Star Cluster Formation and the Origin of Stellar Properties. Matthew Bate University of Exeter

Size: px
Start display at page:

Download "Star Cluster Formation and the Origin of Stellar Properties. Matthew Bate University of Exeter"

Transcription

1 Star Cluster Formation and the Origin of Stellar Properties Matthew Bate University of Exeter

2 Typical molecular cloud (Bate et al. 2003) Denser cloud (Bate & Bonnell 2005) Jeans mass 1 M, Opacity limit 3 MJ, P(k)k -4 Jeans mass 1/3 M

3 Stellar Masses - Dependence on Initial Conditions Typical Initial Conditions 9 Times Denser Cloud Opacity-limited Minimum Mass 3 Times Greater Large-scale Turbulence P(k)k -6 Characteristic stellar mass depends on the cloud s mean Jeans mass (Bate & Bonnell 2005) Denser/cooler clouds produce more brown dwarfs and low-mass stars

4 What is the Origin of the IMF? Jeans Mass Ejection Competitive Accretion

5 Bate 2009a: 500 M cloud with decaying turbulence, 35 million SPH particles Follows binaries to 1 AU, discs to ~10 AU Forms 1253 stars and brown dwarfs - best statistics to date from a single calculation

6 Multiplicity as a Function of Primary Mass Multiplicity fraction = (B+T+Q) / (S+B+T+Q) Observations: Close et al. 2003; Basri & Reiners 2006; Fisher & Marcy 1992; Duquennoy & Mayor 1991; Preibisch et al. 1999; Mason et al. 1998

7 Star/VLM Object Separation Distributions Stars: binary, triple, quad separations Median separation: 26 AU VLM objects: binaries, triples, quads Median separation: 10 AU

8 Stellar Mass Distribution Competitive accretion/ejection gives Salpeter-type slope at high-mass end Low-mass turn over ~4 times as many brown dwarfs as a typical star-forming region Not due to sink particle approximation - results almost identical for different sink parameters

9 Additional Physics Star cluster simulations with radiative transfer (Bate 2009b) Radiative feedback dramatically decreases the amount of fragmentation Magnetic fields Star formation simulations (Price & Bate 2007) Magnetic fields inhibit gravitationally unstable discs and binary formation Substantially reduces the ratio of brown dwarfs to stars, in agreement with observations Removes the dependence of the characteristic stellar mass on the cloud s initial Jeans mass Star cluster simulations (Price & Bate 2008) Magnetic fields reduce the amount of fragmentation and the star formation rate Radiation magnetohydrodynamical simulations Star cluster simulations (Price & Bate 2009) Strong magnetic fields (plasma beta <1) and radiative feedback can give low star formation rates similar to those inferred from observations

10 Star Cluster Formation with Radiative Feedback Repeat Bate, Bonnell & Bromm 2003, Bate & Bonnell M molecular clouds, Decaying `turbulence P(k)k -4 Diameters 0.4 pc and 0.2 pc, Mean thermal Jeans masses 1 M and 1/3 M 3,500,000 SPH particles Sink particles Original calculations: Sink Radii 5 AU, gravity softened within 4 AU Radiative transfer calculations: Sink Radii 0.5 AU, no gravitational softening Radiative transfer No feedback from protostars Intrinsic protostellar luminosity unimportant Gives a lower limit on the effects of radiative feedback Accretion luminosity underestimated (energy liberated from 0.5 AU to stellar surface)

11 BBB2003: Typical molecular cloud Jeans mass 1 M, Opacity limit 3 MJ, P(k)k -4 BBB2003, but with Radiative Transfer

12 BBB2003: Typical cloud: Jeans mass 1 M, P(k)k -4 with Radiative Transfer Log Column Density Mass weight temperature (Log K)

13 Log Column Density BB2005: Dense cloud: Jeans mass 1/3 M, P(k)k -4 with Radiative Transfer Mass weight temperature (Log K)

14 Radiative Feedback and the IMF Radiative feedback reduces the number of objects by factors of 3-5 Radiative feedback brings the star to brown dwarf ratio in line with observations Observations suggest a ratio of 5 ± 2 Chabrier 2003; Greissl et al. 2007; Luhman 2007; Andersen et al Simulations: 25:5 ~ 5 Furthermore, dependence of the IMF on cloud density is removed K-S test on the two IMFs with radiative feedback shows them to be indistinguishable

