2025A&A...704A...8S


Query : 2025A&A...704A...8S

2025A&A...704A...8S - Astronomy and Astrophysics, volume 704A8 (2025/12-1)

Surface activity of a Rossby sequence of cool Hyades stars.

STRASSMEIER K.G., ILYIN I., STEFFEN M. and BARNES S.A.

Abstract (from CDS):

Aims. The Hyades cluster is key for the study of the rotational, activity, and chemical evolution of solar-like low-mass stars. We present quantitative surface-activity information for a sequence of 21 Hyades dwarf stars with effective temperatures 6160-3780 K (all cooler than the red edge of the Li dip), rotation periods 5-16 d, and normalized Rossby numbers (Ron) between 0.14 to 0.54 with respect to the Sun (Ro(Sun) = 1).
Methods. High-resolution Stokes-V spectra and a least-squares deconvolution of thousands of spectral lines per spectrum were employed to measure the longitudinal surface magnetic field. We obtained the velocities, lithium abundances, metallicity, and chromospheric Ca II infrared-triplet (IRT) fluxes from Stokes-I spectra.
Results. The average metallicity, +0.186 ± 0.045 (rms), for our stars with Teff ≥ 4200 K agrees well with the metallicity in the recent literature. The lithium abundances A(Li) range from 95-times solar (A(Li) ≈ + 3.0) on the warm end of the sample to 1/25 solar (A(Li) ≈ - 0.4) on the cool end. We confirm the tight relation of A(Li) with Teff and extend it to K-M stars with even lower Li abundances than previously measurable. A formal relation with rotational period and velocity in the sense of a higher Li abundance for faster rotators is present. Targets that rotate faster than v sin i of 6 km s–1 (Prot ≈ 8 d) appear to be Li saturated at A(Li) ≈3.0 dex. The Ca II IRT fluxes for our sample indicate (logarithmic) chromospheric radiative losses R'IRT in the range -4.0 to -4.9 in units of the bolometric flux. These radiative losses are also related to Teff, Prot, and v sin i, but opposite to A(Li), in an inverse sense with higher radiative losses for the slower, that is, cooler rotators. Longitudinal magnetic field strengths were measured in the range zero to -100 G and +150 G with phase-averaged disk-integrated unsigned values ⟨|B|⟩ of 15.4 ± 3.6(rms) G for targets warmer than ≈5000 K and 91 ± 61(rms) G for targets cooler than this. These unsigned field strengths are related to Prot, v sin i, and Ron, but in a dual-slope fashion. The short-period bona fide single M-target RSP 348 was found to be a double-lined spectroscopic binary with a classification dM3e+dM5e.
Conclusions. We conclude that the dependence on Rossby number of the surface activity tracers A(Li), R'IRT, and ⟨|B|⟩ on our Hyades dwarf sequence primarily originates from convective motions, expressed by its turnover time, and only to a smaller and sometimes inverse extent from surface rotation and its related additional mixing.

Abstract Copyright: © The Authors 2025

Journal keyword(s): stars: activity - stars: magnetic field - stars: rotation - starspots - open clusters and associations: individual: Hyades

VizieR on-line data: <Available at CDS (J/A+A/704/A8): stars.dat tablec2.dat>

Simbad objects: 27

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Number of rows : 27
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 BD+20 598 ** 03 37 34.9779179832 +21 20 35.451123144   10.282 9.362     K0V 101 1
2 HD 285252 PM* 03 55 06.5013825432 +16 59 54.520671696   9.870 8.964 8.472 8.049 K0 125 0
3 HG 7-88 PM* 04 05 25.6705307712 +19 26 31.745309388   12.750 11.400 10.94   K7 81 0
4 HD 285367 PM* 04 05 39.6749447280 +17 56 15.761428188   10.190 9.291     K0 102 0
5 HD 25825 PM* 04 06 16.1277225936 +15 41 53.233746900   8.416 7.811 7.484 7.169 G0V 222 0
6 HD 26736 BY* 04 14 32.3145372576 +23 34 29.798635044   8.711 8.047 7.691 7.356 G5V 245 0
7 V* V984 Tau BY* 04 16 33.4775734800 +21 54 26.882025156   9.944 9.125     ~ 195 0
8 HD 285690 BY* 04 18 19.2717491592 +16 05 17.992962636   10.532 9.548 9.015 8.557 K0 171 0
9 V* V893 Tau BY* 04 18 57.9745736544 +19 54 24.124484232   9.345 8.597 8.192 7.829 G9V 170 0
10 HD 27282 PM* 04 19 08.0079247152 +17 31 29.115479280 9.46 9.157 8.427 8.034 7.675 G8V 213 0
11 HD 27406 BY* 04 20 12.9666179232 +19 14 00.518450172   8.016 7.444 7.131 6.826 F9V+ 216 0
12 V* V988 Tau BY* 04 23 22.8504016872 +19 39 31.317351336   10.290 9.381     K0 138 0
13 V* V993 Tau BY* 04 27 35.8912011816 +15 35 21.090336828   7.949 7.404 7.102 6.805 F8V 262 0
14 HD 28237 PM* 04 27 46.0745928288 +11 44 11.108386212   8.066 7.482     F8 179 0
15 HD 285830 Em* 04 27 47.0352816264 +14 25 03.899709120   10.402 9.475 8.966 8.526 K0 155 0
16 HG 7-224 PM* 04 27 59.2152573288 +18 45 32.668898760   15.82 14.22     dM4.0 42 0
17 HD 285876 Em* 04 31 52.4720892792 +15 29 58.132447224   12.300 11.000 10.622   K0V 121 0
18 HD 28878 PM* 04 33 37.9670187024 +16 45 44.998350336   10.254 9.357 8.874 8.456 G5 138 0
19 HD 28977 PM* 04 34 32.1824860800 +15 49 39.204565644   10.565 9.644 9.139 8.702 K0 134 0
20 HD 28992 BY* 04 34 35.3100676992 +15 30 16.642906992   8.530 7.898 7.556 7.226 G1V 234 0
21 StKM 1-514 PM* 04 47 18.5088254064 +06 27 11.546776224   12.608 11.348 10.89   M0.0V 45 0
22 LP 416-570 PM* 04 48 30.6399634800 +16 23 18.723286140   13.89 12.427 12.057   ~ 40 0
23 HD 286085 PM* 04 50 00.7134564816 +16 24 43.417726236   11.58 10.69     K6 67 0
24 HD 284930 PM* 04 52 23.5314653976 +18 59 48.866831160   11.351 10.280     K0 84 0
25 HD 240629 ** 05 05 40.3801057412 +06 27 54.724586153   10.849 9.880 9.631   K2 74 0
26 NGC 3532 OpC 11 05 33.9 -58 42 13           ~ 414 0
27 * lam And RS* 23 37 33.8427800830 +46 27 29.344721109 5.54 4.84 3.82 3.04 2.47 G8IVk 693 0

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