Abstract
Subdwarf B (sdB) stars are hot, compact, and evolved objects that form the very hot end of the horizontal branch, the so-called Extreme Horizontal Branch (EHB). Understanding the formation of sdB stars is one of the remaining challenges of stellar evolution theory. Several scenarios have been proposed to account for the existence of such objects, made of He-burning core surrounded by very thin H-rich envelope. They give quite different theoretical mass distributions for the resulting sdB stars. Detailed asteroseismic analyses, including mass estimates, of 15 pulsating hot B subdwarfs have been published since a decade. The masses have also been reliably determined by light curve modeling and spectroscopy for 7 sdB components of eclipsing and/or reflection effect binaries. These empirical mass distributions, although based on small-number statistics, can be compared with the expectations of stellar evolution theory. In particular, the two He white dwarfs merger scenario does not seem to be the dominant channel to form isolated sdB stars, while the post-red giant branch scenario is reinforced. This opens new questions on extreme mass loss of red giants to form EHB stars, possibly in connection with the recently discovered close substellar companions and planets orbiting sdB stars.
Highlights
Subdwarf B stars are hot (Teff = 20000 − 40000 K), compact, and evolved objects that form the very hot end of the horizontal branch, the so-called Extreme Horizontal Branch (EHB)
We estimate that the total number of stars involved in each subsample has to reach ∼ 30 to carry out statistically robust comparisons with expectations from theoretical scenarios for the formation of Subdwarf B (sdB) stars
The red boundaries correspond to the calculations for single star evolution, in which a sdB star is formed from a red giant star experiencing a strong mass loss on the red giant branch (RGB) [2]
Summary
The residual very thin H-rich envelope has not retained enough mass to sustain shell-burning, and sdB stars evolve directly toward the white dwarf (WD) cooling sequence after He-core exhaustion, without experiencing the Asymptotic Giant Branch (AGB) and Planetary Nebula (PN) phases of usual stellar evolution.
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