2019ApJ...887...11H


Query : 2019ApJ...887...11H

2019ApJ...887...11H - Astrophys. J., 887, 11-11 (2019/December-2)

Learning about the intermediate neutron-capture process from lead abundances.

HAMPEL M., KARAKAS A.I., STANCLIFFE R.J., MEYER B.S. and LUGARO M.

Abstract (from CDS):

Lead (Pb) is predominantly produced by the slow neutron-capture process (s process) in asymptotic giant branch (AGB) stars. In contrast to significantly enhanced Pb abundances predicted by low-mass, low-metallicity AGB models, observations of Magellanic post-AGB stars show incompatibly low Pb abundances. Observations of carbon-enhanced metal-poor (CEMP) stars whose s-process enrichments are accompanied by heavy elements traditionally associated with the rapid neutron-capture process (r process) have raised the need for a neutron-capture process operating at neutron densities intermediate to the s and r process: the so-called i process. We study i-process nucleosynthesis with single-zone nuclear-network calculations. Our i-process models can explain the heavy-element abundance patterns measured in Magellanic post-AGB stars including their puzzlingly low Pb abundances. Furthermore, the heavy-element enhancements in the post-AGB and CEMP-i stars, particularly their Pb abundance, allow us to characterize the neutron densities and exposures of the i process that produced the observed abundance patterns. We find that the lower-metallicity CEMP-i stars ([Fe/H]~-2.5) have heavy-element abundances best matched by models with higher neutron densities and exposures (τ > 2.0 mbarn–1) compared to the higher-metallicity post-AGB stars ([Fe/H]]~-1.3, τ < 1.3 mbarn–1). This offers new constraints and insights regarding the properties of i-process sites and demonstrates that the responsible process operates on timescales of the order of a few years or less.

Abstract Copyright: © 2019. The American Astronomical Society. All rights reserved.

Journal keyword(s): Asymptotic giant branch stars - Post-asymptotic giant branch - CEMP stars - Stellar abundances - Nuclear astrophysics - Nucleosynthesis - Stellar nucleosynthesis - Chemically peculiar stars - Carbon stars - Binary stars

Simbad objects: 34

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Number of rows : 34
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 HD 224959 SB* 00 02 08.0214788256 -02 49 12.232785144   10.6 9.6     CEMP-rs 104 0
2 BPS CS 31062-0050 Pe* 00 30 31.0646803224 -12 05 10.877225064   13.7 13.05 12.681 12.309 CEMP-r/s 70 0
3 CD-24 266 BS* 00 40 47.9313619824 -24 07 34.183333668   12.955 12.656 12.441 12.216 CEMP-s 100 0
4 SKB 2 Pe* 00 41 39.8197621944 -26 18 54.460585116   13.332 12.184 12.072 11.321 CEMP-s 92 0
5 SB 960 Pe* 00 44 03.5698629048 -13 55 26.268999384   12.69 12.15 11.806 11.483 CEMP-s 114 0
6 OGLE SMC-LPV-4910 pA* 00 44 41.1035011488 -73 21 36.123508332   17.06 15.61 15.44 14.515 G:I 30 0
7 NAME SMC G 00 52 38.0 -72 48 01   2.79 2.2     ~ 12317 1
8 HE 0058-0244 Pe* 01 00 53.0234702616 -02 28 19.950391884   14.42 13.73 13.331 12.942 CEMP-r/s 40 0
9 HE 0143-0441 Pe* 01 45 37.9166141208 -04 26 43.244756916   16.884 16.377     CEMP-s 30 0
10 HE 0243-3044 Pe* 02 45 16.4464212312 -30 32 02.118309504   17.11 16.10     CEMP-rs 15 0
11 BPS CS 29526-0110 Pe* 03 27 43.6392396600 -23 00 29.924362260   13.71 13.35 13.116 12.834 CEMP-r/s 54 0
12 HE 0336+0113 Pe* 03 38 52.9026695424 +01 23 07.778279004   15.807 14.941 14.980   CEMP-s 21 0
13 HE 0338-3945 Pe* 03 39 55.0068570984 -39 35 42.902896452   15.753 15.333 15.098 14.787 CEMP-r/s 42 0
14 HE 0414-0343 SB* 04 17 16.4631860496 -03 36 31.388697180   12.23 11.04     CEMP-r/s 21 0
15 2MASS J05063210-7142298 pA* 05 06 32.1295674936 -71 42 29.924779896 14.801 14.717 14.298 13.950 13.780 A3Iab/F0Ibpe 17 0
16 OGLE LMC-LPV-39792 LP* 05 18 48.8624065560 -70 02 47.086220796 18.692 17.142 15.429 14.31 13.852 F4Ib-II(e) 19 0
17 OGLE LMC-LPV-43685 pA* 05 20 43.8870629914 -69 23 41.139112840 17.618 16.515 15.075 13.92 13.887 F5Ib(e) 23 0
18 NAME LMC G 05 23 34.6 -69 45 22     0.4     ~ 19090 0
19 OGLE LMC-LPV-68005 LP* 05 32 50.7147024408 -71 39 25.723947636 17.985 16.533 15.069   13.803 F6Ia 18 0
20 HD 56126 pA* 07 16 10.2590823192 +09 59 47.954735376   9.20 8.32     F0/5Ia 330 0
21 HE 1305+0007 Pe* 13 08 03.8464604328 -00 08 47.502965400   13.98 12.223 11.541 11.071 CEMP-s 36 0
22 2MASS J13364604+4503086 Pe* 13 36 46.0325838312 +45 03 08.641824120   14.57 13.8 13.401 12.974 CEMP-r/s 19 0
23 UCAC4 407-057901 Pe* 14 07 42.9724778472 -08 36 14.381637516   14.910 14.099 13.929 13.171 CEMP-s 14 0
24 LP 625-44 Pe* 16 43 14.0377103880 -01 55 30.411443424   12.84 11.68     CEMP-s 111 0
25 2MASS J16510881+5712277 Pe* 16 51 08.8035670560 +57 12 27.769041180   14.80 14.4 13.986 13.672 CEMP-s 20 0
26 V* V4334 Sgr CV* 17 52 32.69352 -17 41 08.0160           F2Ia 390 0
27 HD 187861 SB* 19 56 26.9442832128 -65 22 08.014212084   10.42 9.18     CEMP-rs 70 0
28 BPS CS 22898-0027 Pe* 21 05 45.0996805992 -18 36 57.501493128   13.26 12.76 12.476 12.094 CEMP-r/s 88 0
29 HE 2134-3940 Pe* 21 37 45.7673945880 -39 27 22.313379600   13.790 12.660 12.160 11.760 KIIvw 88 0
30 HE 2148-1247 Pe* 21 51 17.9096426016 -12 33 41.557315896   15.266 14.740 14.582   CEMP-r/s 51 0
31 HD 209621 SB* 22 04 25.1430497160 +21 03 08.991263304   10.41 8.86     C-H3III: 111 0
32 HD 235858 pA* 22 29 10.3748806056 +54 51 06.344572284   11.40 9.52 8.47 7.34 G5Ia 264 0
33 BPS CS 22887-0048 Pe* 22 46 44.6216572248 -11 08 42.414994716   13.26 12.87 12.588 12.31 CEMP-s 29 0
34 HE 2258-6358 Pe* 23 01 48.6559441632 -63 42 25.117355556   15.42 14.30 14.07   CEMP-s 14 0

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