6,477 research outputs found

    Nucleon Superfluidity vs Observations of Cooling Neutron Stars

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    Cooling simulations of neutron stars (NSs) are performed assuming that stellar cores consist of neutrons, protons and electrons and using realistic density profiles of superfluid critical temperatures Tcn(ρ)T_{cn}(\rho) and Tcp(ρ)T_{cp}(\rho) of neutrons and protons. Taking a suitable profile of Tcp(ρ)T_{cp}(\rho) with maximum ∌5×109\sim 5 \times 10^9 K one can obtain smooth transition from slow to rapid cooling with increasing stellar mass. Adopting the same profile one can explain the majority of observations of thermal emission from isolated middle--aged NSs by cooling of NSs with different masses either with no neutron superfluidity in the cores or with a weak superfluidity, Tcn<108T_{cn} < 10^8 K. The required masses range from ∌1.2M⊙\sim 1.2 M_\odot for (young and hot) RX J0822-43 and (old and warm) PSR 1055-52 and RX J1856-3754 to ≈1.45M⊙\approx 1.45 M_\odot for the (colder) Geminga and Vela pulsars. Observations constrain the Tcn(ρ)T_{cn}(\rho) and Tcp(ρ)T_{cp}(\rho) profiles with respect to the threshold density of direct Urca process and maximum central density of NSs.Comment: 4 pages, 2 figures, AA Letters, accepte

    Bulk viscosity in superfluid neutron star cores. I. Direct Urca processes in npe\mu matter

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    The bulk viscosity of the neutron star matter due to the direct Urca processes involving nucleons, electrons and muons is studied taking into account possible superfluidity of nucleons in the neutron star cores. The cases of singlet-state pairing or triplet-state pairing (without and with nodes of the superfluid gap at the Fermi surface) of nucleons are considered. It is shown that the superfluidity may strongly reduce the bulk viscosity. The practical expressions for the superfluid reduction factors are obtained. For illustration, the bulk viscosity is calculated for two models of dense matter composed of neutrons, protons,electrons and muons. The presence of muons affects the bulk viscosity due to the direct Urca reactions involving electrons and produces additional comparable contribution due to the direct Urca reactions involving muons. The results can be useful for studying damping of vibrations of neutron stars with superfluid cores.Comment: 14 pages, 7 figures, latex, uses aa.cls, to be published in Astronomy and Astrophysic

    Neutrino Pair Bremsstrahlung in Neutron Star Crusts: a Reappraisal

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    We demonstrate that band-structure effects suppress bremsstrahlung of neutrino pairs by electrons in the crusts of neutron stars at temperatures of the order of 5×109 K5\times 10^9 \,{\rm K} and below. Taking this into account, together with the fact that recent work indicates that the masses of neutron star crusts are considerably smaller than previously estimated, we find neutrino pair bremsstrahlung to be much less important for the thermal evolution of neutron stars than earlier calculations suggested.Comment: 11 plain LaTeX pages, 3 figures available on request, NORDITA-93/72 A/S/

    Nuclear Effects on Bremsstrahlung Neutrino Rates of Astrophysical Interest

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    We calculate in this work the rates for the neutrino pair production by nucleon-nucleon bremsstrahlung taking into account the full contribution from a nuclear one-pion-exchange potential. It is shown that if the temperatures are low enough (T≀20MeVT \leq 20 MeV), the integration over the nuclear part can be done for the general case, ranging from the completely degenerate (D) to the non-degenerate (ND) regime. We find that the inclusion of the full nuclear contribution enhances the neutrino pair production by nnnn and pppp bremsstrahlung by a factor of about two in both the D and ND limits when compared with previous calculations. This result may be relevant for the physical conditions of interest in the semitransparent regions near the neutrinosphere in type II supernovae, cooling of neutron stars and other astrophysical situations.Comment: 11 pages, no figures, LaTex file. submitted to PR

    New records and combinations for Neotropical Leptophlebiidae (Ephemeroptera)

