A new perspective on the?-? contribution to charge-symmetry violation in the nucleon-nucleon force

1992 ◽  
Vol 12 (2-4) ◽  
pp. 123-132 ◽  
Author(s):  
T. Goldman ◽  
J. A. Henderson ◽  
A. W. Thomas
1981 ◽  
Vol 24 (9) ◽  
pp. 2539-2541 ◽  
Author(s):  
A. W. Thomas ◽  
P. Bickerstaff ◽  
A. Gersten

Universe ◽  
2021 ◽  
Vol 7 (6) ◽  
pp. 203
Author(s):  
Peter Shternin ◽  
Isaac Vidaña

We consider transport properties of the hypernuclear matter in neutron star cores. In particular, we calculate the thermal conductivity, the shear viscosity, and the momentum transfer rates for npΣ−Λeμ composition of dense matter in β–equilibrium for baryon number densities in the range 0.1–1 fm−3. The calculations are based on baryon interactions treated within the framework of the non-relativistic Brueckner-Hartree-Fock theory. Bare nucleon-nucleon (NN) interactions are described by the Argonne v18 phenomenological potential supplemented with the Urbana IX three-nucleon force. Nucleon-hyperon (NY) and hyperon-hyperon (YY) interactions are based on the NSC97e and NSC97a models of the Nijmegen group. We find that the baryon contribution to transport coefficients is dominated by the neutron one as in the case of neutron star cores containing only nucleons. In particular, we find that neutrons dominate the total thermal conductivity over the whole range of densities explored and that, due to the onset of Σ− which leads to the deleptonization of the neutron star core, they dominate also the shear viscosity in the high density region, in contrast with the pure nucleonic case where the lepton contribution is always the dominant one.


1982 ◽  
Vol 115 (3) ◽  
pp. 171-173 ◽  
Author(s):  
L.N. Bogdanova ◽  
V.E. Markushin ◽  
V.S. Melezhik ◽  
L.I. Ponomarev

1992 ◽  
Vol 07 (32) ◽  
pp. 3037-3043 ◽  
Author(s):  
T. GOLDMAN ◽  
J.A. HENDERSON ◽  
A.W. THOMAS

In generating a charge-symmetry breaking potential using ρ-ω mixing it is usually assumed that the mixing amplitude is constant (at the on-mass-shell value). Since the exchanged meson is actually far off-shell one must question the validity of this assumption. By constructing a simple quark model in which the mixing is generated by the u-d quark mass difference, we find that the assumption seems to be a very poor one.


1970 ◽  
Vol 32 (7) ◽  
pp. 591-595 ◽  
Author(s):  
D. Gogny ◽  
P. Pires ◽  
R. De Tourreil

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