Granulation in K-type Dwarf Stars. I. Spectroscopic observations

TL;DR

This study uses high-resolution spectroscopy of K-dwarf stars to analyze line asymmetries and shifts caused by granulation, revealing star-to-star differences and enabling precise radial velocity measurements.

Contribution

First detailed spectroscopic analysis of granulation effects in K-dwarfs, linking line asymmetries to stellar parameters and improving radial velocity accuracy.

Findings

Fe I line bisectors show C-shapes indicating granulation.

Wavelength shifts increase with decreasing line strength.

Detected a plateau in line shifts for inactive stars, aiding radial velocity calibration.

Abstract

Very high resolution (R~160,000-210,000), high signal-to-noise ratio (S/N>300) spectra of nine bright K-dwarfs were obtained with the 2dcoude spectrograph on the 2.7m Telescope at McDonald Observatory to determine wavelength shifts and asymmetries of Fe I lines. The observed shapes and positions of Fe I lines reveal asymmetries and wavelength shifts that indicate the presence of granulation. In particular, line bisectors show characteristic C-shapes while line core wavelengths are blueshifted by an amount that increases with decreasing equivalent width (EW). On average, Fe I line bisectors have a span that ranges from nearly 0 for the weakest lines (residual core flux > 0.7) to about 75 m/s for the strongest lines (residual core flux ~ 0.3) while wavelength shifts range from about -150 m/s in the weakest (EW ~ 10 mA) lines to 0 in the strongest (EW > 100 mA) features. A more detailed inspection of the bisectors and wavelength shifts reveals star-to-star differences that are likely associated with differences in stellar parameters, projected rotational velocity, and stellar activity. For the inactive, slow projected rotational velocity stars, we detect, unequivocally, a plateau in the line-shifts at large EW values (EW > 100 mA), a behavior that had been identified before only in the solar spectrum. The detection of this plateau allows us to determine the zero point of the convective blueshifts, which is useful to determine absolute radial velocities. Thus, we are able to measure such velocities with a mean uncertainty of about 60 m/s.