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    Several species of Leptophlebiidae (Atalophlebiinae) from South and Central America are given new generic combinations based on improved knowledge of the Leptophlebiidae of the region. These are Tikuna bilineata (Needham & Murphy, 1924, Choroterpes) comb. nov.; Terpides vinculum (Traver, 1947, Choroterpes) comb. n.; Hermanella costalis (Navas, 1934, Thraulus) comb. n.; Hermanella costalis (Navas, 1934, Thraulus) comb.n.; Ulmeritoides haarupi (Esben-Petersen, 1912, Thraulus) comb. n. (synonyms Deleatidium vittatum, Thew syn. n. and Ulmeritoides fidalgoi Dominguez, 1995, syn. n.). In addition, we give new distribution records for Tikuna bilineata, report Choroterpes from Colombia, and describe Hagenulus marshal sp. n. from Ecuador based on two male imagos.Fil: Peters, J. G.. Florida A&M University; Estados UnidosFil: Flowers, R. W.. Florida A&M University; Estados UnidosFil: Hubbard, M. D.. Florida A&M University; Estados UnidosFil: Dominguez, Eduardo. Consejo Nacional de Investigaciones CientĂ­ficas y TĂ©cnicas. Centro CientĂ­fico TecnolĂłgico Conicet - TucumĂĄn; Argentina. Universidad Nacional de TucumĂĄn. Facultad de Ciencias Naturales e Instituto Miguel Lillo; ArgentinaFil: Savage, H. M.. Centers for Disease Control and Prevention; Estados Unidos. Florida A&M University; Estados Unido

    Three Types of Cooling Superfluid Neutron Stars: Theory and Observations

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    Cooling of neutron stars (NSs) with the cores composed of neutrons, protons, and electrons is simulated assuming 1^1S0_0 pairing of neutrons in the NS crust, and also 1^1S0_0 pairing of protons and weak 3^3P2_2 pairing of neutrons in the NS core, and using realistic density profiles of the superfluid critical temperatures Tc(ρ)T_{\rm c}(\rho). The theoretical cooling models of isolated middle-aged NSs can be divided into three main types. (I) {\it Low-mass}, {\it slowly cooling} NSs where the direct Urca process of neutrino emission is either forbidden or almost fully suppressed by the proton superfluidity. (II) {\it Medium-mass} NSs which show {\it moderate} cooling via the direct Urca process suppressed by the proton superfluidity. (III) {\it Massive} NSs which show {\it fast} cooling via the direct Urca process weakly suppressed by superfluidity. Confronting the theory with observations we treat RX J0822--43, PSR 1055--52 and RX J1856--3754 as slowly cooling NSs. To explain these sufficiently warm sources we need a density profile Tc(ρ)T_{\rm c}(\rho) in the crust with a rather high and flat maximum and sharp wings. We treat 1E 1207--52, RX J0002+62, PSR 0656+14, Vela, and Geminga as moderately cooling NSs. We can determine their masses for a given model of proton superfluidity, Tcp(ρ)T_{\rm cp}(\rho), and the equation of state in the NS core. No rapidly cooling NS has been observed so far.Comment: 12 pages, 10 figures, Astron. Astrophys., submitte

    Contribution of the massive photon decay channel to neutrino cooling of neutron stars

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    We consider massive photon decay reactions via intermediate states of electron-electron-holes and proton-proton-holes into neutrino-antineutrino pairs in the course of neutron star cooling. These reactions may become operative in hot neutron stars in the region of proton pairing where the photon due to the Higgs-Meissner effect acquires an effective mass mγm_{\gamma} that is small compared to the corresponding plasma frequency. The contribution of these reactions to neutrino emissivity is calculated; it varies with the temperature and the photon mass as T3/2mγ7/2e−mγ/TT^{3/2}m_{\gamma}^{7/2} e^{-m_{\gamma}/T} for T<mγT < m_{\gamma}. Estimates show that these processes appear as extra efficient cooling channels of neutron stars at temperatures T≃(109−1010)T \simeq (10^9-10^{10}) K.Comment: accepted to publication in Zh. Eksp. Teor. Fiz. (JETP

    Local Density Approximation for proton-neutron pairing correlations. I. Formalism

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    In the present study we generalize the self-consistent Hartree-Fock-Bogoliubov (HFB) theory formulated in the coordinate space to the case which incorporates an arbitrary mixing between protons and neutrons in the particle-hole (p-h) and particle-particle (p-p or pairing) channels. We define the HFB density matrices, discuss their spin-isospin structure, and construct the most general energy density functional that is quadratic in local densities. The consequences of the local gauge invariance are discussed and the particular case of the Skyrme energy density functional is studied. By varying the total energy with respect to the density matrices the self-consistent one-body HFB Hamiltonian is obtained and the structure of the resulting mean fields is shown. The consequences of the time-reversal symmetry, charge invariance, and proton-neutron symmetry are summarized. The complete list of expressions required to calculate total energy is presented.Comment: 22 RevTeX page
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