This document discusses using eclipsing binary red giants to test asteroseismic scaling relations. The author identified 19 red giants in eclipsing binary systems from Kepler data. Most systems oscillate, but 4 do not. For one well-characterized equal-mass binary system, modeling of light curves and radial velocities directly measured the stars' properties. Comparison to asteroseismic analysis showed the scaling relations overestimate mass and radius. The author suggests tides and magnetism in close, circularized binary systems dampen oscillations. Red giant binaries provide benchmarks to test and improve asteroseismic analysis techniques.
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Cool Stars 19 Talk
1. Red Giants in Eclipsing Binaries
Exploring Non-Oscillators and
Testing Asteroseismic Scalings
Meredith L. Rawls
New Mexico State University
University of Washington/LSST (Fall 2016)
June 10, 2016 Cool Stars 19
@merrdiff
Image: G Perez, IAC, SMM
In collaboration with P. Gaulme, J. McKeever, J. Jackiewicz, et al.
2. Meredith L. Rawls @merrdiff
Eclipsing binaries with light curves and radial
velocities let us directly measure M, R
Asteroseismology is a powerful tool to characterize
lots of stars quickly, using light curves alone
We can study oscillating stars in eclipsing binaries
from two independent perspectives
A set of well-characterized binaries lets us explore
why some dont oscillate when we think they should
How to measure stellar properties?
3. Meredith L. Rawls @merrdiff
Kepler red giant catalog: ~14,000
Kepler eclipsing binary catalog: 2,500+
After cross-correlating: 19
Most systems are SB2, but 4 are SB1
Most are oscillators, but 4 are not
Searching for red giants in
eclipsing binary systems
Gaulme et al. 2013 & 2014
4. Meredith L. Rawls @merrdiff
僚
僚max
Power
Frequency 僚
Acoustic pressure modes
Buoyant gravity modes
Evolutionary state
Scaling relations
Characterizing a star: asteroseismology
6. Meredith L. Rawls @merrdiff
Pipeline comparisons: Teff, [Fe/H], log g
Gaulme et al. submitted
7. Meredith L. Rawls @merrdiff
Tides and magnetism affect oscillations
P = 20 d
e ~ 0
non-oscillator
P = 207 d
e = 0.23
oscillator
Rawls et al. in prep
8. Meredith L. Rawls @merrdiff
Tides and magnetism affect oscillations
Observede
expect e ~ 0 expect e > 0
short P long P
Rawls et al. in prep
Predicted change in
eccentricity from stellar
evolution modeling
Non-oscillators have
short P, circularized
orbits, and spots
9. Meredith L. Rawls @merrdiff
Asteroseismic scalings
overestimate M and R
0.8 1 1.2 1.4 1.6 1.8 2 2.2
0.8
1
1.2
1.4
1.6
1.8
2
2.2
Dynamical mass [M]
Asteroseismicmass[M]
Seismicmass(M)
Dynamic mass (M)
16%
*
8 9 10 11 12 13 14
8
9
10
11
12
13
14
Dynamical radius [R]
Asteroseismicradius[R]
Dynamic radius (R)
Seismicradius(R)
6%
*
Gaulme et al. submitted
10. Meredith L. Rawls @merrdiff
Solar-like oscillations are damped by
magnetism & tides, which occur together
Scaling relations overestimate giant M, R
These stars are references for survey pipelines
Asteroseismic surveys underestimate ages
and exclude active stars and close binaries
Red giant binaries are powerful
benchmarks for asteroseismology