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http://dx.doi.org/10.1103/physrevc.44.1812 | DOI Listing |
Eur Phys J A Hadron Nucl
October 2024
Institute for Advanced Simulation, Forschungszentrum Jülich, 52425 Jülich, Germany.
Understanding the strong interactions within baryonic systems beyond the up and down quark sector is pivotal for a comprehensive description of nuclear forces. This study explores the interactions involving hyperons, particularly the particle, within the framework of nuclear lattice effective field theory (NLEFT). By incorporating hyperons into the NLEFT framework, we extend our investigation into the sector, allowing us to probe the third dimension of the nuclear chart.
View Article and Find Full Text PDFPhys Rev Lett
March 2024
Department of Physics and Astronomy, University of Manchester, Manchester, United Kingdom.
The fraction of χ_{c1} and χ_{c2} decays in the prompt J/ψ yield, F_{χ_{c}→J/ψ}=σ_{χ_{c}→J/ψ}/σ_{J/ψ}, is measured by the LHCb detector in pPb collisions at sqrt[s_{NN}]=8.16 TeV. The study covers the forward (1.
View Article and Find Full Text PDFPhys Rev Lett
September 2023
Department of Physics and Astronomy, University of Manchester, Manchester, United Kingdom.
Phys Rev Lett
April 2022
Department of Physics and Astronomy, University of Manchester, Manchester, United Kingdom.
Sci Rep
September 2021
Department of Physics, K. N. Toosi University of Technology, Tehran, Iran.
The matrix elements of relativistic nucleon-nucleon (NN) potentials are calculated directly from the nonrelativistic potentials as a function of relative NN momentum vectors, without a partial wave decomposition. To this aim, the quadratic operator relation between the relativistic and nonrelativistic NN potentials is formulated in momentum-helicity basis states. It leads to a single integral equation for the two-nucleon (2N) spin-singlet state, and four coupled integral equations for two-nucleon spin-triplet states, which are solved by an iterative method.
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