2022A&A...667A..50N


Query : 2022A&A...667A..50N

2022A&A...667A..50N - Astronomy and Astrophysics, volume 667A50 (2022/11-1)

Hunting for anti-solar differentially rotating stars using the Rossby number An application to the Kepler field.

NORAZ Q., BRETON S.N., BRUN A.S., GARCIA R.A., STRUGAREK A., SANTOS A.R.G., MATHUR S. and AMARD L.

Abstract (from CDS):



em Context. Anti-solar differential rotation profiles have been found for decades in numerical simulations of convective envelopes of solar-type stars. These profiles are characterized by a slow equator and fast poles (i.e., reversed with respect to the Sun) and have been found in simulations for high Rossby numbers. Rotation profiles like this have been reported in evolved stars, but have never been unambiguously observed for cool solar-type stars on the main sequence. As solar-type stars age and spin down, their Rossby numbers increase, which could therefore induce a transition toward an anti-solar differential rotation regime before the end of the main sequence. Such a rotational transition will impact the large-scale dynamo process and the magnetic activity. In this context, detecting this regime in old main-sequence solar-type stars would improve our understanding of their magnetorotational evolution.

em Aims. The goal of this study is to identify the most promising cool main-sequence stellar candidates for anti-solar differential rotation in the Kepler sample.

em Methods. First, we introduce a new theoretical formula to estimate fluid Rossby numbers, Rof, of main-sequence solar-type stars. We derived it from observational quantities such as Teff and Prot, and took the influence of the internal structure into account. Then, we applied it on a subset of the most recent catalog of Kepler rotation periods, after removing subgiants and selecting targets with solar metallicity. Next, we considered the highest computed Rof and inspected each target individually to select the most reliable anti-solar candidate. Finally, we extended our study to stars with metallicities different from that of the Sun. To this end, we developed a formulation for Rof dependent on the metallicity index [Fe/H] by using 1D stellar grids, and we also considered this compositional aspect for the selection of the targets.

em Results. We obtain a list of the most promising stars that are likely to show anti-solar differential rotation. We identify two samples: one at solar metallicity, including 14 targets, and another for other metallicities, including 8 targets. We find that the targets with the highest Rof are likely to be early-G or late-F stars at about log10g = 4.37 dex. Conclusions. We conclude that cool main-sequence stellar candidates for anti-solar differential rotation exist in the Kepler sample. The most promising candidate is KIC 10907436, and two other particularly interesting candidates are the solar analog KIC 7189915 and the seismic target KIC 12117868. Future characterization of these 22 stars is expected to help us understand how dynamics can impact magnetic and rotational evolution of old solar-type stars at high Rossby number.

Abstract Copyright: © Q. Noraz et al. 2022

Journal keyword(s): stars: rotation - stars: solar-type - Sun: evolution - methods: analytical - methods: data analysis - methods: observational

VizieR on-line data: <Available at CDS (J/A+A/667/A50): tablec1.dat>

Status at CDS : All or part of tables of objects could be ingested in SIMBAD with priority 2.

Simbad objects: 28

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Number of rows : 28
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 UCAC4 689-063777 * 18 50 24.7228679472 +47 44 57.522190920   13.316 12.642 12.549   ~ 5 0
2 UCAC4 662-069347 * 18 57 00.5674707360 +42 20 13.582994028   15.200 14.566 14.307   ~ 3 0
3 UCAC4 664-070155 * 18 57 12.2315316840 +42 41 01.027276944   13.464 12.916 12.788   G2V 4 0
4 2MASS J18591470+4823235 SB* 18 59 14.7088717656 +48 23 23.434854216           F5 5 0
5 TYC 3541-2345-1 Em* 19 02 09.8972932896 +45 16 39.357745608   10.90 10.21     G3V 57 0
6 2MASS J19022987+3846463 Ro* 19 02 29.8741828272 +38 46 46.298412912           ~ 8 0
7 2MASS J19043983+4304409 * 19 04 39.831 +43 04 40.95           ~ 3 0
8 BD+38 3428 PM* 19 05 45.2617733112 +38 31 22.560830328   9.77 9.22     F9IV-V 78 0
9 UCAC4 646-066160 * 19 08 02.5677012888 +39 10 00.030128484       15.686   ~ 3 0
10 UCAC4 662-070984 * 19 10 02.8904818152 +42 23 14.878256208   15.266 14.763 14.679   ~ 4 0
11 UCAC4 664-072397 * 19 13 46.7418739080 +42 47 24.377981388   16.015 15.676 15.383   ~ 3 0
12 2MASS J19165995+4147419 PM* 19 16 59.9505521664 +41 47 41.773684668           ~ 4 0
13 2MASS J19223530+3814431 Ro* 19 22 35.3027683344 +38 14 43.106195400           ~ 7 0
14 UCAC4 702-064912 * 19 23 00.2830115208 +50 16 51.859381620       14.203   ~ 3 0
15 UCAC4 693-067360 * 19 24 34.3148892744 +48 31 27.312417048   15.453 14.540 14.258   ~ 3 0
16 UCAC4 645-069921 * 19 24 55.5872052312 +38 50 23.791880220   13.456 12.768 12.584   ~ 3 0
17 UCAC4 638-069651 * 19 26 47.4174330072 +37 31 28.533393984   14.489 13.840 13.684   G0.5V 6 0
18 UCAC4 647-069440 * 19 29 28.6087286616 +39 19 26.576905188   14.273 13.603 13.539   ~ 4 0
19 UCAC4 690-069270 * 19 35 33.5366146176 +47 54 01.309090536   14.972 14.251 14.052   ~ 3 0
20 2MASS J19355427+3856069 * 19 35 54.2767665960 +38 56 06.970748352           ~ 5 0
21 TYC 3568-959-1 Em* 19 41 00.3007494768 +50 41 41.466858288   11.19 10.54     F6IV 24 0
22 2MASS J19413531+4011459 RG* 19 41 35.3237536104 +40 11 45.782902644   15.510 14.662 14.294 13.44 ~ 9 0
23 UCAC4 671-077255 * 19 43 53.7391295760 +44 07 50.602871352   16.158 15.175 15.031   ~ 3 0
24 2MASS J19481098+4154190 * 19 48 10.9927148160 +41 54 18.940202676           ~ 3 0
25 UCAC4 669-077822 * 19 48 36.2441196000 +43 40 54.246525240   16.063 15.368 15.135   ~ 3 0
26 2MASS J19504197+4823579 * 19 50 42.0238384656 +48 23 57.443070048           ~ 3 0
27 UCAC4 657-079524 * 19 54 14.8004801904 +41 21 39.570446484       14.516   ~ 3 0
28 2MASS J20003706+4400563 * 20 00 37.0683011448 +44 00 56.317347972           ~ 4 0

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