local $NN$ interactions are calculated. The results obtained reproduce nicely the benchmark calculation results using the traditional Faddeev scheme which requires much more tedious and time-consuming calculations.
Key concepts: Breakup, Faddeev equations, Discretization, Three-body problem, Physics, Classical mechanics, Scattering, Few-body systems