2020A&A...638A.115H


Query : 2020A&A...638A.115H

2020A&A...638A.115H - Astronomy and Astrophysics, volume 638A, 115-115 (2020/6-1)

The CARMENES search for exoplanets around M dwarfs. The He I infrared triplet lines in PHOENIX models of M 2-3 V stars.

HINTZ D., FUHRMEISTER B., CZESLA S., SCHMITT J.H.M.M., SCHWEITZER A., NAGEL E., JOHNSON E.N., CABALLERO J.A., ZECHMEISTER M., JEFFERS S.V., REINERS A., RIBAS I., AMADO P.J., QUIRRENBACH A., ANGLADA-ESCUDE G., BAUER F.F., BEJAR V.J.S., CORTES-CONTRERAS M., DREIZLER S., GALADI-ENRIQUEZ D., GUENTHER E.W., HAUSCHILDT P.H., KAMINSKI A., KURSTER M., LAFARGA M., LOPEZ DEL FRESNO M., MONTES D. and MORALES J.C.

Abstract (from CDS):

The HeI infrared (IR) line at a vacuum wavelength of 10833Å is a diagnostic for the investigation of atmospheres of stars and planets orbiting them. For the first time, we study the behavior of the HeIIR line in a set of chromospheric models for M-dwarf stars, whose much denser chromospheres may favor collisions for the level population over photoionization and recombination, which are believed to be dominant in solar-type stars. For this purpose, we use published PHOENIX models for stars of spectral types M2 V and M3 V and also compute new series of models with different levels of activity following an ansatz developed for the case of the Sun. We perform a detailed analysis of the behavior of the HeIIR line within these models. We evaluate the line in relation to other chromospheric lines and also the influence of the extreme ultraviolet (EUV) radiation field. The analysis of the HeIIR line strengths as a function of the respective EUV radiation field strengths suggests that the mechanism of photoionization and recombination is necessary to form the line for inactive models, while collisions start to play a role in our most active models. Moreover, the published model set, which is optimized in the ranges of the NaI D2, Hα, and the bluest CaIIIR triplet line, gives an adequate prediction of the HeIIR line for most stars of the stellar sample. Because especially the most inactive stars with weak HeIIR lines are fit worst by our models, it seems that our assumption of a 100% filling factor of a single inactive component no longer holds for these stars.

