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Observation and modelling of main‐sequence star chromospheres – XV. New constraints on the dynamo mechanisms for dM1 stars ★
Author(s) -
Houdebine E. R.
Publication year - 2011
Publication title -
monthly notices of the royal astronomical society
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 2.058
H-Index - 383
eISSN - 1365-2966
pISSN - 0035-8711
DOI - 10.1111/j.1365-2966.2010.17846.x
Subject(s) - physics , astrophysics , metallicity , stars , radius , dynamo , luminosity , absolute magnitude , stellar rotation , spectral line , line (geometry) , astronomy , stellar atmosphere , balmer series , emission spectrum , magnetic field , galaxy , geometry , computer security , mathematics , computer science , quantum mechanics
With the help of measures of rotation, radius and metallicity for a selected sample of dM1 stars (with T eff = 3460 ± 60 K ), we aim to set new constraints on the dynamo mechanisms. We recover 913 high‐resolution spectra for 97 different M1 dwarfs from the European Southern Observatory and Observatoire de Haute Provence data bases. We present 660 new measurements of the Ca  ii resonance lines and 913 new measurements of the Hα line for dM1 stars. We also compile other measurements available in the literature. In total, we obtain 2216 measures of the Ca  ii lines for 113 different dM1 stars. This represents the largest compilation of chromospheric line measurements at a single spectral type. We cross‐correlate these magnetic activity indicators with various stellar parameters to set new constraints on the dynamo mechanisms and on the properties of the outer atmosphere. We find a correlation of the Ca  ii line mean equivalent width with the absolute magnitude and the metallicity. We correct the Ca  ii line measures from the metallicity effect and find that the surface flux in the Ca  ii lines grows roughly as the power of 3.6 of the stellar radius. This corrected flux is a direct measure of magnetic activity at the chromospheric level. We find that the total magnetic activity level grows roughly as the power of 5.6 of the stellar radius. This trend is confirmed by the correlation between the Hα line and absolute magnitude and the Hα line luminosity and stellar radius: the Hα luminosity grows roughly as the volume of the star for low activity dM1 stars and as the power of roughly 5/2 of the stellar radius for dM1e stars. The advantage of the Hα line is that its formation in not dependent on metallicity. In contrast to the Ca  ii line, we find no correlation between L X and the absolute magnitude. We find that L X roughly correlates with the Ca  ii luminosity although the correlation is not very good. This correlation shows that L X grows as the power of 3/2 of the Ca  ii luminosity, i.e. the coronal emission grows faster than the chromospheric emission. We find a correlation between the corrected Ca  ii line equivalent width and P /sin  i , i.e. the Ca  ii surface flux grows as the power of −1.5 of the rotation period. We also find a correlation between F X , the X‐ray surface flux, and P /sin  i : F X ∝ ( P /sin  i ) −3.7 . In other words, the coronal emission is much more dependent on the rotation period than the chromospheric emission. We find that the level of magnetic activity in dM1 stars is more dependent on the stellar radius than on rotation at the chromospheric level. We discuss the implications of these results on the models of stellar dynamos.

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