2022MNRAS.515.3014A


Query : 2022MNRAS.515.3014A

2022MNRAS.515.3014A - Mon. Not. R. Astron. Soc., 515, 3014-3027 (2022/September-2)

Thermal luminosity degeneracy of magnetized neutron stars with and without hyperon cores.

ANZUINI F., MELATOS A., DEHMAN C., VIGANO D. and PONS J.A.

Abstract (from CDS):

The dissipation of intense crustal electric currents produces high Joule heating rates in cooling neutron stars. Here, it is shown that Joule heating can counterbalance fast cooling, making it difficult to infer the presence of hyperons (which accelerate cooling) from measurements of the observed thermal luminosity Lγ. Models with and without hyperon cores match Lγ of young magnetars (with poloidal-dipolar field Bdip ≳ 1014 G at the polar surface and Lγ ≳ 1034 erg s–1 at t ≲ 105 yr) as well as mature, moderately magnetized stars (with Bdip ≲ 1014 G and 1031 erg s–1 ≲ Lγ ≲ 1032 erg s–1 at t ≳ 105 yr). In magnetars, the crustal temperature is almost independent of hyperon direct Urca cooling in the core, regardless of whether the latter is suppressed or not by hyperon superfluidity. The thermal luminosities of light magnetars without hyperons and heavy magnetars with hyperons have Lγ in the same range and are almost indistinguishable. Likewise, Lγ data of neutron stars with Bdip ≲ 1014 G but with strong internal fields are not suitable to extract information about the equation of state as long as hyperons are superfluid, with maximum amplitude of the energy gaps of the order ≈1 MeV.

Abstract Copyright: © 2022 The Author(s). Published by Oxford University Press on behalf of Royal Astronomical Society.

Journal keyword(s): stars: evolution - stars: interiors - stars: magnetic field - stars: neutron ;

Simbad objects: 3

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Number of rows : 3
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 PSR J0357+32 Psr 03 57 52.161 +32 05 23.63           ~ 104 0
2 RBS 1556 N* 16 05 18.9 +32 49 07     26.8     ~ 105 1
3 RX J1856.6-3754 Psr 18 56 35.11 -37 54 30.5     25.7     ~ 456 0

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