Description Usage Arguments Details Value Author(s) References Examples
Create a 1-d convolution kernel to broaden a spectrum from a rotating star
1 | lsf_rotate(deltav, vsini, epsilon=0.6)
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deltav |
step increment in the output rotation kernel, scalar, in km/s |
vsini |
rotational velocity projected along the line of sight, scalar, in km/s |
epsilon |
limb-darkening coefficient, scalar (default = 0.6) |
This function can be used to derive the broadening effect, or line spread function (LSF), due to stellar rotation on a synthetic stellar spectrum. It assumes constant limb darkening across the disk. To actually compute the broadening. the spectrum should be convolved with the rotational LSF using a function like kernapply or filter.
The number of points in the output lsf will be always be odd (the kernel is symmetric) and equal to either ceil(2*Vsini/deltav) or ceil(2*Vsini/deltav) +1 (whichever number is odd).
The limb darkening coefficient epsilon = 0.6 is typical for photospheric lines. The specific intensity I at any angle theta from the specific intensity Icen at the center of the disk is given by
1 |
.
The algorithm is adapted from rotin3.f in the SYNSPEC software of Hubeny & Lanz http://nova.astro.umd.edu/. Also see Eq. 17.12 in Gray (1992).
lsf |
convolution kernel vector for the specified rotational velocity |
Written by W. Landsman 2001
R adaptation by Arnab Chakraborty June 2013
Gray, D., 1992, "The Observation and Analysis of Stellar Photospheres"
1 2 3 4 | # Plot the LSF for a star rotating at 90 km/s in both velocity space and
# for a central wavelength of 4300 A. Compute the LSF every 3 km/s
lsf = lsf_rotate(3,90) # LSF will contain 61 pts
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