15 The Apparent Invariance of the IMF Bate 2009b In the absence of stellar feedback, cloud fragments into objects separated by Jeans length Jeans length and Jeans mass smaller for denser clouds But, heating of the gas surrounding a newly-formed protostar inhibits nearby fragmentation Effectively increases the effective Jeans length and Jeans mass Effective Jeans length and Jeans mass increases by a larger fraction in denser clouds Show that this effective Jeans mass depends very weakly on cloud density Low-density Cloud Higher-density Cloud

16 Large-scale Simulations with Radiative Feedback Currently re-running Bate (2009a) with radiative feedback 500 M cloud, using 35,000,000 SPH particles Resolves opacity limit for fragmentation Follows: Results so far All binaries (0.02 AU) and discs to ~1 AU radius Recently reached 1.14 initial cloud free-fall times Formed 145 stars and brown dwarfs Original calculation at the same time: 403 stars and brown dwarfs

17

18

19 Large-scale Simulations with Radiative Feedback Comparison of the IMFs obtained without and with radiative feedback Confirms Bate (2009b), Offner et al. (2009) Many fewer brown dwarfs Much better statistics

20 Large-scale Simulations with Radiative Feedback Multiplicity as a function of primary mass Smaller numbers so far, but consistent with observations If anything, multiplicities are somewhat higher with radiative feedback

21 Radiation Magnetohydrodynamical Simulations Price & Bate (2009) Hydrodynamical Mass-to-flux ratio: 10 Mass-to-flux ratio: 5 Mass-to-flux ratio: 3 Upper panels: Without radiative feedback Lower panels: With radiative feedback

22 Star Formation Rate Star formation rate decreases with Increasing magnetic field strength Radiative feedback Observationally Evans et al Spitzer c2d survey, 5 clouds ~3-6% SFR/t ff Numerical results 10-32% SFR/t ff Strongest field, with radiative feedback ~10% SFR/t ff

23 Conclusions Hydrodynamical/sink particle simulations Statistics now good enough that meaningful comparison can be made with observations Reasonable multiplicity, separation, eccentricity distributions Too many brown dwarfs, too few unequal mass stellar binaries Radiative feedback has a huge effect, even for low-mass star formation Inhibits fragmentation of discs and filaments near existing protostars Solves the over-production of brown dwarfs Removes or severely weakens the dependence of the IMF on the cloud s mean Jeans mass Magnetic fields have a significant effect on large-scales Strong magnetic fields (plasma beta ~1) Can produce large-scale voids and magnetic structures in the gas Decrease the star formation efficiency, bringing it into line with observational estimates Do not seem to alter stellar masses greatly; rather decrease rate at which objects form

24 The Future: Self-gravitating radiation magnetohydrodynamical simulations Statistics as good or better than observational surveys This work was conducted as part of: the EURYI scheme award. See the EC Marie Curie Research Training Network CONSTELLATION It was also partially funded by a 2003 Philip Leverhulme Prize The calculations were performed on the UK Astrophysical Fluids Facility (UKAFF) and the University of Exeter Supercomputer

Numerical Simulations of Star Cluster Formation. Matthew Bate

Numerical Simulations of Star Cluster Formation. Matthew Bate Numerical Simulations of Star Cluster Formation Matthew Bate http://www.astro.ex.ac.uk/people/mbate Typical molecular cloud Jeans mass 1 M, Opacity limit 3 MJ, P(k) k -4 Denser cloud Jeans mass 1/3 M Lower

More information

The dependence of star cluster formation on initial conditions. Matthew Bate University of Exeter

The dependence of star cluster formation on initial conditions. Matthew Bate University of Exeter The dependence of star cluster formation on initial conditions Matthew Bate University of Exeter Stellar properties do not greatly depend on initial conditions constellation Little evidence for variation

More information

N-body Dynamics in Stellar Clusters Embedded in Gas

N-body Dynamics in Stellar Clusters Embedded in Gas N-body Dynamics in Stellar Clusters Embedded in Gas Matthew Bate, University of Exeter Kurosawa, Harries, Bate & Symington (2004) Collaborators: Ian Bonnell, St Andrews Volker Bromm, Texas Star Formation

More information

arxiv:astro-ph/ v1 17 Mar 2006

arxiv:astro-ph/ v1 17 Mar 2006 Mon. Not. R. Astron. Soc. 000, 000 000 (0000) Printed 21 January 2014 (MN LaT E X style file v2.2) The Jeans mass and the origin of the knee in the IMF arxiv:astro-ph/0603444v1 17 Mar 2006 I. A. Bonnell

More information

The Jeans mass and the origin of the knee in the IMF

The Jeans mass and the origin of the knee in the IMF Mon. Not. R. Astron. Soc. 368, 1296 1300 (2006) doi:10.1111/j.1365-2966.2006.10214.x The Jeans mass and the origin of the knee in the IMF I. A. Bonnell, 1 C. J. Clarke 2 and M. R. Bate 3 1 School of Physics

