2005
DOI: 10.1016/j.physrep.2005.04.005
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Electron and photon scattering on three-nucleon bound states

Abstract: A big spectrum of processes induced by real and virtual photons on the 3 He and 3 H nuclei is theoretically investigated through many examples based on nonrelativistic Faddeev calculations for bound and continuum states. The modern nucleon-nucleon potential AV18 together with the threenucleon force UrbanaIX is used. The single nucleon current is augmented by explicit π-and ρ-like two-body currents which fulfill the current continuity equation together with the corresponding parts of the AV18 potential. We also… Show more

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Cited by 129 publications
(228 citation statements)
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References 287 publications
(464 reference statements)
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“…In the second case, we have three free nucleons in the final state and their asymptotic relative motions are represented by p and q. In order to calculate the crucial matrix elements N µ given in (4.1), it is not necessary to solve the corresponding Faddeev equations directly for the 3N scattering states [11]. Instead, we solve a Faddeev-type equation for an auxiliary state | U .…”
Section: Two-pion Exchange Currents In the 3n Systemmentioning
confidence: 99%
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“…In the second case, we have three free nucleons in the final state and their asymptotic relative motions are represented by p and q. In order to calculate the crucial matrix elements N µ given in (4.1), it is not necessary to solve the corresponding Faddeev equations directly for the 3N scattering states [11]. Instead, we solve a Faddeev-type equation for an auxiliary state | U .…”
Section: Two-pion Exchange Currents In the 3n Systemmentioning
confidence: 99%
“…For details about the solution of Eqs (4.3)-(4.4), see Ref. [11]. It is important to mention that these equations are solved in the partial wave basis.…”
Section: Two-pion Exchange Currents In the 3n Systemmentioning
confidence: 99%
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“…Compared to elastic scattering, a new dynamical ingredient, namely the electromagnetic current operator j μ , enters the calculation. The transition amplitude for radiative capture can be obtained via time reversal symmetry from the transition amplitude N Nd μ for two-body photodisintegration of the corresponding 3N bound state, γ + 3 He → p + d in our case [8,9].…”
Section: The Radiative Proton-deuteron Capture Reactionmentioning
confidence: 99%
“…In the following, we use the Siegert theorem to include implicitly many-body electromagnetic current operators (see [8,9] for more details).…”
Section: The Radiative Proton-deuteron Capture Reactionmentioning
confidence: 99%