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dc.contributor.authorPiersanti, Luciano
dc.contributor.authorDomínguez Aguilera, María Inmaculada 
dc.date.accessioned2022-03-23T13:04:29Z
dc.date.available2022-03-23T13:04:29Z
dc.date.issued2022-02-16
dc.identifier.citationLuciano Piersanti... [et al.], 2022 ApJ 926 103. [https://doi.org/10.3847/1538-4357/ac403b]es_ES
dc.identifier.urihttp://hdl.handle.net/10481/73662
dc.descriptionThis publication is part of the project I + D + I PGC2018-095317-B-C21 funded by MICIN/AEI/10.13039/501100011033 and FEDER "A way of doing Europe" (E.B. and I.D.); L.P. and O.S. acknowledge financial support from the INAF-mainstream project "Type Ia Supernovae and their Parent Galaxies: Expected Results from LSST." O.S. and L.P. acknowledge their participation to the V:ANS project (Vanvitelli program on standard candles in astrophysics: Atomic and Nuclear physics in SNIa) supported by the Vanvitelli University.es_ES
dc.description.abstractIn accreting white dwarfs (WDs) approaching the Chandrasekhar limit, hydrostatic carbon burning precedes the dynamical breakout. During this simmering phase, e-captures are energetically favored in the central region of the star, while beta-decay are favored more outside, and the two zones are connected by a growing convective instability. We analyze the interplay between weak interactions and convection, the so-called convective URCA process, during the simmering phase of Type Ia supernovae (SNe Ia) progenitors and its effects on the physical and chemical properties at the explosion epoch. At variance with previous studies, we find that the convective core powered by the carbon burning remains confined within the (21)(Ne,F) URCA shell. As a result, a much larger amount of carbon has to be consumed before the explosion that eventually occurs at larger density than previously estimated. In addition, we find that the extension of the convective core and its average neutronization depend on the the WD progenitor's initial metallicity. For the average neutronization in the convective core at the explosion epoch, we obtain (eta) over bar (exp) = (1.094 +/- 0.143) x 10(-3) + (9.168 +/- 0.677) x 10(-2) x Z. Outside the convective core, the neutronization is instead determined by the initial amount of C + N + O in the progenitor star. Since S, Ca, Cr, and Mn, the elements usually exploited to evaluate the pre-explosive neutronization, are mainly produced outside the heavily neutronized core, the problem of too high metallicity estimated for the progenitors of the historical Tycho and Kepler SNe Ia remains unsolved.es_ES
dc.description.sponsorshipFEDER "A way of doing Europe"es_ES
dc.description.sponsorshipINAF-mainstream project "Type Ia Supernovae and their Parent Galaxies: Expected Results from LSST"es_ES
dc.description.sponsorshipVanvitelli University PGC2018-095317-B-C21es_ES
dc.description.sponsorshipMICIN/AEI/10.13039/501100011033es_ES
dc.language.isoenges_ES
dc.publisherAmerican Astronomical Societyes_ES
dc.rightsAtribución 3.0 España*
dc.rights.urihttp://creativecommons.org/licenses/by/3.0/es/*
dc.titlePre-explosive Accretion and Simmering Phases of SNe Iaes_ES
dc.typejournal articlees_ES
dc.rights.accessRightsopen accesses_ES
dc.identifier.doi10.3847/1538-4357/ac403b
dc.type.hasVersionVoRes_ES


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