More information

The Initial Mass Function Elisa Chisari

The Initial Mass Function Elisa Chisari The Initial Mass Function AST 541 Dec 4 2012 Outline The form of the IMF Summary of observations Ingredients of a complete model A Press Schechter model Numerical simulations Conclusions The form of the

More information

Stellar, brown dwarf and multiple star properties from a radiation hydrodynamical simulation of star cluster formation

Stellar, brown dwarf and multiple star properties from a radiation hydrodynamical simulation of star cluster formation Mon. Not. R. Astron. Soc. 419, 3115 3146 (2012) doi:10.1111/j.1365-2966.2011.19955.x Stellar, brown dwarf and multiple star properties from a radiation hydrodynamical simulation of star cluster formation

More information

The formation of a star cluster: predicting the properties of stars and brown dwarfs

The formation of a star cluster: predicting the properties of stars and brown dwarfs Mon. Not. R. Astron. Soc. 339, 577 599 (2003) The formation of a star cluster: predicting the properties of stars and brown dwarfs Matthew R. Bate, 1,2 Ian A. Bonnell 3 and Volker Bromm 2,4 1 School of

More information

Formation of massive stars : a review

Formation of massive stars : a review Formation of massive stars : a review Patrick Hennebelle (a former «star formation ignorant» Ant s postdoc) Benoit Commerçon, Marc Joos, Andrea Ciardi, Gilles Chabrier One of the Constellation network

More information

The formation mechanism of brown dwarfs

The formation mechanism of brown dwarfs Mon. Not. R. Astron. Soc. 332, L65 L68 (2002) The formation mechanism of brown dwarfs Matthew R. Bate, 1,2P Ian A. Bonnell 3 and Volker Bromm 2,4 1 School of Physics, University of Exeter, Stocker Road,

More information

Formation of massive stars: a review

Formation of massive stars: a review Formation of massive stars: a review Patrick Hennebelle Thanks to: Benoît Commerçon, Marc Joos, Andrea Ciardi Gilles Chabrier, Romain Teyssier How massive stars form? -Can we form massive stars in spite

More information

The effect of magnetic fields on the formation of circumstellar discs around young stars

The effect of magnetic fields on the formation of circumstellar discs around young stars Astrophysics and Space Science DOI 10.1007/sXXXXX-XXX-XXXX-X The effect of magnetic fields on the formation of circumstellar discs around young stars Daniel J. Price and Matthew R. Bate c Springer-Verlag

More information

The Competitive Accretion Debate

The Competitive Accretion Debate The Competitive Accretion Debate 1,2 Paul C. Clark 2 Ralf S. Klessen 3 Ian A. Bonnell 3 Rowan J. Smith 1 KITP 2 University of Heidelberg 3 University of St Andrews What is CA and how does it work? Theory

More information

The effect of magnetic fields on star cluster formation

The effect of magnetic fields on star cluster formation Mon. Not. R. Astron. Soc. 000, 1 16 (2007) Printed 15 January 2008 (MN LATEX style file v2.2) The effect of magnetic fields on star cluster formation Daniel J. Price and Matthew R. Bate School of Physics,

More information

MAGNETIC FIELDS IN STAR FORMATION: FROM GALAXIES TO STARS

MAGNETIC FIELDS IN STAR FORMATION: FROM GALAXIES TO STARS To appear in Magnetic fields in the Universe II (2008) RevMexAA(SC) MAGNETIC FIELDS IN STAR FORMATION: FROM GALAXIES TO STARS Daniel J. Price, 1 Matthew R. Bate 1 and Clare L. Dobbs 1 RESUMEN Favor de

More information

Early Phases of Star Formation

Early Phases of Star Formation Early Phases of Star Formation Philippe André, CEA/SAp Saclay Outline Introduction: The earliest stages of the star formation process Probing the formation and evolution of prestellar cores with Herschel

More information

arxiv:astro-ph/ v1 14 Nov 2006

arxiv:astro-ph/ v1 14 Nov 2006 Mon. Not. R. Astron. Soc. 000, 000 000 (0000) Printed 4 December 2013 (MN LATEX style file v2.2) On the relative motions of dense cores and envelopes in star-forming molecular clouds arxiv:astro-ph/0611421v1

More information

The formation of close binary systems by dynamical interactions and orbital decay

The formation of close binary systems by dynamical interactions and orbital decay Mon. Not. R. Astron. Soc. 336, 705 713 (2002) The formation of close binary systems by dynamical interactions and orbital decay Matthew R. Bate, 1,2 Ian A. Bonnell 3 and Volker Bromm 2,4 1 School of Physics,

