2025A&A...698A.216R


Query : 2025A&A...698A.216R

2025A&A...698A.216R - Astronomy and Astrophysics, volume 698A216 (2025/6-1)

The occurrence and impact of carbon-oxygen shell mergers in massive stars.

ROBERTI L., PIGNATARI M., BRINKMAN H.E., JEENA S.K., SIEVERDING A., FALLA A., LIMONGI M., CHIEFFI A. and LUGARO M.

Abstract (from CDS):

Context. In their final stages before undergoing a core-collapse supernova, massive stars may experience mergers between internal shells where carbon (C) and oxygen (O) are consumed as fuels for nuclear burning. This interaction, known as a C-O shell merger, can dramatically alter the internal structure of the star, leading to peculiar nucleosynthesis and potentially influencing the supernova explosion and the propagation of the subsequent supernova shock.
Aims. Our understanding of the frequency and consequences of C-O shell mergers remains limited. This study aims to identify, for the first time, early diagnostics in the stellar structure that lead to C-O shell mergers in more advanced stages. We also assess their role in shaping the chemical abundances in the most metal poor stars of the Galaxy.
Methods. We analyzed a set of 209 stellar evolution models available in the literature, with different initial progenitor masses and metallicities. We then compared the nucleosynthetic yields from a subset of these models with the abundances of odd-Z elements in metal-poor stars.
Results. We find that the occurrence of C-O shell mergers in stellar models can be predicted with a good approximation based on the outcomes of the central He burning phase, specifically, from the CO core mass (MCO) and the 12C central mass fraction (XC12): 90% of models with a C-O merger have XC12 <0.277 and MCO <4.90 M⊙, with average values of MCO = 4.02 M⊙ and XC12 = 0.176. The quantities XC12 and MCO are indirectly affected from several stellar properties, including the initial stellar mass and metallicity. Additionally, we confirm that the Sc-rich and K-rich yields from models with C-O mergers would solve the long-standing underproduction of these elements in massive stars.
Conclusions. Our results emphasize the crucial role of C-O shell mergers in enriching the interstellar medium, particularly in the production of odd-Z elements. This highlights the necessity of further investigations to refine their influence on presupernova stellar properties and their broader impact on Galactic chemical evolution.

Abstract Copyright: © The Authors 2025

Journal keyword(s): convection - nuclear reactions, nucleosynthesis, abundances - stars: abundances - stars: evolution - stars: massive - supernovae: general

