2021A&A...648A.107A


Query : 2021A&A...648A.107A

2021A&A...648A.107A - Astronomy and Astrophysics, volume 648A107-107 (2021/4-1)

Rubidium abundances in solar metallicity stars.

ABIA C., DE LAVERNY P., KOROTIN S., ASENSIO RAMOS A., RECIO-BLANCO A. and PRANTZOS N.

Abstract (from CDS):


Context. Rubidium is one of the few elements produced by the neutron capture s- and r-processes in almost equal proportions. Recently, a Rb deficiency ([Rb/Fe]<0.0), amounting to a factor of about two with respect to the Sun, has been found in M dwarfs of near-solar metallicity. This stands in contrast to the close-to-solar [Sr, Zr/Fe] ratios derived in the same stars. This deficiency is difficult to understand from the point of view of observations and of nucleosynthesis.
Aims. To test the reliability of this Rb deficiency, we study the Rb and Zr abundances in a sample of KM-type giant stars across a similar metallicity range, extracted from the AMBRE Project.
Methods. We used high-resolution and high signal-to-noise spectra to derive Rb and Zr abundances in a sample of 54 bright giant stars with metallicities in the range of -0.6≤[Fe/H]≤+0.4dex, via spectral synthesis in both local and non-local thermodynamic equilibrium (LTE and NLTE, respectively). We also studied the impact of the Zeeman broadening in the profile of the RbI at λ7800 Å line.
Results. The LTE analysis also results in a Rb deficiency in giant stars, however, it is considerably lower than that obtained in M dwarfs. However, once NLTE corrections are performed, the [Rb/Fe] ratios are very close to solar (average -0.01±0.09dex) in the full metallicity range studied here. This stands in contrast to the value found for M dwarfs. The [Zr/Fe] ratios derived are in excellent agreement with those obtained in previous studies in FGK dwarf stars with a similar metallicity. We investigate the effect of gravitational settling and magnetic activity as possible causes of the Rb deficiency found in M dwarfs. Although the former phenomenon has a negligible impact on the surface Rb abundance, the presence of an average magnetic field with an intensity that is typical of that observed in M dwarfs may result in systematic Rb abundance underestimations if the Zeeman broadening is not considered in the spectral synthesis. This may explain the Rb deficiency in M dwarfs, but not fully. On the other hand, the new [Rb/Fe] and [Rb/Zr] versus [Fe/H] relationships can be explained when the Rb production by rotating massive stars and low-to-intermediate mass stars (these latter also producing Zr) are considered, without the need to deviate from the standard s-process nucleosynthesis in asymptotic giant branch stars, as suggested previously.

Abstract Copyright: © ESO 2021

Journal keyword(s): stars: abundances - stars: late-type - nuclear reactions, nucleosynthesis, abundances

CDS comments: G244-77 could be G244-37 or G244-47 in Simbad.

