219 research outputs found

    In-medium enhancement of the modified Urca neutrino reaction rates

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    We calculate modified Urca neutrino emission rates in the dense nuclear matter in neutron star cores. We find that these rates are strongly enhanced in the beta-stable matter in regions of the core close to the direct Urca process threshold. This enhancement can be tracked to the use of the in-medium nucleon spectrum in the virtual nucleon propagator. We describe the in-medium nucleon scattering in the non-relativistic Bruckner-Hartree-Fock framework taking into account two-body as well as the effective three-body forces, although the proposed enhancement does not rely on a particular way of the nucleon interaction treatment. Finally we suggest a simple approximate expression for the emissivity of the n-branch of the modified Urca process that can be used in the neutron stars cooling simulations with any nucleon equation of state of dense matter.Comment: 8 pages, 3 figures; accepted for publication in PLB. In v.2 misprint in eq.(9) corrected and discussion of cooling curves expande

    The γ\gamma-ray pulsar J0633+0632 in X-rays

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    We analysed Chandra observations of the bright Fermi pulsar J0633+0632 and found evidence of an absorption feature in its spectrum at 80426+42804^{+42}_{-26} eV (the errors here and below are at 90% confidence) with equivalent width of 6336+4763^{+47}_{-36} eV. In addition, we analysed in detail the X-ray spectral continuum taking into account correlations between the interstellar absorption and the distance to the source. We confirm early findings by Ray et al. (2011) that the spectrum contains non-thermal and thermal components. The latter is equally well described by the blackbody and magnetised atmosphere models and can be attributed to the emission from the bulk of the stellar surface in both cases. The distance to the pulsar is constrained in a range of 1--4 kpc from the spectral fits. We infer the blackbody surface temperature of 10814+22108^{+22}_{-14} eV, while for the atmosphere model, the temperature, as seen by a distant observer, is 537+1253^{+12}_{-7} eV. In the latter case J0633+0632 is one of the coldest middle-aged isolated neutron stars with measured temperatures. Finally, it powers an extended pulsar wind nebula whose shape suggests a high pulsar proper motion. Looking backwards the direction of the presumed proper motion we found a likely birthplace of the pulsar -- the Rosette nebula, a 50-Myr-old active star-forming region located at about 1. ⁣ ⁣.\!\!^\circ5 from the pulsar. If true, this constrains the distance to the pulsar in the range of 1.2--1.8 kpc.Comment: 15 pages, 9 figures, 3 table

    Fusion of neutron rich oxygen isotopes in the crust of accreting neutron stars

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    Fusion reactions in the crust of an accreting neutron star are an important source of heat, and the depth at which these reactions occur is important for determining the temperature profile of the star. Fusion reactions depend strongly on the nuclear charge ZZ. Nuclei with Z6Z\le 6 can fuse at low densities in a liquid ocean. However, nuclei with Z=8 or 10 may not burn until higher densities where the crust is solid and electron capture has made the nuclei neutron rich. We calculate the SS factor for fusion reactions of neutron rich nuclei including 24^{24}O + 24^{24}O and 28^{28}Ne + 28^{28}Ne. We use a simple barrier penetration model. The SS factor could be further enhanced by dynamical effects involving the neutron rich skin. This possible enhancement in SS should be studied in the laboratory with neutron rich radioactive beams. We model the structure of the crust with molecular dynamics simulations. We find that the crust of accreting neutron stars may contain micro-crystals or regions of phase separation. Nevertheless, the screening factors that we determine for the enhancement of the rate of thermonuclear reactions are insensitive to these features. Finally, we calculate the rate of thermonuclear 24^{24}O + 24^{24}O fusion and find that 24^{24}O should burn at densities near 101110^{11} g/cm3^3. The energy released from this and similar reactions may be important for the temperature profile of the star.Comment: 7 pages, 4 figs, minor changes, to be published in Phys. Rev.
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