期刊
ASTROPHYSICAL JOURNAL LETTERS
卷 924, 期 1, 页码 -出版社
IOP Publishing Ltd
DOI: 10.3847/2041-8213/ac441f
关键词
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资金
- NASA ATP grant [ATP80NSSC18K0560]
- National Science Foundation at the KITP [PHY 17-48958]
- Center for Scientific Computing from the CNSI, MRL: an NSF MRSEC [DMR-1720256]
- NSF [CNS-1725797]
- Simons Foundation
Increasing stellar mass leads to higher stellar luminosity, causing radiation pressure to dominate in the stellar envelope. Additional instabilities can occur in OB stars, manifesting as low-frequency variability in lightcurves. 3D simulations validate these observations and show similar characteristics to real stars.
Increasing main-sequence stellar luminosity with stellar mass leads to the eventual dominance of radiation pressure in stellar-envelope hydrostatic balance. As the luminosity approaches the Eddington limit, additional instabilities (beyond conventional convection) can occur. These instabilities readily manifest in the outer envelopes of OB stars, where the opacity increase associated with iron yields density and gas-pressure inversions in 1D models. Additionally, recent photometric surveys (e.g., TESS) have detected excess broadband low-frequency variability in power spectra of OB star lightcurves, called stochastic low-frequency variability (SLFV). This motivates our novel 3D Athena++ radiation hydrodynamical (RHD) simulations of two 35 M (circle dot) star envelopes (the outer approximate to 15% of the stellar radial extent), one on the zero-age main sequence and the other in the middle of the main sequence. Both models exhibit turbulent motion far above and below the conventional iron-opacity peak convection zone (FeCZ), obliterating any quiet part of the near-surface region and leading to velocities at the photosphere of 10-100 km s(-1), directly agreeing with spectroscopic data. Surface turbulence also produces SLFV in model lightcurves with amplitudes and power-law slopes that are strikingly similar to those of observed stars. The characteristic frequencies associated with SLFV in our models are comparable to the thermal time in the FeCZ (approximate to 3-7 day(-1)). These ab initio simulations are directly validated by observations and, though more models are needed, we remain optimistic that 3D RHD models of main-sequence O-star envelopes exhibit SLFV originating from the FeCZ.
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