Steven W. Stahler’s research while affiliated with University of California, Berkeley and other places

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Publications (135)


Outward migration in Nascent stellar groups
  • Article

March 2024

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1 Read

Monthly Notices of the Royal Astronomical Society

Steven W Stahler

As a stellar group forms within its parent molecular cloud, new members first appear in the deep interior. These overcrowded stars continually diffuse outward to the cloud boundary, and even beyond. Observations have so far documented only the interior drift. Those stars that actually leave the cloud form an expanding envelope that I call the ‘stellar mantle.’ Simple fluid models for the cloud and mantle illustrate their basic structure. The mantle’s expansion speed is subsonic with respect to the cloud’s dynamical temperature. I describe, in qualitative terms, how the expanding mantle and Galactic tidal radius might together shape the evolution of specific types of stellar groups. The massive stars in OB associations form in clouds that contract before extruding a substantial mantle. In contrast, the more slowly evolving clouds forming open clusters and T associations have extended mantles that encounter a shrinking tidal radius. These clouds are dispersed by internal stellar outflows. If the remaining group of stars is gravitationally bound, it appears as a long-lived open cluster, truncated by the tidal radius. If the group is unbound, it is a late-stage T association that will soon be torn apart by the tidal force. The ‘distributed’ populations of pre-main sequence stars observed in the outskirts of several star-forming regions are too distant to be stellar mantles. Rather, they could be the remnants of especially low-mass T associations.


The Nature of Class I Sources: Periodic Variables in Orion

October 2019

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7 Reads

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5 Citations

The Astrophysical Journal

We present a quantitative, empirically based argument that at least some Class I sources are low-mass, pre-main-sequence stars surrounded by spatially extended envelopes of dusty gas. The source luminosity arises principally from stellar gravitational contraction, as in optically visible pre-main-sequence stars that lack such envelopes. We base our argument on the fact that some Class I sources in Orion and other star-forming regions have been observed by Spitzer to be periodic variables in the mid-infrared, and with periods consistent with T Tauri rotation rates. Using a radiative transfer code, we construct a variety of dust envelopes surrounding rotating, spotted stars, to see whether an envelope that produces a Class I spectral energy distribution at least broadly matches the observed modulations in luminosity. Acceptable envelopes can be either spherical or flattened and may or may not have polar cavities. The key requirement is that they have a modest equatorial optical depth at the Spitzer waveband of 3.6 μ m, typically τ 3.6 ≈ 0.6. The total envelope mass, based on this limited study, is at most about 0.1 M ⊙ , less than a typical stellar mass. Future studies should focus on the dynamics of the envelope, to determine whether material is actually falling onto the circumstellar disk.


The Nature of Class I Sources: Periodic Variables in Orion

September 2019

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2 Reads

We present a quantitative, empirically based argument that at least some Class I sources are low-mass, pre-main-sequence stars surrounded by spatially extended envelopes of dusty gas. The source luminosity arises principally from stellar gravitational contraction, as in optically visible pre-main-sequence stars that lack such envelopes. We base our argument on the fact that some Class I sources in Orion and other star-forming regions have been observed by Spitzer to be periodic variables in the mid-infrared, and with periods consistent with T Tauri rotation rates. Using a radiative transfer code, we construct a variety of dust envelopes surrounding rotating, spotted stars, to see if an envelope that produces a Class I SED at least broadly matches the observed modulations in luminosity. Acceptable envelopes can either be spherical or flattened, and may or may not have polar cavities. The key requirement is that they have a modest equatorial optical depth at the Spitzer waveband of 3.6 {\mu}m, typically {\tau}3.6 {\approx} 0.6. The total envelope mass, based on this limited study, is at most about 0.1 M{\odot}, less than a typical stellar mass. Future studies should focus on the dynamics of the envelope, to determine whether material is actually falling onto the circumstellar disk.


Embedded Binaries and Their Dense Cores

April 2017

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54 Reads

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47 Citations

Monthly Notices of the Royal Astronomical Society

We explore the relationship between young, embedded binaries and their parent cores, using observations within the Perseus Molecular Cloud. We combine recently published VLA observations of young stars with core properties obtained from SCUBA-2 observations at 850 um. Most embedded binary systems are found toward the centres of their parent cores, although several systems have components closer to the core edge. Wide binaries, defined as those systems with physical separations greater than 500 au, show a tendency to be aligned with the long axes of their parent cores, whereas tight binaries show no preferred orientation. We test a number of simple, evolutionary models to account for the observed populations of Class 0 and I sources, both single and binary. In the model that best explains the observations, all stars form initially as wide binaries. These binaries either break up into separate stars or else shrink into tighter orbits. Under the assumption that both stars remain embedded following binary breakup, we find a total star formation rate of 168 Myr^-1. Alternatively, one star may be ejected from the dense core due to binary breakup. This latter assumption results in a star formation rate of 247 Myr^-1. Both production rates are in satisfactory agreement with current estimates from other studies of Perseus. Future observations should be able to distinguish between these two possibilities. If our model continues to provide a good fit to other star-forming regions, then the mass fraction of dense cores that becomes stars is double what is currently believed.


