Triton Binding Energy of Kharkov Potential

Kamada, H.; Arslanaliev, A. M.

doi:10.1007/s00601-017-1241-2

Cited by 9 publications

(5 citation statements)

References 38 publications

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“…We will show our calculations in the CPR versus those with the Bonn potential. In this context we have tried to set links between the Kharkov potential built up by using the UCT method and the high-precision covariant one-boson-exchange potentials for the neutron-proton scattering below 350 MeV [7,11,12,14,15].…”

Section: Theory and Experimentsmentioning

confidence: 99%

Untitled

2018

ATCP

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Some recollectionsOne day in the mid-90s after my lecture delivered for experimentalists from the High Energy Physics Dept. of our Center and devoted to the role of meson exchange currents in electromagnetic interactions with nuclei we were discussing a surprising property of atomic nuclei. Namely, when considering any nucleus as a system of interacting meson and nucleon fields we often forget the spring of nuclear forces and prefer to a handle a set of particles that preserve their property to be physical nucleons with specific interactions (rather phenomenological) between them, i.e., coming to the well known contemporary picture.

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Section: Theory and Experimentsmentioning

confidence: 99%

Untitled

2018

ATCP

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“…Currently, the UCT method has been applied in the mesodynamics to the processes that involve interac-tions of the clothed 𝜋, 𝜂, 𝜌, 𝜔, 𝛿, 𝜎 mesons and nucleons [3,[5][6][7][8][9]. The applications of this method in QED and quantum chromodynamics (QCD) are shown in [10][11][12][13].…”

Section: Introductionmentioning

confidence: 99%

A New Family of Interactions between Clothed Particles in QED

Arslanaliev

Kostylenko

2021

Ukr. J. Phys.

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The method of unitary clothing transformations (UCTs) has been applied to the quantum electrodynamics (QED) by using the clothed particle representation (CPR). Within CPR, the Hamiltonian for interacting electromagnetic and electron-positron fields takes the form in which the interaction operators responsible for such two-particle processes as e−e− → e−e−, e+e+ → e+e+, e−e+ → e−e+, e−e+ → yy, yy → e−e+, ye− → ye−, and ye+ → ye+ are obtained on the same physical footing. These novel interactions include the off-energy-shell and recoil effects (the latter without any expansion in (v/c)2-series) and their on-energy shell matrix elements reproduce the well-known results derived within the perturbation theory based on the Dyson expansion for the S-matrix (in particular, the Møller formula for the e−e−-scattering, the Bhabha formula for e−e+-scattering, and the Klein–Nishina one for the Compton scattering).

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“…We have been constructing a relativistic framework in the form of relativistic Faddeev equations [3][4][5][6][7][8][9][10] according to the Bakamjian-Thomas theory [11]. Not only using the realistic nonrelativistic nucleon-nucleon (NN) potentials but using Kharkov relativistic NN potential [12] we obtained the triton wave function by solving the relativistic Faddeev equation [13][14][15]. However, in the three-body scattering states, the relativistic effects appear to be generally small [16,17] and insufficient to significantly improve the data description.…”

Section: Introductionmentioning

confidence: 99%