Results 171 to 180 of about 200,466 (211)
High-accuracy laser spectroscopy of H 2 + and the proton-electron mass ratio. [PDF]
Alighanbari S +3 more
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Dispersive determination of nucleon gravitational form factors. [PDF]
Cao XH, Guo FK, Li QZ, Yao DL.
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Hypernuclei and baryon-baryon interaction
Russian Physics Journal, 1997A central ΛN potential containing spin and charge dependences is constructed on the basis of an analysis of fundamental hypernuclear data (Λp scattering, the binding energies of the ground and excited states of hypernuclei). The lightest hypernuclei ( Λ 3 H, Λ 4 H, Λ 4 He) are calculated as a system of three or four particles on the basis of the highly
N. N. Kolesnikov, V. I. Tarasov
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Meson-Baryon and Baryon-Baryon Reactions in a Quark Model
Physical Review, 1966An "independent-quark model" for mesons and baryons which recently was applied very successfully to elastic scattering at high energies, is extended to inelastic meson-baryon and baryon-baryon reactions. A number of relations between cross sections are derived, most of which are independent of $\mathrm{SU}(3)$.
H. J. Lipkin, F. Scheck, H. Stern
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Meson-baryon coupling constants and baryon-baryon interactions
Nuclear Physics A, 1998Abstract We present a chiral-invariant SU( 3 ) Lagrangian describing the interactions of the baryon octet with the lowest-mass meson nonets. Empirical estimates for the strengths of these vertices are given. The nonlinear realization of the chiral symmetry generates pair-meson interaction vertices, the coupling constants for which contain no new free
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Baryon-Baryon Interactions and the Eightfold Way*
Physical Review, 1963The deuteron is shown to belong to a ten-dimensional irreducible representation of the group $\mathrm{SU}(3)$ in the symmetry scheme called the eightfold way. The baryon-baryon states, which together with the deuteron comprise this supermultiplet, are studied.
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Recent soft-core baryon–baryon interactions
Nuclear Physics A, 2005Recent results obtained with the extended-soft-core (ESC) interactions are presented. In a unified manner the ESC-model, describes nucleon-nucleon (NN), hyperon-nucleon (YN), and hyperon-hyperon (YY), using (broken) SU F (3)-symmetry. In the ESC approach to baryon-baryon (BB) the dynamics is derived from (i) one-boson-exchanges (OBE), (ii) two-meson ...
Rijken, T.A., Yamamoto, Y.
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