2002
DOI: 10.1016/s0375-9474(02)00991-0
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Direct Urca processes on nucleons in cooling neutron stars

Abstract: We use the field theoretical model to perform relativistic calculations of neutrino energy losses caused by the direct Urca processes on nucleons in the degenerate baryon matter. By our analysis, the direct neutron decay in the superdense nuclear matter under beta equilibrium is open only due to the isovector meson fields, which create a large energy gap between protons and neutrons in the medium. Our expression for the neutrino energy losses, obtained in the mean field approximation, incorporates the effects … Show more

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Cited by 38 publications
(35 citation statements)
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“…In the rate calculations (3) and (4), E * should be used for the energies in the matrix element and in the energy factors in the denominator, while E should be used in the energy delta function and the Fermi Dirac factors [15,41,42]. However, in the approximation we used for the direct Urca matrix element (7), the E * factors cancel out.…”
Section: A Models Of Nuclear Mattermentioning
confidence: 99%
“…In the rate calculations (3) and (4), E * should be used for the energies in the matrix element and in the energy factors in the denominator, while E should be used in the energy delta function and the Fermi Dirac factors [15,41,42]. However, in the approximation we used for the direct Urca matrix element (7), the E * factors cancel out.…”
Section: A Models Of Nuclear Mattermentioning
confidence: 99%
“…2 we show the results when B = 10 16 G (solid circles) and B = 2 × 10 16 G (open squares) at the baryon density ρ B = ρ 0 (left panel) and ρ B = 2ρ 0 (right panel). in the MU process and direct Urca (DU) process [13] with the dashed and dotted lines, respectively. We confirm again that our results are much larger than those of DU and MU processes.…”
Section: Resultsmentioning
confidence: 99%
“…(2.22) and (2.24) one requires the distribution of neutron number density and the effective mass over the radius of the neutron star's core in beta equilibrium. To calculate these functions we employ the Walecka-type relativistic model of baryon matter [61], where the baryons interact via exchange of σ, ω, and ρ mesons (see details in [62,63]). The functions n n (r) /n 0 and m * n (r) /m n found in this way are shown in The temperature dependence of the cooling rates entering to this equation is of a power law l = qT n with n = 7 for slow neutrino cooling and with n = 5 for axions which corresponds to fast cooling process.…”
Section: (224)mentioning
confidence: 99%