Embedded Binaries and Their Dense Cores

April 2017

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1 Read

We explore the relationship between young, embedded binaries and their parent cores, using observations within the Perseus Molecular Cloud. We combine recently published VLA observations of young stars with core properties obtained from SCUBA-2 observations at 850 um. Most embedded binary systems are found toward the centres of their parent cores, although several systems have components closer to the core edge. Wide binaries, defined as those systems with physical separations greater than 500 au, show a tendency to be aligned with the long axes of their parent cores, whereas tight binaries show no preferred orientation. We test a number of simple, evolutionary models to account for the observed populations of Class 0 and I sources, both single and binary. In the model that best explains the observations, all stars form initially as wide binaries. These binaries either break up into separate stars or else shrink into tighter orbits. Under the assumption that both stars remain embedded following binary breakup, we find a total star formation rate of 168 Myr^-1. Alternatively, one star may be ejected from the dense core due to binary breakup. This latter assumption results in a star formation rate of 247 Myr^-1. Both production rates are in satisfactory agreement with current estimates from other studies of Perseus. Future observations should be able to distinguish between these two possibilities. If our model continues to provide a good fit to other star-forming regions, then the mass fraction of dense cores that becomes stars is double what is currently believed.


EXors and the stellar birthline

February 2017

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41 Reads

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5 Citations

Astronomy and Astrophysics

We assess the evolutionary status of EXors. These low-mass, pre-main-sequence stars repeatedly undergo sharp luminosity increases, each a year or so in duration. We place into the HR diagram all EXors that have documented quiescent luminosities and effective temperatures, and thus determine their masses and ages. Two alternate sets of pre-main-sequence tracks are used, and yield similar results. Roughly half of EXors are embedded objects, i.e., they appear observationally as Class I or flat-spectrum infrared sources. We find that these are relatively young and are located close to the stellar birthline in the HR diagram. Optically visible EXors, on the other hand, are situated well below the birthline. They have ages of several Myr, typical of classical T Tauri stars. Judging from the limited data at hand, we find no evidence that binarity companions trigger EXor eruptions; this issue merits further investigation. We draw several general conclusions. First, repetitive luminosity outbursts do not occur in all pre-main-sequence stars, and are not in themselves a sign of extreme youth. They persist, along with other signs of activity, in a relatively small subset of these objects. Second, the very existence of embedded EXors demonstrates that at least some Class I infrared sources are not true protostars, but very young pre-main-sequence objects still enshrouded in dusty gas. Finally, we believe that the embedded pre-main-sequence phase is of observational and theoretical significance, and should be included in a more complete account of early stellar evolution.






Citations (33)


... the 2MASS, WISE, Spitzer, AKARI, and Herschel (see T.Onaka et al. 2021, and references therein). The black-solid line represents the AKARI spectrum. The red downward arrows indicate the upper limit obtained with the present ALMA observations. Typical SEDs of Class I and II YSOs in Taurus are plotted by orange and blue squares (Á.Ribas et al. 2017;E. A. Ellithorpe et al. 2019). The brown diamonds represent the photometric data of an OH/IR star, OH 26.5+0.6, obtained by 2MASS, MSX, WISE, and Herschel, whose fluxes are scaled to fit the distance to Object 1 or Object 2 (M. P.Egan et al. 2003;M. F. Skrutskie et al. 2006;E. L. Wright et al. 2010;S. Molinari et al. 2016). The green lines represent the synthesized ...

Reference:

ALMA Observations of Peculiar Embedded Icy Objects
The Nature of Class I Sources: Periodic Variables in Orion
  • Citing Article
  • October 2019

The Astrophysical Journal

... In disk fragmentation models, massive disks can become gravitationally unstable and produce one or more companions and, combined with capture, 2+2 systems can be formed (Kratter & Lodato 2016). Filament fragmentation has also been discussed as leading to bound binaries and multiples (e.g., Bonnell & Bastien 1993;Pineda et al. 2015;Sadavoy & Stahler 2017). ...

