Abstract

<i>Context. <i/>The measurement of line broadening in cool stars is in general a difficult task. In order to detect slow rotation or weak magnetic fields, an accuracy of 1 km s<sup>-1<sup/> is needed. In this regime the broadening from convective motion becomes important. We present an investigation of the velocity fields in early to late M-type star hydrodynamic models, and we simulate their influence on molecular line shapes. The M star model parameters range between of and effective temperatures from 2500 K to 4000 K.<i>Aims. <i/>Our aim is to characterize the - and -dependence of the velocity fields and express them in terms of micro- and macro-turbulent velocities in the one dimensional sense. We present a direct comparison between 3D hydrodynamical velocity fields and 1D turbulent velocities. The velocity fields strongly affect the line shapes of , and it is our goal to give a rough estimate of the and parameter range in which 3D spectral synthesis is necessary and where 1D synthesis suffices. We want to distinguish between the velocity-broadening from convective motion and the rotational- or Zeeman-broadening in M-type stars we are planning to measure. For the latter, lines are an important indicator.<i>Methods. <i/>In order to calculate M-star structure models, we employ the 3D radiative-hydrodynamics (RHD) code CO<sup>5<sup/>BOLD. The spectral synthesis in these models is performed with the line synthesis code LINFOR3D. We describe the 3D velocity fields in terms of a Gaussian standard deviations and project them onto the line of sight to include geometrical and limb-darkening effects. The micro- and macro-turbulent velocities are determined with the “curve of growth” method and convolution with a Gaussian velocity profile, respectively. To characterize the and dependence of lines, the equivalent width, line width, and line depth are examined.<i>Results. <i/>The velocity fields in M-stars strongly depend on and . They become stronger with decreasing and increasing . The projected velocities from the 3D models agree within ~100 m s<sup>-1<sup/> with the 1D micro- and macro-turbulent velocities. The line quantities systematically depend on and .<i>Conclusions. <i/>The influence of hydrodynamic velocity fields on line shapes of M-type stars can well be reproduced with 1D broadening methods. lines turn out to provide a means to measure and in M-type stars. Since different lines all behave in a similar manner, they provide an ideal measure for rotational and magnetic broadening.

Highlights

  • Most of our knowledge about stars comes from spectroscopic investigation of atomic or molecular lines

  • We investigate the influence of velocity fields, log g, and Teff on the FeH molecular lines

  • In order to analyze the influence of velocity fields in M-stars on FeH lines, we construct a set of CO5BOLD-models with Teff = 2500 K–4000 K and log g = 3.0−5.0 [cgs]

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Summary

Introduction

Most of our knowledge about stars comes from spectroscopic investigation of atomic or molecular lines. M type stars exhibit a number of molecular absorption bands in the infrared, for example FeH In these bands, the individual lines are relatively well separated and provide a good tracer of stellar velocity fields. We model the surface velocity fields of M type stars and their influence on the narrow spectral lines of FeH. We investigate the influence of velocity fields, log g, and Teff on the FeH molecular lines. In order to analyze the influence of velocity fields in M-stars on FeH lines, we construct a set of CO5BOLD-models with Teff = 2500 K–4000 K and log g = 3.0−5.0 [cgs]. We will call the spectral lines synthesized from 3D -models “ 3D -lines”

Atmosphere structures
Velocity fields in the CO5BOLD-models
Reduction of the 3D velocity fields
Weighted velocities
Radial velocity shifts
Micro- and macro-turbulent velocities
Determination of micro- and macro-turbulent velocities
T eff- and log g-dependence of FeH molecular lines
FeH line data
An ensemble of 3D- and 3D -FeH lines
Equivalent width Wλ
Line depth
Findings
Summary and conclusion
Full Text
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