2025A&A...699A.180C


Query : 2025A&A...699A.180C

2025A&A...699A.180C - Astronomy and Astrophysics, volume 699A180 (2025/7-1)

Power density spectra morphologies of seismically unresolved red-giant asteroseismic binaries.

CHOI J.Y., ESPINOZA-ROJAS F., COPPEE Q. and HEKKER S.

Abstract (from CDS):

Context. Asteroseismic binaries are two oscillating stars detected in a single light curve. These systems provide robust constraints on stellar models from the combination of dynamical and asteroseismical stellar parameters. Predictions suggested that approximately 200 asteroseismic binaries may exist among the long-cadence Kepler data, and the majority of them consist of two red-clump (core helium burning) stars. However, detecting these systems is challenging when the binary components exhibit oscillations at similar frequencies that are indistinguishable (i.e., unresolved asteroseismic binaries).
Aims. In this study, we predict the morphologies of power density spectra (PDSs) of seismically unresolved red-giant asteroseismic binaries to provide examples that can be used to identify the systems among observed stars.
Methods. We created 5000 artificial asteroseismic binary (AAB) systems by combining the KASOC light curves of red giants with oscillations at similar frequency ranges. To quantify the complexity of the oscillation patterns, we used the maximum signal-to-noise ratio of the background-normalized PDS and Shannon entropy. Additionally, we identified the radial and quadrupole mode pairs for the individual binary component and determined their impact on the PDS morphologies of AABs.
Results. Our results reveal that the majority of AABs (∼47%) consist of the two red-clump stars. The PDSs of AABs generally exhibit increased Shannon entropy and decreased oscillation power compared to individual components. We focused on the ∼8% of AABs whose stellar components have a similar brightness and classified them into four distinct morphologies: (i) single star-like PDSs, whereby oscillations from one component dominate, (ii) aligned, whereby the dominant oscillations in the stars that form the AAB appear at similar frequencies, (iii) partially aligned, whereby some oscillation modes of component stars are aligned while others are not, and (iv) PDSs containing complex structures with unclear mode patterns caused by the misalignment of the mode frequencies of both components.
Conclusions. We found that most AABs with detectable oscillations from both components show complex oscillation patterns. Therefore, unresolved asteroseismic binaries with a low oscillation power and complex oscillation patterns as characterized by high Shannon entropy offer a potential explanation to understand the observed stars with complex PDSs.

Abstract Copyright: © The Authors 2025

Journal keyword(s): asteroseismology - stars: oscillations

Simbad objects: 13

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Number of rows : 13
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 2MASS J18485932+4606494 HB* 18 48 59.3222984304 +46 06 49.523749704           G5V: 27 0
2 HD 176465 ** 18 58 03.46393 +47 11 30.6471       8.462   G4V 62 0
3 HD 177412 SB* 19 02 39.4175915928 +43 07 02.940702096   8.38 7.86     F6IV 76 0
4 2MASS J19034433+3734348 RG* 19 03 44.3348079384 +37 34 34.897774728           ~ 33 0
5 2MASS J19110454+4342478 HB* 19 11 04.5403965336 +43 42 47.896592832           G6V 33 0
6 2MASS J19141861+4238492 RG* 19 14 18.6062217816 +42 38 49.279955496   12.228 11.608 11.303   G8IV 34 0
7 KIC 2568888 ** 19 20 22.453488 +37 51 41.40828   15.16 13.83 13.42   ~ 15 0
8 2MASS J19214781+4646111 HB* 19 21 47.8138363344 +46 46 11.012729844           ~ 27 0
9 UCAC4 637-069192 RG* 19 28 23.8954887744 +37 23 23.929037664   15.173 13.757 13.456   ~ 21 0
10 2MASS J19332527+4905240 HB* 19 33 25.2745261440 +49 05 23.962279092           K2IIIb 27 0
11 TYC 3557-2118-1 EB* 19 41 20.9933729592 +45 30 17.199878004   10.67 9.82     G5 31 0
12 HD 188753 ** 19 54 58.3717655 +41 52 17.529759   8.24 7.44 6.9   G9V 138 1
13 HD 190585 EB* 20 03 48.3209367264 +45 36 14.805207576   10.74 9.65     K2 51 0

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