Embedded Binaries and Their Dense Cores
  • Citing Article
  • April 2017

Monthly Notices of the Royal Astronomical Society

... The resulting radial profile is the Bonnor-Ebert (BE) solution, which can be found by solving the Lane-Emden equation numerically for an isothermal equation of state with the characteristic radiusl c following Stahler & Palla (2008). Obviously this BE sphere has the same characteristic scalel c as the plane layer, which is the same critical length of l c from the time scale criterion, for ρ c = ρ Hill . ...

Cloud Equilibrium and Stability
  • Citing Chapter
  • January 2008

... This object could be periodic and the Lomb-Scargle analysis calculates a period of ∼ 970 days. In the third panel the object shows a single-epoch significant outburst (∆K s ≈ 1.5 mag), typical of EX Lupi (EXor)-type sources (Herbig 2007;Moody & Stahler 2017). This light curve is unique in our sample. ...

EXors and the stellar birthline
  • Citing Article
  • February 2017

Astronomy and Astrophysics

... Another source of difficulty would be inaccuracies of the progenitor's evolution and presupernova structure (e.g., Branch & Wheeler 2017). Such inaccuracies may stem from uncertainties in the complicated evolution processes, which include mass loss (e.g., Renzo et al. 2017), convection (e.g., Woosley et al. 2002), rotation (e.g., Heger et al. 2008;Chatzopoulos et al. 2016), magnetic fields (e.g., Maeder & Stahler 2009), and nuclear reactions (e.g., Weaver & Woosley 1993;Sallaska et al. 2013;Fields et al. 2018). ...

Physics, Formation and Evolution of Rotating Stars
  • Citing Article
  • September 2009

Physics Today

... M. Converse & S. W. Stahler 2011). This heating process prevents core collapse while accelerating the cluster's expansion and dissolution (R. M. O'Leary et al. 2014). However, on the contrary, the dynamical relaxation slows the expansion and can still produce mass segregation (C. ...

Two paths of cluster evolution: Global expansion versus core collapse
  • Citing Article
  • June 2014

Monthly Notices of the Royal Astronomical Society

... As was explained in Section 6, accretion of material onto the stellar surface at 8 Myr will not induce visible variation in the [Fe/H] abundance due to the size of the stellar convective layer at this early stage (Kunitomo et al. 2018). However, as the star evolves, the convective zone will gradually shrink (Stahler & Palla 2004); thus, the signature on the star's composition caused by planet engulfment would be increasingly great at later ages. ...

The Formation of Stars
  • Citing Article
  • January 2005

... Once a star has reached a mass of about 10 M , its spectrum becomes UV-dominated and it begins to ionize its environment. This means that accretion as well as ionizing and non-ionizing radiation needs to be considered in concert (Keto, 2002;Keto, 2003Keto, , 2007Peters et al., 2010a;Peters et al., 2010b). It was realized decades ago that in simple one-dimensional collapse models, the outward radiation force on the accreting material should be significantly stronger than the inward pull of gravity (Larson & Starrfield, 1971;Kahn, 1974), in particular if one accounts for dust opacity. ...

The Dynamics of Ultracompact HII Regions
  • Citing Article
  • Full-text available
  • November 2013

Monthly Notices of the Royal Astronomical Society

... He also suggested that the LP solution was unrealistic, arguing that only finely-tuned initial and boundary conditions could lead to it. However, numerical simulations of self-consistently evolving cores from non-singular initial conditions systematically show that the flow approaches the LP solution (e.g., Larson 1969;Penston 1969;Hunter 1977;Foster & Chevalier 1993;Mohammadpour & Stahler 2013;Naranjo-Romero et al. 2015, although see Keto et al. 2015 for a counterexample). In addition, Shu's inside-out solution has a number of problems of its own. ...

Externally Fed Star Formation: A Numerical Study
  • Citing Article
  • June 2013

Monthly Notices of the Royal Astronomical Society

... This is consistent with the interpretation of Agra-Amboage et al. (2011), and yields a knot launch date of 2001.7 +0.2 −0.6 , consistent with a 2.5 yr ejection period. Second, we assign knot C a proper motion of 0. 17 yr −1 , which is consistent with the proper motion of knot B. This is significantly slower than the knot velocity implied by the radial velocity of knot C; however, Launch date (UT) we note that the knots in Herbig-Haro objects often show discrepancies between their proper motion and radial velocity (Eislöffel & Mundt 1992, 1994. This knot trajectory passes through the cluster of knot observations reported by Takami et al. (2002) and (Fig. 11). ...

Entralnment by Stellar Jets
  • Citing Article
  • January 1994