2023ApJ...951...90W


Query : 2023ApJ...951...90W

2023ApJ...951...90W - Astrophys. J., 951, 90 (2023/July-2)

Stellar Characterization and Radius Inflation of Hyades M-dwarf Stars from the APOGEE Survey.

WANDERLEY F., CUNHA K., SOUTO D., SMITH V.V., CAO L., PINSONNEAULT M., ALLENDE PRIETO C., COVEY K., MASSERON T., PASCUCCI I., STASSUN K.G., TERRIEN R., BERGSTEN G.J., BIZYAEV D., FERNANDEZ-TRINCADO J.G., JONSSON H., HASSELQUIST S., HOLTZMAN J.A., LANE R.R., MAHADEVAN S., MAJEWSKI S.R., MINNITI D., PAN K., SERNA J., SOBECK J. and STRINGFELLOW G.S.

Abstract (from CDS):

We present a spectroscopic analysis of a sample of 48 M-dwarf stars (0.2M⊙ < M < 0.6 M⊙) from the Hyades open cluster using high-resolution H-band spectra from the Sloan Digital Sky Survey/Apache Point Observatory Galactic Evolution Experiment (APOGEE) survey. Our methodology adopts spectrum synthesis with LTE MARCS model atmospheres, along with the APOGEE Data Release 17 line list, to determine effective temperatures, surface gravities, metallicities, and projected rotational velocities. The median metallicity obtained for the Hyades M dwarfs is [M/H] = 0.09 ± 0.03 dex, indicating a small internal uncertainty and good agreement with optical results for Hyades red giants. Overall, the median radii are larger than predicted by stellar models by 1.6% ± 2.3% and 2.4% ± 2.3%, relative to a MIST and DARTMOUTH isochrone, respectively. We emphasize, however, that these isochrones are different, and the fractional radius inflation for the fully and partially convective regimes have distinct behaviors depending on the isochrone. Using a MIST isochrone there is no evidence of radius inflation for the fully convective stars, while for the partially convective M dwarfs the radii are inflated by 2.7% ± 2.1%, which is in agreement with predictions from models that include magnetic fields. For the partially convective stars, rapid rotators present on average higher inflation levels than slow rotators. The comparison with SPOTS isochrone models indicates that the derived M-dwarf radii can be explained by accounting for stellar spots in the photosphere of the stars, with 76% of the studied M dwarfs having up to 20% spot coverage, and the most inflated stars with ∼20%-40% spot coverage.

Abstract Copyright: © 2023. The Author(s). Published by the American Astronomical Society.

Journal keyword(s): M dwarf stars - Near infrared astronomy - Open star clusters - Stellar activity - Metallicity