Simbad objects: 62

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Number of rows : 62
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 1638 * 00 20 28.3131118560 -30 33 19.877390424   10.05 8.73     K1III 37 0
2 HD 5544 * 00 57 13.0376891352 +00 20 32.401126356   8.76 7.63     K0III 46 0
3 G 244-37 PM* 01 51 51.1331191583 +64 26 05.922299097       11.036   M2.5V 75 0
4 HD 11643 PM* 01 53 23.1726086160 -38 35 40.673979852   7.234 6.086     K1/2III 38 0
5 G 244-47 PM* 02 01 35.3407161312 +63 46 11.997406488       10.630   M2.5V 88 0
6 HD 12642 PM* 02 03 40.4889439392 -04 06 12.653704296   7.189 5.609     M1IIICa1 46 0
7 * 39 Ari PM* 02 47 54.5420751618 +29 14 49.625779256 6.710 5.630 4.510 3.72 3.14 K0.5IIIb 184 0
8 * alf Cet LP? 03 02 16.77307 +04 05 23.0596 6.10 4.17 2.53 1.18 0.02 M1.5IIIa 480 1
9 * alf Tau LP? 04 35 55.23907 +16 30 33.4885 4.32 2.40 0.86 -0.37 -1.31 K5+III 1298 2
10 * omi02 Ori PM* 04 56 22.2759672613 +13 30 52.087623488 6.31 5.21 4.06 3.18 2.55 K2-IIIb 138 0
11 HD 61603 * 07 40 58.5185843832 +23 01 06.703077972   7.458 5.906     K5III 57 0
12 HD 65354 * 07 57 03.0244580448 -34 22 42.353381640   8.41 6.82     K3III 35 0
13 HD 71160 SB* 08 24 39.8543446248 -32 55 26.544582156   9.44 7.96     K3/4III 30 0
14 HD 72505 PM* 08 33 45.0461058600 +13 15 26.322654420   7.447 6.247     K0III 53 0
15 HD 74088 * 08 38 27.8603163504 -62 50 35.661016284   8.30 6.71     K4III 35 0
16 * 78 Cnc PM* 09 09 02.3116000152 +17 28 10.749983016   8.386 7.176     K3III 54 0
17 HD 79349 * 09 11 43.0372705608 -48 46 23.463580188   10.01 8.53     K5/M0IV 34 0
18 * alf Hya * 09 27 35.24270 -08 39 30.9583 5.14 3.42 1.97 0.93 0.16 K3IIIa 455 1
19 * 10 Leo SB* 09 37 12.6793421832 +06 50 08.960833176   6.050 5.009     K1III 108 0
20 HD 90862 * 10 29 44.4174363432 +16 58 47.942088132   10.16 8.67     K2 33 0
21 * nu. Hya PM* 10 49 37.4882533447 -16 11 37.129417316 5.62 4.35 3.11 2.17 1.53 K1.5IIIHdel-0.5 191 0
22 HD 95208 * 10 57 15.7821844824 -75 05 59.140672008   7.630 6.122     K1II 22 0
23 * p03 Leo PM* 11 03 36.5918764464 -00 00 02.990493144   7.157 5.927     K2III 58 0
24 LP 733-99 LM* 11 20 06.1045187904 -10 29 46.727203956   12.734 11.250 10.887   M2.0V 65 0
25 * nu. Vir LP* 11 45 51.5595979999 +06 31 45.748996439 7.32 5.54 4.04 2.79 1.78 M1III 267 0
26 HD 102780 * 11 50 08.0380679712 +20 17 13.426967184   9.80 8.18     K2 22 0
27 * eps Cru PM* 12 21 21.6081337639 -60 24 04.133270061   4.98 3.57     K3III 97 0
28 HD 111464 * 12 50 14.0215011504 -62 38 28.677227784 9.59 8.10 6.63     K3III 28 0
29 HD 119971 PM* 13 47 38.5389693936 -50 19 14.478304008   6.791 5.446     K2III 47 0
30 HD 121416 PM* 13 56 19.7763079968 -46 35 34.616994576   6.955 5.815     K1III 57 0
31 HD 124186 * 14 11 15.1208225784 +32 17 45.212040312   7.393 6.129     K4III 65 0
32 * alf Boo RG* 14 15 39.67207 +19 10 56.6730 2.46 1.18 -0.05 -1.03 -1.68 K1.5IIIFe-0.5 2417 1
33 HD 128688 ** 14 38 50.8801425307 -22 32 34.590049581   9.68 8.93     G8/K0V 17 0
34 * 18 Lib PM* 14 58 53.5813630608 -11 08 38.462393832   7.146 5.857     K3-IIICN2 129 0
35 2MASS J15023844-4156105 * 15 02 38.4331191264 -41 56 10.519243584           K7III 3 0
36 V* OT Ser PM* 15 21 52.9325510712 +20 58 39.910874376 12.662 11.522 10.003 8.993 7.843 M1.0V 170 0
37 * 37 Lib PM* 15 34 10.7024841438 -10 03 52.317750492 6.48 5.63 4.62 3.85 3.33 K1III-IV 187 0
38 * alf Ser PM* 15 44 16.0741095811 +06 25 32.268792881 5.080 3.800 2.630 1.82 1.25 K2IIIbCN1 533 0
39 * eps CrB PM* 15 57 35.2514020181 +26 52 40.366652765 6.650 5.360 4.130 3.27 2.64 K2IIIab 280 1
40 HD 145206 SB* 16 09 50.5038223560 -03 28 00.278812956   6.817 5.378     K4III 76 0
41 * del Oph PM* 16 14 20.7390218758 -03 41 39.572826363 6.30 4.34 2.75 1.46 0.43 M0.5III 377 0
42 HD 148513 PM* 16 28 33.9807973104 +00 39 54.001143144 8.65 6.85 5.39     K3V 170 0
43 HD 148291 * 16 30 49.3595489040 -61 38 00.620711808   6.417 5.182     K1IIb 31 1
44 * h Her PM* 16 32 36.2919789280 +11 29 16.948144457 8.16 6.34 4.85 3.65 2.79 K4.5III 164 0
45 * H Sco V* 16 36 22.4715031529 -35 15 19.193081688   5.730 4.156     K5III 66 0
46 M 13 GlC 16 41 41.634 +36 27 40.75     5.8     ~ 2291 0
47 * zet Ara * 16 58 37.2125360584 -55 59 24.499906233   4.701 3.076     K3III 108 0
48 * bet Ara s*r 17 25 17.9878053183 -55 31 47.574076000 5.87 4.31 2.85     K0/1Ib 139 0
49 NGC 6352 GlC 17 25 29.11 -48 25 19.8           ~ 425 0
50 HD 320868 * 17 54 37.0721487840 -34 51 48.599767908   10.31 8.92     K5 13 0
51 * 104 Her V* 18 11 54.1566238248 +31 24 19.256317416 8.56 6.62 4.97     M3III 127 0
52 V* V401 Dra BY* 18 17 25.1255884056 +48 22 02.331245064   12.81 11.37 10.91   dM2.0 58 0
53 HD 167818 * 18 18 03.1916425335 -27 02 33.516672033   6.265 4.627     K3II 59 0
54 HD 169191 PM* 18 22 49.0396549896 +17 49 35.819693400   6.499 5.249     K3III 86 0
55 * lam Sgr PM* 18 27 58.2407185 -25 25 18.114589 4.75 3.85 2.81 2.06 1.50 K1IIIb 290 0
56 * ksi Tel V* 20 07 23.1574676136 -52 52 50.854022940 8.40 6.56 4.94     K5III 61 0
57 HD 198357 * 20 51 00.7581658752 -37 54 47.992190904   6.889 5.500     K3III 35 0
58 HD 199642 * 21 00 43.4224961664 -53 44 20.648477688   7.84 6.26     K5/M0III 24 0
59 * phi Cap * 21 15 37.8995516616 -20 39 06.102756432   6.317 5.152     K0II/III 46 0
60 * 33 Cap PM* 21 24 09.5931989472 -20 51 06.731650296   6.535 5.366     K0III 123 0
61 * ups PsA * 22 08 25.9315263653 -34 02 37.826070169 8.28 6.47 4.99     K4III 45 0
62 * phi Aqr SB* 23 14 19.3582404192 -06 02 56.423128812 7.64 5.77 4.22 2.94 1.86 M1.5III 137 0

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