Abstract Copyright: © ESO 2020

Journal keyword(s): stars: activity - stars: chromospheres - stars: late-type

Simbad objects: 50

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Number of rows : 50
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2024
#notes
1 Wolf 1056 PM* 00 38 59.0443396237 +30 36 58.387586417   12.60   10.6   M2.5V 96 0
2 Wolf 44 PM* 01 01 20.0492200601 +61 21 56.681648637   12.26 10.87     M2.0V 92 1
3 BD+70 68a * 01 01 29.6446208664 +71 41 02.412982860   11.39 10.28     ~ 5 0
4 G 3-14 PM* 01 43 20.1790598651 +04 19 17.959793419 13.64 12.45 10.915 9.879 8.614 M2V 150 0
5 G 244-47 PM* 02 01 35.3407161312 +63 46 11.997406488       10.630   M2.5V 69 0
6 V* VX Ari Er* 02 44 15.5097410539 +25 31 24.114854200 13.363 12.141 10.563 9.49 8.115 dM3 220 0
7 Ross 567 PM* 03 53 10.4354617848 +62 34 08.066015328       11.084   M3.0V 43 0
8 HD 285968 PM* 04 42 55.7750207949 +18 57 29.395947044 12.668 11.49 9.951 8.931 7.702 M2.5V 335 2
9 G 222-11 PM* 06 10 19.8468098360 +82 06 24.318574744   12.214   9.5   M2.5V 122 0
10 G 250-33 PM* 07 04 25.9413809225 +68 17 19.653201657     11.99 11.460   M3.0V 60 0
11 G 112-21 PM* 07 28 45.4392980865 -03 17 53.314880583 14.298 13.023 11.456 10.351 8.954 M3V 82 0
12 MCC 499 PM* 07 35 21.8791699200 +54 50 58.969242060   12.93 11.325 10.868   M2.5V 58 0
13 G 234-57 ** 09 13 23.849448 +68 52 30.70416   12.767 11.168 10.760   M2.5Ve 43 0
14 L 678-39 EB* 09 36 01.6372169407 -21 39 38.877606712 13.647 12.48 10.906 9.858 8.577 M2.5V 159 0
15 G 236-1 PM* 09 42 34.8407291884 +70 02 01.964331947   11.86 10.58 9.53 8.24 M2.5Ve 94 0
16 MCC 573 PM* 10 16 45.9486335041 -11 57 42.405573294 13.559 12.464 10.998 9.953 8.624 dM3.0 92 0
17 G 162-70 PM* 10 35 01.1174982552 -09 24 38.578905216   13.66 12.110 11.02 9.63 dM3.0 32 0
18 G 55-35 PM* 10 39 40.5638632278 -06 55 25.507022782 13.939 12.79 11.281 10.244 8.961 dM2.5 86 0
19 Ross 104 PM* 11 00 04.2570074282 +22 49 58.645009946 12.826 11.584 10.020 8.952 7.646 M4V 184 0
20 LP 733-99 LM* 11 20 06.1045187904 -10 29 46.727203956   12.734 11.250 10.887   M2.0V 49 0
21 Ross 905 PM* 11 42 11.0933350978 +26 42 23.650782778   12.06 10.613 10.272 8.24 M3V 645 1
22 LP 733-71 PM* 11 46 42.9131118835 -14 00 51.785571654 14.331 13.19 11.700 10.639 9.287 M3V 84 0
23 Ross 690 PM* 12 23 00.1603475794 +64 01 50.965179127   13.23 13.481 10.9   M3V 79 0
24 Ross 695 PM* 12 24 52.5030065444 -18 14 32.257135052 13.954 12.863 11.272 10.243 8.991 dM2.0 127 0
25 * tau Boo B * 13 47 15.3324773299 +17 27 26.432463096     11.1     M3V 33 0
26 Ross 992 PM* 14 15 16.9799792836 +45 00 53.282434981       11.499   M3V 53 0
27 Ross 1047 PM* 15 09 35.5922555405 +03 10 00.552794932 14.131 12.986 11.473 10.405 9.052 M2V 78 0
28 G 152-50 SB* 15 47 24.5487998193 -10 53 47.266942275 14.179 12.88 11.279 10.213 8.907 M2.5V 58 1
29 G 137-84 PM* 16 09 16.2650806623 +09 21 07.546478830   11.5   11.398   M3.0Ve 30 0
30 HD 147379B BY* 16 16 45.3144811630 +67 15 22.481125328   12.20   10.310   M3.0V 144 0
31 G 202-48 PM* 16 25 24.6230388531 +54 18 14.765465640   11.78 10.07 9.66   M1.5V 207 0
32 G 138-39 PM* 16 32 45.1914759119 +12 36 45.996003308 14.65 13.642 12.158 11.115 9.771 M3.0V 56 0
33 G 138-64 PM* 16 46 13.7424594567 +16 28 40.792117609 14.346 13.15 11.68 11.28 9.272 M3.0V 66 0
34 Ross 863 PM* 17 07 07.4897699547 +21 33 14.472908816 14.435 13.248 11.677 10.579 9.239 M3V 93 0
35 G 139-27 PM* 17 16 40.9809159936 +08 03 30.206482884 14.301 13.087 11.529 10.48 9.219 M2.5V 76 0
36 G 181-39 PM* 17 19 52.7123256416 +41 42 49.699619416   11.423   10.4   M2V 95 0
37 G 204-39 PM* 17 57 50.9660613981 +46 35 19.127676045   13.97 11.64 11.3   M2.5V 82 0
38 V* V401 Dra BY* 18 17 25.1255884056 +48 22 02.331245064   12.81 11.37 10.91   dM2.0 43 0
39 Ross 145 PM* 18 41 59.0357706782 +31 49 49.763356483   12.84 13.126 10.845   M2V 86 0
40 G 155-42 PM* 18 48 01.2689841187 -14 34 51.198310862   13.64 12.13 11.738   dM2.5 37 0
41 Ross 730 PM* 19 07 05.5646181264 +20 53 16.940417573 13.54 12.397 10.774 9.745 8.543 M2.0V 160 0
42 HD 349726 PM* 19 07 13.2039504383 +20 52 37.258158623 13.553 12.383 10.771 9.739 8.531 M2V 164 0
43 G 262-15 PM* 20 30 32.0453969319 +65 26 58.411357864   12.00   10.124   M3V 165 0
44 Wolf 896 PM* 20 56 46.5969248424 -10 26 54.747253252 14.112 12.999 11.487 10.428 9.106 dM2.5 101 0
45 Wolf 906 PM* 21 01 58.6411604621 -06 19 07.472265720 13.883 12.748 11.276 10.912 8.86 M2.5V 90 0
46 LSPM J2116+0234 PM* 21 16 27.2844602256 +02 34 51.392019432   13.4   11.639   M3.0V 37 0
47 BD-05 5715 PM* 22 09 40.3443137051 -04 38 26.650757960 13.006 11.868 10.366 9.279 7.877 M3.5V 286 1
48 Wolf 1014 PM* 22 12 35.9448323372 +08 33 11.611207118 14.713 13.545 11.982 10.913 9.581 M3.0V 71 0
49 BD-17 6785 PM* 23 38 08.1567206712 -16 14 10.201491564   12.830 11.288 11.079 9.08 M2V 58 0
50 Wolf 1051 SB* 23 58 32.6519707715 +07 39 30.055027679 14.382 13.258 11.739 10.654 9.277 M3.0V 58 0

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