2021MNRAS.502.5856S


Query : 2021MNRAS.502.5856S

2021MNRAS.502.5856S - Mon. Not. R. Astron. Soc., 502, 5856-5874 (2021/April-3)

Rotation of the convective core in γ Dor stars measured by dips in period spacings of g modes coupled with inertial modes.

SAIO H., TAKATA M., LEE U., LI G. and VAN REETH T.

Abstract (from CDS):

The relation of period spacing (ΔP) versus period (P) of dipole prograde g modes is known to be useful to measure rotation rates in the g-mode cavity of rapidly rotating γ Dor and slowly pulsating B (SPB) stars. In a rapidly rotating star, an inertial mode in the convective core can resonantly couple with g-mode propagative in the surrounding radiative region. The resonant coupling causes a dip in the P - ΔP relation, distinct from the modulations due to the chemical composition gradient. Such a resonance dip in ΔP of prograde dipole g modes appears around a frequency corresponding to a spin parameter 2frot(cc)/νco–rot ∼8-11 with frot(cc) being the rotation frequency of the convective core and νco–rot the pulsation frequency in the co-rotating frame. The spin parameter at the resonance depends somewhat on the extent of core overshooting, central hydrogen abundance, and other stellar parameters. We can fit the period at the observed dip with the prediction from prograde dipole g modes of a main-sequence model, allowing the convective core to rotate differentially from the surrounding g-mode cavity. We have performed such fittings for 16 selected γ Dor stars having well-defined dips, and found that the majority of γ Dor stars we studied rotate nearly uniformly, while convective cores tend to rotate slightly faster than the g-mode cavity in less evolved stars.

Abstract Copyright: © 2021 The Author(s) Published by Oxford University Press on behalf of Royal Astronomical Society

Journal keyword(s): asteroseismology - stars: interiors - stars: oscillations - stars: rotation - stars: variables:general

Simbad objects: 20

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Number of rows : 20
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 TYC 3549-900-1 gD* 18 57 28.9160567616 +49 47 11.305591476   10.45 10.11     F1V 9 0
2 TYC 3545-127-1 gD* 19 00 25.5619212312 +48 32 27.313425672   10.43 10.07     ~ 8 0
3 TYC 3549-2766-1 gD* 19 05 53.5806685440 +49 35 54.142171224   11.70 11.23     ~ 12 0
4 TYC 3550-369-1 gD* 19 11 29.4137959896 +50 14 29.689592532   11.82 11.72     F1V 24 0
5 TYC 3125-1185-1 gD* 19 12 18.5346248400 +40 52 39.730925676   10.24 9.88     F2Vswkmet(A7) 22 0
6 2MASS J19171780+5102520 gD* 19 17 17.8131742272 +51 02 51.943068492           F1V 11 0
7 UCAC4 636-069559 gD* 19 24 49.7613579720 +37 03 32.048241876   13.034 12.504 12.610   F2V 5 0
8 2MASS J19250578+3827444 dS* 19 25 05.7825104256 +38 27 44.312683140           F0IV 17 0
9 KIC 1164966 gD* 19 27 19.7173937592 +36 50 13.365112524           ~ 1 0
10 TYC 3564-16-1 Pu* 19 37 03.2104066656 +50 30 20.417184432   10.64 10.23     ~ 25 0
11 TYC 3147-226-1 gD* 19 39 20.2142658192 +43 47 49.776188676   12.29 11.83     ~ 6 0
12 TYC 3557-1023-1 gD* 19 45 24.0389158536 +46 52 19.571243124   10.40 10.11     ~ 12 0
13 HD 225808 gD* 19 47 12.5075196816 +40 28 02.432697240   11.04 10.71     F2V 17 0
14 UCAC4 648-077895 gD* 19 49 06.4872328464 +39 27 09.008371152       13.841   F0V 8 0
15 2MASS J19493877+4957418 gD* 19 49 38.7799420152 +49 57 41.798822760           ~ 9 0
16 2MASS J19524679+3952109 gD* 19 52 46.7940352488 +39 52 10.917704820           ~ 11 0
17 UCAC4 657-079153 gD* 19 52 51.3327794208 +41 12 03.719855196       15.865   ~ 7 0
18 UCAC4 653-082798 gD* 19 54 59.2997880960 +40 35 52.162978560   13.97 13.46 13.22 12.70 ~ 7 0
19 UCAC4 672-079691 gD* 19 59 10.6113733752 +44 14 04.987988160   13.432 13.021 12.868   A9V 7 0
20 2MASS J20033305+4412065 gD* 20 03 33.0554613116 +44 12 06.440880713   14.3060 13.8637     F1V 20 0

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