2022A&A...668A..58A


Query : 2022A&A...668A..58A

2022A&A...668A..58A - Astronomy and Astrophysics, volume 668A58 (2022/12-1)

Structure and evolution of ultra-massive white dwarfs in general relativity.

ALTHAUS L.G., CAMISASSA M.E., TORRES S., BATTICH T., CORSICO A.H., REBASSA-MANSERGAS A. and RADDI R.

Abstract (from CDS):

Context. Ultra-massive white dwarfs (M⋆ ≳ 1.05 M⊙) are of utmost importance in view of the role they play in type Ia supernovae explosions, merger events, the existence of high-magnetic -field white dwarfs, and the physical processes in the super asymptotic giant branch phase. Aims. We aim to present the first set of constant rest-mass ultra-massive oxygen-neon white dwarf cooling tracks with masses of M⋆ > 1.29 M⊙ which fully take into account the effects of general relativity on their structural and evolutionary properties. Methods. We computed the full evolution sequences of 1.29, 1.31, 1.33, 1.35, and 1.369 M⊙ white dwarfs with the La Plata stellar evolution code, LPCODE. For this work, the standard equations of stellar structure and evolution have been modified to include the effects of general relativity. Specifically, the fully general relativistic partial differential equations governing the evolution of a spherically symmetric star are solved in a way so that they resemble the standard Newtonian equations of stellar structure. For comparison purposes, the same sequences have been computed for the Newtonian case. Results. According to our calculations, the evolutionary properties of the most massive white dwarfs are strongly modified by general relativity effects. In particular, the resulting stellar radius is markedly smaller in the general relativistic case, being up to 25% smaller than predicted by the Newtonian treatment for the more massive ones. We find that oxygen-neon white dwarfs more massive than 1.369 M⊙ become gravitationally unstable with respect to general relativity effects. When core chemical distribution due to phase separation on crystallization is considered, such instability occurs at somewhat lower stellar masses, ≳1.36 M⊙. In addition, cooling times for the most massive white dwarf sequences are about a factor of two smaller than in the Newtonian case at advanced stages of evolution. Finally, a sample of white dwarfs have been identified as ideal candidates to test these general relativistic effects. Conclusions. We conclude that the general relativity effects should be taken into account for an accurate assessment of the structural and evolutionary properties of the most massive white dwarfs. These new ultra-massive white dwarf models constitute a considerable improvement over those computed in the framework of the standard Newtonian theory of stellar interiors.

Abstract Copyright: © L. G. Althaus et al. 2022

Journal keyword(s): stars: evolution - stars: interiors - white dwarfs

Simbad objects: 29

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Number of rows : 29
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 SDSS J003908.33+303538.9 WD* 00 39 08.3750668296 +30 35 39.758551332           DC 8 0
2 SN 2007if SN* 01 10 51.37 +15 27 39.9   23.3 19.5     SNIap 142 1
3 Gaia DR3 534407181320476288 WD? 01 54 08.7177753216 +72 04 08.298560136           ~ 4 0
4 LEHPM 2617 WD* 02 35 38.5493846364 -30 32 25.533289536           DA 12 0
5 TYC 5893-1218-1 * 04 16 12.4709187432 -18 26 59.432166024   13.01 11.88     ~ 1 0
6 Gaia DR3 283928743068277376 WD? 05 06 00.4065699294 +59 03 26.877537328           ~ 7 0
7 Gaia DR3 5763109404082525696 WD* 09 10 00.7194989376 -02 22 00.901520400           DC 7 0
8 Gaia DR3 3586879608689430400 WD* 11 36 47.9121012888 -10 57 24.142531860           DC 5 0
9 TYC 5513-1064-1 * 11 36 48.9172705680 -10 57 28.315404900   11.94 11.26     ~ 3 0
10 Gaia DR3 3585053427252374272 WD* 11 42 35.0307657792 -13 15 49.671051156           DC 6 0
11 Gaia DR3 3480787358063803520 WD* 11 49 56.4945653520 -29 06 03.510982717           ~ 2 0
12 SDSS J125106.11+440303.0 WD* 12 51 06.1607127984 +44 03 03.085257672   20.5 20.18 20.3   DC 14 0
13 Gaia DR3 6178573689547383168 WD* 13 55 44.9047269378 -26 00 28.960103639           DC 6 0
14 LSPM J1403+4533 WD* 14 03 24.7543609728 +45 33 33.020709048   19.37 18.81 18.9   DC 25 0
15 Gaia DR3 1674805012263764352 WD? 14 07 59.7162366535 +69 55 33.588848226           ~ 4 0
16 SN 2003fg SN* 14 16 18.924 +52 14 53.68           SNIa 141 1
17 Gaia DR3 6211904903507006336 WD* 15 03 00.5381096520 -30 05 47.667060636           DC 6 0
18 SN 2009dc SN* 15 51 12.12 +25 42 28.0           SNIa-norm 188 1
19 Gaia DR3 1424656526287583744 WD* 16 12 36.8881359864 +51 28 13.048913100           DC 6 0
20 SDSS J161252.59+512849.9 QSO 16 12 52.596 +51 28 49.96           ~ 2 0
21 Gaia DR3 4461423190259561728 PM* 16 49 05.3298510546 +13 46 58.726685385           ~ 2 0
22 Gaia DR3 4377579209528621184 WD? 16 51 36.8953112664 -04 15 44.379058896           ~ 4 0
23 SN 2006gz SN* 18 10 26.33 +30 59 44.4   16.6       SNIa 156 1
24 GALEX J183202.8+085635 WD* 18 32 02.8284063864 +08 56 36.244571280           DBA 21 0
25 IPHAS J190132.77+145807.6 WD* 19 01 32.7398565120 +14 58 07.176092088   15.51 15.72 15.78   DC2 42 0
26 Gaia DR3 1738863551836243840 WD? 21 24 29.2014772243 +06 39 34.931096256           ~ 5 0
27 Gaia DR3 6565940122868224640 WD? 21 48 54.4481513448 -43 04 18.010749792           ~ 4 0
28 Gaia DR3 6385055135655898496 WD? 22 29 30.5992094376 -70 18 20.818666980           ~ 5 0
29 Gaia DR3 1983698716601024512 WD? 22 40 01.3522554840 +46 48 43.340472936           ~ 3 0

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