More information

Formation Mechanisms of Brown Dwarfs: Observations & Theories. Dan Li April 2009

Formation Mechanisms of Brown Dwarfs: Observations & Theories. Dan Li April 2009 Formation Mechanisms of Brown Dwarfs: Observations & Theories Dan Li April 2009 What is brown dwarf (BD)? BD Mass : upper-limit ~ 0.075 M lower-limit ~ 0.013 M (?) Differences between BD and giant planet:

More information

An overview of star formation

An overview of star formation An overview of star formation Paul Clark ITA: Ralf Klessen Robi Banerjee Simon Glover Ian Bonnell Clare Dobbs Jim Dale Why study star formation? Stars chemically the enrich the Universe, so star formation

More information

(Numerical) study of the collapse and of the fragmentation of prestellar dense core

(Numerical) study of the collapse and of the fragmentation of prestellar dense core (Numerical) study of the collapse and of the fragmentation of prestellar dense core Benoît Commerçon Supervisors: E. Audit, G. Chabrier and P. Hennebelle Collaborator: R. Teyssier (3D - AMR) CEA/DSM/IRFU/SAp

More information

Revealing and understanding the low-mass end of the IMF. Low-mass part of the Initial Mass Function Star, brown dwarf formation. G.

Revealing and understanding the low-mass end of the IMF. Low-mass part of the Initial Mass Function Star, brown dwarf formation. G. Revealing and understanding the low-mass end of the IMF Low-mass part of the Initial Mass Function Star, brown dwarf formation G. Chabrier Field: Resolved objects IMF down to the HB limit Salpeter Kroupa

More information

The Effects of Radiative Transfer on Low-Mass Star Formation

The Effects of Radiative Transfer on Low-Mass Star Formation The Effects of Radiative Transfer on Low-Mass Star Formation Stella Offner NSF Fellow, ITC Dense Cores in Dark Clouds Oct 23 2009 Collaborators: Chris McKee (UC Berkeley), Richard Klein (UC Berkeley; LLNL),

More information

Star formation Part III

Star formation Part III Lecture 4 Star formation Part III Lecture Universität Heidelberg WS 11/12 Dr. C. Mordasini Based partially on script of Prof. W. Benz Matthew R. Bate Mentor Prof. T. Henning Lecture 4 overview 1. Heating

More information

Gravitational collapse of gas

Gravitational collapse of gas Gravitational collapse of gas Assume a gas cloud of mass M and diameter D Sound speed for ideal gas is c s = γ P ρ = γ nkt ρ = γ kt m Time for sound wave to cross the cloud t sound = D == D m c s γ kt

More information

Gravitational fragmentation of discs can form stars with masses

Gravitational fragmentation of discs can form stars with masses Gravitational fragmentation of discs can form stars with masses from ~3 M J to ~200 M J (0.2M ) Defining stars, brown dwarfs Stars and planets Objects formed by gravitational instability on a dynamical

More information

The Formation of Star Clusters

The Formation of Star Clusters The Formation of Star Clusters Orion Nebula Cluster (JHK) - McCaughrean Jonathan Tan University of Florida & KITP In collaboration with: Brent Buckalew (ERAU), Michael Butler (UF u-grad), Jayce Dowell

More information

while the Planck mean opacity is defined by

while the Planck mean opacity is defined by PtII Astrophysics Lent, 2016 Physics of Astrophysics Example sheet 4 Radiation physics and feedback 1. Show that the recombination timescale for an ionised plasma of number density n is t rec 1/αn where

More information

Forming Gas-Giants Through Gravitational Instability: 3D Radiation Hydrodynamics Simulations and the Hill Criterion

Forming Gas-Giants Through Gravitational Instability: 3D Radiation Hydrodynamics Simulations and the Hill Criterion Forming Gas-Giants Through Gravitational Instability: 3D Radiation Hydrodynamics Simulations and the Hill Criterion Patrick D Rogers & James Wadsley June 15, 2012 Forming Gas-Giants Through Gravitational

More information

Early Stages of (Low-Mass) Star Formation: The ALMA Promise

Early Stages of (Low-Mass) Star Formation: The ALMA Promise Early Stages of (Low-Mass) Star Formation: The ALMA Promise Philippe André, CEA/SAp Saclay Outline Introduction: Prestellar cores and the origin of the IMF Identifying proto-brown dwarfs Bate et al. 1995

More information

The formation of binary stars

The formation of binary stars The formation of binary stars Motivation: Best testbed for star formation theory Report: Progress in observations and simulations And in memory of: Eduardo Delgado Donate 3.10.77-10.2.07 Progress in observations

