2017A&A...604A..97L


Query : 2017A&A...604A..97L

2017A&A...604A..97L - Astronomy and Astrophysics, volume 604A, 97-97 (2017/8-1)

Metallicity determination of M dwarfs. Expanded parameter range in metallicity and effective temperature.

LINDGREN S. and HEITER U.

Abstract (from CDS):

Context. Reliable metallicity values for late K and M dwarfs are important for studies of the chemical evolution of the Galaxy and advancement of planet formation theory in low-mass environments. Historically it has been challenging to determine the stellar parameters of low-mass stars because of their low surface temperature, which causes several molecules to form in the photospheric layers. In our work we use the fact that infrared high-resolution spectrographs have opened up a new window for investigating M dwarfs. This enables us to use similar methods as for warmer solar-like stars.
Aims. Metallicity determination with high-resolution spectra is more accurate than with low-resolution spectra, but it is rather time consuming. In this paper we expand our sample analyzed with this precise method both in metallicity and effective temperature to build a calibration sample for a future revised empirical calibration.
Methods. Because of the relatively few molecular lines in the J band, continuum rectification is possible for high-resolution spectra, allowing the stellar parameters to be determined with greater accuracy than with optical spectra. We obtained high-resolution spectra with the CRIRES spectrograph at the Very Large Telescope (VLT). The metallicity was determined using synthetic spectral fitting of several atomic species. For M dwarfs that are cooler than 3575K, the line strengths of FeH lines were used to determine the effective temperatures, while for warmer stars a photometric calibration was used.
Results. We analyzed 16 targets with a range of effective temperature from 3350-4550K. The resulting metallicities lie between -0.5<[M/H]<+0.4. A few targets have previously been analyzed using low-resolution spectra and we find a rather good agreement with our values. A comparison with available photometric calibrations shows varying agreement and the spread within all empirical calibrations is large.
Conclusions. Including the targets from our previous paper, we analyzed 28 M dwarfs with high-resolution infrared spectra. The targets spread approximately one dex in metallicity and 1400K in effective temperature. For individual M dwarfs we achieve uncertainties of 0.05dex and 100K on average.

Abstract Copyright: © ESO, 2017

Journal keyword(s): stars: low-mass - stars: abundances - techniques: spectroscopic - techniques: spectroscopic

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 - 2024
#notes
1 CD-23 1056 PM* 02 46 42.8869269570 -23 05 11.802392748 12.911 11.651 10.237 9.36 8.544 K5V 65 1
2 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
3 Wolf 1539 PM* 04 52 05.7321216445 +06 28 35.588676189 14.791 13.568 12.018 10.854 9.334 M2V 158 1
4 Ross 41 PM* 05 28 00.1514481321 +09 38 38.155965013 15.341 14.082 12.443 11.272 9.788 M3.5V 117 0
5 BD+10 1032 ** 06 10 54.80387 +10 19 04.9946 12.9 11.844 10.385 9.365 8.065 M2.5V 70 0
6 CD-61 1439 Er* 06 39 50.0234724000 -61 28 41.530139940 12.224 11.043 9.746 9.11 8.223 K7V(e) 79 0
7 HD 50281B ** 06 52 18.0415140183 -05 11 24.042331473   11.47 10.05 9.870   M2.5V 123 0
8 L 675-81 Pe* 08 40 59.2057867166 -23 27 22.592748045   13.2 11.975 11.637 9.37 M3.5V 146 1
9 BD-08 2582 PM* 09 06 45.3496653632 -08 48 24.614510228 12.184 10.928 9.478 8.564 7.653 K7V 85 0
10 CD-30 8858 PM* 10 58 35.0883696526 -31 08 38.200769022     11.926 11.588 9.63 M2 53 1
11 BD-01 2505 PM* 11 17 13.6639950829 -01 58 54.674999195   10.95 9.878 9.804   K4/5V 56 0
12 CD-31 9113 PM* 11 35 26.9477670462 -32 32 23.884215079 12.508 11.322 9.813 8.821 7.664 M2V 157 1
13 Ross 905 PM* 11 42 11.0933350978 +26 42 23.650782778   12.06 10.613 10.272 8.24 M3V 645 1
14 TYC 8638-366-1 PM* 11 43 31.4394151504 -57 59 12.557409442   11.69 10.59 9.89 9.20 M0-M1 9 0
15 L 399-68 PM* 12 40 46.2893984278 -43 33 58.991739064 15.365 13.969 12.239 11.075 9.619 M3V 67 0
16 BD+11 2576 PM* 13 29 59.7858994351 +10 22 37.784532575 11.728 10.524 9.029 8.07 7.013 M1.0V 257 0
17 BD-07 4003 BY* 15 19 26.8269387505 -07 43 20.189497466 13.403 11.76 10.560 9.461 8.911 M3V 641 2
18 BD-12 4523 BY* 16 30 18.0583947383 -12 39 45.321217732 12.829 11.638 10.072 8.917 7.421 M3V 315 0
19 CD-46 11540 LM* 17 28 39.9455781571 -46 53 42.688095874 12.177 10.973 9.407 8.337 7.006 M3V 254 1
20 V* AX Mic Er* 21 17 15.2690680973 -38 52 02.503938581   8.06 6.68     M1V 224 0
21 HD 204961 PM* 21 33 33.9751191976 -49 00 32.399427028 11.359 10.176 8.672 7.665 6.479 M2/3V 290 1
22 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
23 * ksi Peg PM* 22 46 41.5798542334 +12 10 22.388860108 4.66 4.69 4.20 3.73 3.42 F6V 386 0
24 * ksi Peg B PM* 22 46 42.3418753790 +12 10 21.120204399   13.5 11.7 11.6   M3.5 36 0
25 BD-15 6290 BY* 22 53 16.7325836486 -14 15 49.304052185 12.928 11.749 10.192 9.013 7.462 M3.5V 1013 1
26 HD 216899 PM* 22 56 34.8046530863 +16 33 12.355636588 11.323 10.143 8.638 7.657 6.542 M1.5V 292 0
27 V* BR Psc BY* 23 49 12.5250852078 +02 24 04.405476893 11.532 10.427 8.993 8.029 6.946 dM1 326 0

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