Simbad objects: 35

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Number of rows : 35
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 2MASS J00061720+1057419 Pe* 00 06 17.2023422184 +10 57 41.854295088           ~ 7 0
2 HE 0039-4154 Pe* 00 41 43.4057863080 -41 37 57.347566500   14.654 13.832 13.318 12.786 ~ 15 0
3 HE 0048-6408 Pe* 00 50 45.2846592720 -63 51 50.416091208   13.52 12.48 12.29   ~ 15 0
4 BPS CS 22183-0031 Pe* 01 09 05.0900915136 -04 43 21.343580436   14.24 13.62 13.178 12.724 ~ 52 0
5 HE 0124-0119 Pe* 01 26 58.5792560424 +01 35 15.359701704   13.902 12.671 12.499   ~ 19 0
6 HE 0130-1749 Pe* 01 32 26.3749806552 -17 34 22.557244224   15.598 14.871 14.882   CEMP-no 8 0
7 HE 0139-2826 Pe* 01 41 36.8114907696 -28 11 02.828648508   14.42 13.74 13.81   CEMP-no 8 0
8 HE 0312-5200 Pe* 03 13 56.5301656296 -51 49 02.189359488   16.158 15.431 15.506   ~ 5 0
9 HE 0315-1528 Pe* 03 17 36.0539075280 -15 17 22.698017664   14.05 13.34 12.853 12.372 CEMP-no 23 0
10 HE 0324-0152 Pe* 03 26 53.8806654840 +02 02 28.154905512   12.49 12.67     CEMP-no 21 0
11 CD-24 1782 Pe* 03 38 41.4850201416 -24 02 50.292102948   10.54 9.97 9.246 8.811 ~ 91 0
12 HE 0409-1212 Pe* 04 12 13.8814287960 -12 05 05.075250072   13.843 12.897   11.764 ~ 72 0
13 Ross 889 Pe* 09 40 43.2053340378 +01 00 29.511836741       10.39   sdA4 166 0
14 HE 1124-2335 RG* 11 27 26.9490704592 -23 52 05.593418292     14.634   13.721 CEMP-no 16 0
15 BD-13 3695 RG* 13 22 44.1122246232 -13 55 31.431021528   11.428 10.686 9.794 9.434 ~ 35 0
16 HD 126587 Pe* 14 27 00.3636631296 -22 14 38.992940592   9.88 9.60 8.75   CEMP-no 145 0
17 UCAC4 302-083986 SB* 15 57 30.1025796144 -29 39 22.771142172   14.170 13.175 12.937   CEMP 15 0
18 SMSS J183719.09-262725.0 Pe* 18 37 19.0645753968 -26 27 25.010829828           ~ 2 0
19 BPS CS 22891-0200 Pe* 19 35 19.0776472464 -61 42 24.374080224   14.77 13.93   12.79 CEMP-no 45 0
20 HE 2002-5843 Pe* 20 07 03.7915948392 -58 34 57.592948836   13.72 13.03   12.102 CEMP-no 30 0
21 BPS CS 22950-0046 Pe* 20 21 28.3975657104 -13 16 33.601931364   15.13 14.224 13.639 13.066 CEMP-no 43 0
22 BPS CS 22879-0012 Pe* 20 37 14.0345099448 -41 02 33.500573556   15.11 14.72     ~ 13 0
23 BPS CS 30314-0067 Pe* 20 52 50.9878832880 -34 19 40.547263404   12.98 11.85 11.175 10.583 CEMP-no 36 0
24 BPS CS 22897-0008 Pe* 21 03 11.8565397504 -65 05 08.852220600   14.02 13.33     CEMP-no 80 0
25 BPS CS 29498-0043 Pe* 21 03 52.1197651440 -29 42 50.344181712   14.8 13.72 13.013 12.406 CEMP-no 100 0
26 HD 200654 Pe* 21 06 34.7513254468 -49 57 50.280288000   9.74 9.1     CEMP 118 0
27 BPS CS 30492-0110 Pe* 21 21 45.8298095616 -38 08 57.881349888   15.38 14.63     CEMP-no 15 0
28 BPS CS 22965-0016 Pe* 21 57 07.9207556880 -04 34 08.378375016 14.860 14.81 14.05     ~ 15 0
29 HE 2215-2548 Pe* 22 17 58.6422094992 -25 33 22.328173188   16.296 15.649 15.505   ~ 5 0
30 BPS CS 29502-0092 Pe* 22 22 35.9982138384 -01 38 27.620508552   12.64 11.87 11.365 10.862 CEMP-no 67 0
31 HE 2233-4724 Pe* 22 35 59.2821279768 -47 08 36.552379524   15.53 14.51 14.34   ~ 7 0
32 BPS CS 22893-0010 Pe* 22 58 11.7253311672 -11 56 45.431946204   15.34 14.73 14.70   ~ 19 0
33 BD+38 4955 SB* 23 13 38.8205905578 +39 25 02.589638688 11.52 11.67 11.01 10.38 9.92 F6 128 0
34 BPS CS 22941-0017 Pe* 23 32 50.1815130552 -33 59 25.571473908   15.56 15.00     ~ 15 0
35 BPS CS 30315-0029 Pe* 23 34 26.6960486448 -26 42 14.003379828   14.56 13.64 13.092 12.518 ~ 32 0

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