Simbad objects: 57

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Number of rows : 57
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 LP 413-24 PM* 03 39 07.1296199856 +20 25 26.699785896   16.5   14.1   M4.5 34 0
2 LP 356-778 PM* 03 41 36.9052220856 +23 20 37.356133488   15.33   12.4   M: 40 0
3 LP 413-89 PM* 03 41 55.4900293176 +18 45 35.769378672   14.87 13.266 13.030   ~ 41 0
4 LP 413-93 PM* 03 43 47.0794972272 +20 51 36.343033776     14.54     ~ 37 0
5 Cl Melotte 22 OpC 03 46 38.0 +24 10 41           ~ 3679 0
6 2MASS J03534647+1323312 PM* 03 53 46.4932620480 +13 23 31.151437836           ~ 21 0
7 LP 474-28 LM* 03 58 14.3643428664 +12 37 40.884533796           ~ 31 0
8 LP 357-279 PM* 03 58 54.5335914096 +25 13 11.279044380   15.59 14.03     M2.6 30 0
9 HG 8-59 PM* 03 59 14.1879749064 +22 02 37.884757812     13.066 12.598   ~ 41 0
10 LP 414-30 PM* 04 00 15.5839347360 +19 24 36.529740108   17.89 16.17     ~ 42 0
11 K2-25 PM* 04 13 05.6131374072 +15 14 52.018080576   15.81 15.56 13.72   M4.5V 108 0
12 HG 7-150 PM* 04 17 28.1413374096 +14 54 03.817587888   16.01 14.47 14.46   M3 52 0
13 HG 7-154 PM* 04 17 51.6258147336 +15 13 37.778242404   17.131 15.596 13.476   M3: 51 0
14 LP 414-158 PM* 04 18 33.8482883496 +18 21 53.000536788     16.09   13.29 M3.6 43 0
15 HG 7-163 PM* 04 19 03.0986676144 +19 32 39.552153756   15.28       ~ 33 0
16 LP 358-685 Er* 04 19 29.7843231048 +21 45 13.982294412   15.55 14.03     ~ 39 0
17 LP 415-543 PM* 04 20 27.6272249568 +18 53 49.921871856   15.34 15.24     M3.9 39 0
18 LP 358-722 PM* 04 23 57.4054495008 +22 10 53.733967968     15.18     ~ 33 0
19 LP 415-50 PM* 04 24 20.9451702384 +19 10 50.818114992   18.47 16.68     M4.8 41 0
20 LP 358-268 PM* 04 27 03.1391394120 +24 06 15.756803352           ~ 31 0
21 V* V1103 Tau BY* 04 29 01.0133482776 +18 40 25.322063340   14.751 13.310 12.982   M2.5V 63 0
22 LP 358-730 PM* 04 29 10.9876446624 +26 14 48.317186112   14.42 12.910 12.569   ~ 34 0
23 LP 358-351 PM* 04 29 37.3969001856 +21 40 07.116218148   15.76 14.21     ~ 32 0
24 HG 7-244 PM* 04 29 55.7394509088 +16 54 50.582358432   14.31 12.820 12.407   ~ 58 0
25 LP 358-352 PM* 04 30 17.0360433720 +26 22 26.261846184     16.50     M4.5V 33 0
26 Cl Melotte 25 OpC 04 30 27.4 +16 46 43           ~ 3309 0
27 LP 415-165 PM* 04 31 11.0207446152 +16 23 45.140411652   16.71 15.13 15.08   ~ 44 0
28 Cl* Melotte 25 VA 674 PM* 04 32 28.9806260592 +17 54 16.701872148   17.07 15.46 15.11   ~ 38 0
29 LP 415-2120 Em* 04 33 42.8134443504 +18 45 59.175582372   17 15.37     M4.5e 35 0
30 LP 415-208 PM* 04 33 55.4666760312 +18 22 50.752855344   17.80 16.48 16.22   ~ 34 0
31 LP 415-1379 PM* 04 33 56.7186713304 +16 52 08.627544444   16.70 15.09 14.80   M1 40 0
32 2MASS J04350330+2451146 PM* 04 35 03.3088186920 +24 51 14.516491104           ~ 14 0
33 Cl* Melotte 25 REID 355 ** 04 36 30.811560 +19 05 27.21804   16.32 14.73 15.02   ~ 13 0
34 LP 415-1619 PM* 04 36 38.9458035168 +18 36 56.713956768   14.82 13.338 12.986   M2.0V 53 0
35 2MASS J04370517+2043054 PM* 04 37 05.1735578952 +20 43 05.347971444           ~ 28 0
36 LP 415-292 PM* 04 38 54.7206035184 +19 10 55.986372984   15.55 14.04 13.70   ~ 36 0
37 HG 8-68 PM* 04 40 12.7100600088 +19 17 09.948013944   15.05 13.577 13.287   M2.43 41 0
38 LP 415-1816 TT? 04 40 28.2712249440 +18 05 16.011614508   16.66 15.01     ~ 33 0
39 LP 415-348 PM* 04 42 18.8217611760 +17 41 38.282956008   15.02       ~ 31 0
40 2MASS J04425217+2320224 PM* 04 42 52.1709767184 +23 20 22.494061464           ~ 27 0
41 LP 415-3051 PM* 04 42 58.4852303832 +20 36 17.407635012     15.06     ~ 29 0
42 LP 416-572 PM* 04 49 11.0861326584 +17 42 55.559736648   15.52 14.00     ~ 30 0
43 UCAC4 536-010184 PM* 04 49 36.5795629608 +17 01 59.070867168       14.15   ~ 26 0
44 2MASS J04501665+2037330 Em* 04 50 16.6696789824 +20 37 32.967777756           M4.5e 33 0
45 LP 416-130 PM* 04 54 44.1105864672 +19 40 51.236942448   15.43 13.89     ~ 28 0
46 UCAC4 557-011753 PM* 04 55 14.8558821840 +21 21 50.574396096           ~ 27 0
47 2MASS J04561668+2122019 PM* 04 56 16.6948237632 +21 22 01.918106184           ~ 23 0
48 2MASS J04574644+1628202 PM* 04 57 46.4446677624 +16 28 20.324653608           M3 24 0
49 2MASS J04575778+1427071 PM* 04 57 57.7907039352 +14 27 07.224325380           M2 27 0
50 2MASS J05011599+1608409 LM* 05 01 16.0005968064 +16 08 40.866396000           ~ 24 0
51 NGC 2264 OpC 06 40 53.7 +09 52 32           ~ 1876 0
52 V* YY Gem SB* 07 34 37.4474327544 +31 52 10.179641496 11.60 10.56 9.27 7.69 6.67 M0.5VeFe-2 882 0
53 NGC 2516 OpC 07 58 00.5 -60 46 36           ~ 793 0
54 NGC 2547 OpC 08 10 01.5 -49 12 08           ~ 445 0
55 NSVS 7394765 EB* 08 25 51.8920686720 +24 27 04.604802912           ~ 17 0
56 V* GU Boo EB* 15 21 54.8243257728 +33 56 09.067285032     13.11     M0/M1.5 99 0
57 [DCO2008] T-Cyg1-12664 EB* 19 51 39.8192840592 +48 19 55.437246624   14.240   13.315   G3V 39 0

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