2025A&A...698A...7F


Query : 2025A&A...698A...7F

2025A&A...698A...7F - Astronomy and Astrophysics, volume 698A7 (2025/6-1)

LAMOST medium-resolution observations of the Pleiades.

FRASCA A., ZHANG J.Y., ALONSO-SANTIAGO J., FU J.N., MOLENDA-ZAKOWICZ J., DE CAT P. and CATANZARO G.

Abstract (from CDS):

Aims. In this work, we present the results of our analysis of medium-resolution LAMOST spectra of late-type candidate members of the Pleiades with the aim of determining the stellar parameters, activity level, and lithium abundance.
Methods. We used the ROTFIT code to determine the atmospheric parameters (Teff, log g, and [Fe/H]), along with the radial velocity (RV) and projected rotation velocity (v sin i). Moreover, for late-type stars (Teff ≤ 6500 K), we also calculated the Hα and Li Iλ6708 net equivalent width by means of the subtraction of inactive photospheric templates. We also used the rotation periods from the literature and we purposely determined them for 89 stars by analyzing the available Transiting Exoplanet Survey Satellite (TESS) photometry.
Results. We derived the RV, v sin i, and atmospheric parameters for 1581 spectra of 283 stars. Literature data were used to assess the accuracy of the derived parameters. The RV distribution of the cluster members peaks at 5.0 km s–1 with a dispersion of 1.4 km s–1, while the average metallicity is [Fe/H]=-0.03±0.06, in line with previous determinations. Fitting empirical isochrones of Li depletion to EW measures of stars with Teff ≤ 6500 K, we obtained a reliable age for the Pleiades of 118±6 Myr, in agreement with the recent literature. The activity indicators Hα line flux (FHα) and luminosity ratio (R'Hα) show the hottest stars to be less active (on average) than the coldest ones, as expected for a 100-Myr old cluster. When plotted against the Rossby number, RO, our R'Hα values display a typical activity-rotation trend, with a steep decay for RO ≥ 0.2 and a nearly flat (saturated) activity level for smaller values. However, we still see a slight dependence on RO in the saturated regime, which is well fitted by a power law with a slope of -1.18 ± 0.02; this is in agreement with a number of previous works. For three sources with multi-epoch data, we had access to LAMOST spectra acquired during flares, which are characterized by strong and broad Hα profiles and the presence of the He Iλ6678 Å emission line. Among our targets, we identified 39 possible SB1 and ten SB2 systems. We have also shown the potential of the LAMOST-MRS spectra in allowing us to refine the orbital solution of a number of binaries and to discover a new double-lined binary as well.

Abstract Copyright: © The Authors 2025

Journal keyword(s): stars: abundances - stars: activity - binaries: spectroscopic - stars: flare - stars: fundamental parameters - open clusters and associations: individual: Pleiades

VizieR on-line data: <Available at CDS (J/A+A/698/A7): table1.dat table3.dat table4.dat tablea2.dat>

Status at CDS : Tables of objects will be appraised for possible ingestion in SIMBAD.

