2025AJ....170..181I


Query : 2025AJ....170..181I

2025AJ....170..181I - Astron. J., 170, 181 (2025/September-0)

The California Legacy Survey. VI. The Fate of Activity Cycles in Sun-like Stars.

ISAACSON H., KANE S.R., CARTER B. and HOWARD A.W.

Abstract (from CDS):

We analyze the spectra of 91 solar-type G- and K-type main-sequence dwarfs in the solar neighborhood to assess activity trends with stellar properties. As a follow-on work to our studies of the decoupling of rotation from age, we use chromospheric activity time series data to probe changes in stellar activity cycles as further evidence of differences in magnetic dynamos. We present evidence that the average chromospheric activity remains nearly constant while the variation in a star's activity decreases by an order of magnitude. Measurable changes to the stellar dynamo are suggested that are not strongly correlated with the average stellar activity, but instead correlated with the amplitude of activity variations for stars beyond the age of the Sun. In contrast, while the activity cycle period is strongly correlated with effective temperature for stars aged between 2 and 4 Gyr, we find no such correlation for stars older than the Sun or otherwise low-activity stars beyond ${\mathrm{log}}\,({R}_{\mathrm{HK}}^{{\prime} })$ = -4.90. By quantifying the Ca II H and K activity variation over the timescales of stellar cycles, we suggest that age dating of mature-age solar-type stars requires knowledge of activity variability in addition to the average activity.

Abstract Copyright: © 2025. The Author(s). Published by the American Astronomical Society.

Journal keyword(s): Stellar activity - Stellar chromospheres - Stellar ages - Stellar rotation

Simbad objects: 19

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Number of rows : 19
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 * eta Cas PM* 00 49 06.2945942922 +57 48 54.638239716 4.04 4.02 3.44 2.94 2.58 F9V 680 0
2 HD 4915 PM* 00 51 10.8478903584 -05 02 21.401155212 7.792 7.643 6.972 6.604 6.252 G5V 163 0
3 * tau Cet PM* 01 44 04.0831371922 -15 56 14.927607677 4.43 4.22 3.50 2.88 2.41 G8V 1354 1
4 * 51 Ari PM* 03 02 26.0263370112 +26 36 33.260418324       6.2   G8V 176 0
5 HD 38858 PM* 05 48 34.9402551240 -04 05 40.721787744 6.71 6.61 5.97     G2V 349 1
6 HD 42618 PM* 06 12 00.5668858951 +06 46 59.057784676 7.632 7.496 6.839 6.478 6.143 G4V 214 0
7 HD 45184 PM* 06 24 43.8795895848 -28 46 48.415725948   7.01 6.39 6.24 8.94 G2Va 238 1
8 HD 52711 PM* 07 03 30.4592307736 +29 20 13.493121298 6.57 6.53   5.6   G0V 280 0
9 * 20 LMi PM* 10 01 00.6568762394 +31 55 25.213014837   6.05 5.37 4.9   G3VaHdel1 430 0
10 * 47 UMa PM* 10 59 27.9727514012 +40 25 48.920572724   5.66   4.7   G1-VFe-0.5 824 1
11 * 10 CVn PM* 12 44 59.4049642264 +39 16 44.098132297 6.47 6.50 5.95 5.41 5.12 F9V_Fe-0.3 400 0
12 * 61 Vir PM* 13 18 24.3139864471 -18 18 40.297748582 5.710 5.440 4.740     G6.5V 742 1
13 HD 126053 PM* 14 23 15.2847745835 +01 14 29.641269692 6.98 6.90 6.27 5.71 5.39 G1.5V 442 0
14 * nu.02 Lup PM* 15 21 48.1499105161 -48 19 03.469906910 6.35 6.30 5.65     G2-V 354 1
15 * sig CrB B PM* 16 14 40.3874065885 +33 51 27.096186894   7.04 6.42     G1V 146 0
16 * sig CrB A SB* 16 14 40.8534439608 +33 51 31.011629868   6.14 5.55     F6V 68 1
17 HD 166620 PM* 18 09 37.4162111401 +38 27 27.998016381 7.86 7.27 6.40 5.63 5.14 K2V 481 0
18 HD 190067 PM* 20 02 34.1553139987 +15 35 31.468310729 8.098 7.854 7.115 6.696 6.304 K0VFe-0.9 151 0
19 HD 221354 PM* 23 31 22.2087431778 +59 09 55.867801045   7.57   6.2   K0V 190 0

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