Simbad objects: 58

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Number of rows : 58
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 Cl Melotte 20 MGr 03 26 50.6 +48 51 48           ~ 928 0
2 BSD 47-525 Em* 03 31 03.3397547136 +31 19 14.301200064   12.27 11.46     K1 11 0
3 HIP 17020 Y*O 03 38 56.8648730744 +24 34 11.314278699   11.180 10.578 10.469 9.794 ~ 67 0
4 Cl* Melotte 22 DH 184 PM* 03 41 39.5818216522 +23 45 47.130989524 17.272 16.025 14.583   12.770 M1.5 58 0
5 V* LO Tau Er* 03 42 40.2234476357 +23 59 21.705715226   17.07 15.72   13.29 M2.9 72 0
6 2MASS J03434860+2332218 Y*O 03 43 48.6023686968 +23 32 21.806723760 16.839 15.39 14.02     M1.1 76 0
7 V* MS Tau PM* 03 43 55.6869949730 +24 25 35.099244442   15.705 14.339   12.539 M1.5 89 0
8 BD+23 502A * 03 44 14.6299858032 +24 06 07.587808128           ~ 21 0
9 HD 23232 * 03 44 20.2200174192 +24 52 29.756321364   10.46 8.848     K2 22 0
10 HD 23246 PM* 03 44 25.7165880744 +24 23 40.975909332   8.44 8.18     A8V 94 0
11 Cl Melotte 22 370 A * 03 44 32.0001429480 +23 52 30.184169664           ~ 20 0
12 2MASS J03443541+2400048 Y*O 03 44 35.4064162377 +24 00 04.817154001   15.760 14.329   12.582 M1.0 66 0
13 Cl* Melotte 22 DH 352 Em* 03 44 41.8184993240 +22 27 52.371554393   11.473 10.757   9.954 ~ 53 0
14 V* V785 Tau PM* 03 44 50.1780343951 +24 54 40.045323288   14.53 13.34   12.00 K5Ve 91 0
15 Cl Melotte 22 513 Y*O 03 44 58.9560256802 +23 23 20.175395617 16.692 15.09 13.77     M1.2 77 0
16 Cl Melotte 22 517 * 03 45 01.4836794792 +24 05 32.515022220   14.3       ~ 5 0
17 2MASS J03451534+2517221 Y*O 03 45 15.3524954712 +25 17 22.129906236   11.8 11.3   10.35 G8V 70 0
18 HD 23375 dS* 03 45 34.4631249960 +24 27 47.922382692   8.94 8.58   8.33 F0V 113 0
19 V* V1085 Tau BY* 03 45 35.3982230827 +24 04 59.563296540   10.73 11.92 10.04 9.37 F2 103 0
20 V* V855 Tau Y*O 03 45 40.1782648711 +24 37 38.007136109   10.6 9.9   9.05 F9V 108 1
21 V* V969 Tau BY* 03 45 42.1185203606 +24 54 21.622880032   10.18 9.56   8.82 G3 145 1
22 Cl Melotte 22 761 Y*O 03 45 44.4132583283 +24 13 13.134939048   11.22 10.55   9.77 G2V 93 0
23 V* OW Tau Y*O 03 45 48.9406173551 +23 51 10.397233543   15.63 14.27 13.83 12.51 M1.2 79 0
24 BD+23 521 * 03 46 17.9919005844 +23 29 11.939258173 11.984 11.4 10.6   9.59 F8V 71 0
25 HD 282952 Y*O 03 46 27.3523093248 +25 08 07.920713904   11.3 10.9     F9 91 0
26 V* PR Tau Er* 03 46 35.3297089922 +23 24 42.229120112   16.25 14.77   12.85 M1.7 82 0
27 V* V642 Tau Er* 03 46 37.284936 +24 20 36.71124   13.362 12.321 11.964 10.97 K5V 87 0
28 V* V642 Tau A PM* 03 46 37.3039349414 +24 20 36.748414421           ~ 5 0
29 2MASS J03463777+2444517 Y*O 03 46 37.7719499679 +24 44 51.681848077   12.80 11.92   10.89 K0V 88 0
30 Cl Melotte 22 OpC 03 46 38.0 +24 10 41           ~ 3679 0
31 V* V1065 Tau RS* 03 46 40.2476949658 +23 29 51.877806260 14.016 13.01 12.02   10.93 K0 99 0
32 BD+22 552 Y*O 03 46 47.0620046173 +22 54 52.487006394   11.3 10.8   9.77 F8 98 0
33 V* V534 Tau dS* 03 47 03.5551874064 +24 49 11.812255356   8.65 8.30   7.83 A9V 120 0
34 V* QQ Tau Er* 03 47 03.7754677449 +23 36 58.721846410   17.03 15.35 14.95 12.89 M2.5Ve 77 0
35 V* V536 Tau Y*O 03 47 09.4374407542 +23 44 31.855919375         12.85 M3Ve 75 0
36 Cl* Melotte 22 HHJ 417 Er* 03 47 20.8285882212 +25 05 12.372242448   17.321 15.699   13.399 M2.2 58 0
37 Cl* Melotte 22 PELS 66 Er* 03 47 34.1645066613 +21 44 48.521290070   13.341 12.325   11.224 ~ 47 0
38 V* V1172 Tau BY* 03 47 38.0074370120 +23 28 04.974381557   14.87 13.50   12.10 K1 83 0
39 V* V869 Tau Er* 03 48 16.4191457736 +22 32 40.553078100   16.066 14.667   12.754 M: 19 0
40 V* V343 Tau Y*O 03 48 17.2906550111 +24 30 15.934120758   15.69 14.29     M1.4 81 0
41 Cl Melotte 22 2126 Y*O 03 49 02.3336482213 +23 15 08.771656641   12.50 11.64   10.80 K0V 88 0
42 V* V357 Tau BY* 03 49 11.2836053136 +23 33 18.809901180   15.60 14.23   12.50 M1.7 64 0
43 HD 282965 SB* 03 49 11.7330709952 +24 38 11.688977570 11.15 11.2 10.6 9.88 9.74 F9V 85 0
44 Cl Melotte 22 2311 Y*O 03 49 28.7425971397 +23 42 43.885888515   12.19 11.36   10.50 ~ 92 0
45 Cl Melotte 22 2406 Y*O 03 49 39.4016007216 +23 17 24.383128632   11.86 11.10     G1 73 0
46 V* V371 Tau A * 03 50 12.8625710651 +24 21 06.525590359           ~ 24 0
47 V* V371 Tau Y*O 03 50 12.876576 +24 21 06.71724   16.56 15.11 14.94 12.68 M3Ve 42 0
48 V* V1091 Tau Er* 03 50 35.7229146744 +25 25 35.421006037   13.026 12.095   10.987 ~ 55 0
49 V* V1175 Tau BY* 03 50 40.0721202291 +23 55 58.950949335   10.9 10.5   9.61 F9 110 0
50 ZTF J035046.05+225549.6 RS* 03 50 46.0312695988 +22 55 50.436642748   14.01 12.86 12.48   ~ 33 0
51 2MASS J03512213+2509580 Y*O 03 51 22.1363944477 +25 09 58.070915302   15.69 14.23     M1.0 46 0
52 TYC 1261-573-1 EB* 03 53 19.9634477856 +21 57 06.218523504   11.99 11.48     F8 15 0
53 V* V399 Tau BY* 03 53 57.2707965801 +23 20 43.086630632   15.60 14.26   12.48 M2.5 44 0
54 V* V889 Tau SB* 03 54 52.5651385631 +24 34 34.497430118   14.510 13.167   11.587 M0 53 0
55 Cl* Melotte 22 PELS 180 * 04 08 38.7636026592 +23 38 04.452272592   12.01 11.46     ~ 8 0
56 Cl Melotte 25 OpC 04 30 27.4 +16 46 43           ~ 3309 0
57 IC 2602 OpC 10 42 55.9 -64 25 22           ~ 735 0
58 NGC 6475 OpC 17 53 44.1 -34 49 36           ~ 413 0

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