More information

From Massive Cores to Massive Stars

From Massive Cores to Massive Stars From Massive Cores to Massive Stars Mark Krumholz Princeton University / UC Santa Cruz Collaborators: Richard Klein, Christopher McKee (UC Berkeley) Kaitlin Kratter, Christopher Matzner (U. Toronto) Jonathan

More information

Star Cluster Formation

Star Cluster Formation Star Cluster Formation HST Colin Hill Princeton Astrophysics 4 December 2012 Trapezium VLT Outline Star Clusters: Background + Observations The Life of a Cluster - Fragmentation - Feedback Effects - Mass

More information

Brown dwarf formation by gravitational fragmentation of massive, extended protostellar discs

Brown dwarf formation by gravitational fragmentation of massive, extended protostellar discs Mon. Not. R. Astron. Soc. 382, L30 L34 (2007) doi:10.1111/j.1745-3933.2007.00383.x Brown dwarf formation by gravitational fragmentation of massive, extended protostellar discs Dimitris Stamatellos, David

More information

BROWN DWARF FORMATION BY DISC FRAGMENTATION

BROWN DWARF FORMATION BY DISC FRAGMENTATION BROWN DWARF FORMATION BY DISC FRAGMENTATION Ant Whitworth, Cardiff Dimitri Stamatellos, Cardiff plus Steffi Walch, Cardiff Murat Kaplan, Cardiff Simon Goodwin, Sheffield David Hubber, Sheffield Richard

More information

Thermal physics, cloud geometry and the stellar initial mass function

Thermal physics, cloud geometry and the stellar initial mass function Mon. Not. R. Astron. Soc. 359, 211 222 (2005) doi:10.1111/j.1365-2966.2005.08881.x Thermal physics, cloud geometry and the stellar initial mass function Richard B. Larson Yale Astronomy Department, Box

More information

Multiplicity in early stellar evolution!

Multiplicity in early stellar evolution! Multiplicity in early stellar evolution Bo Reipurth: University of Hawaii Alan Boss: Carnegie Institute of Washington Cathie Clarke, IOA Cambridge Simon Goodwin: University of Sheffield Luis Felipe Rodriguez:

More information

arxiv:astro-ph/ v1 28 Jun 2005

arxiv:astro-ph/ v1 28 Jun 2005 Mon. Not. R. Astron. Soc. 000, 000 000 (0000) Printed 8 June 2018 (MN LaT E X style file v2.2) Binary systems and stellar mergers in massive star formation arxiv:astro-ph/0506689v1 28 Jun 2005 Ian A. Bonnell

More information

Substellar companions and isolated planetary-mass objects from protostellar disc fragmentation

Substellar companions and isolated planetary-mass objects from protostellar disc fragmentation Mon. Not. R. Astron. Soc. 346, L36 L40 (2003) Substellar companions and isolated planetary-mass objects from protostellar disc fragmentation W. K. M. Rice, 1 P. J. Armitage, 2,3 I. A. Bonnell, 1 M. R.

More information

Substellar companions and isolated planetary-mass objects from protostellar disc fragmentation

Substellar companions and isolated planetary-mass objects from protostellar disc fragmentation Mon. Not. R. Astron. Soc. 346, L36 L40 (2003) Substellar companions and isolated planetary-mass objects from protostellar disc fragmentation W. K. M. Rice, 1 P. J. Armitage, 2,3 I. A. Bonnell, 1 M. R.

More information

arxiv:astro-ph/ v1 17 Mar 2006

arxiv:astro-ph/ v1 17 Mar 2006 The Origin of the Initial Mass Function Ian A. Bonnell University of St Andrews Richard B. Larson Yale University Hans Zinnecker Astrophysikalisches Institut Potsdam arxiv:astro-ph/0603447v1 17 Mar 2006

More information

Accretion Mechanisms

Accretion Mechanisms Massive Protostars Accretion Mechanism Debate Protostellar Evolution: - Radiative stability - Deuterium shell burning - Contraction and Hydrogen Ignition Stahler & Palla (2004): Section 11.4 Accretion

More information

The Origin of the Initial Mass Function

The Origin of the Initial Mass Function The Origin of the Initial Mass Function Ian A. Bonnell University of St Andrews Richard B. Larson Yale University Hans Zinnecker Astrophysikalisches Institut Potsdam Bonnell et al.: Origin of the Initial

More information

Star Formation and Protostars

Star Formation and Protostars Stellar Objects: Star Formation and Protostars 1 Star Formation and Protostars 1 Preliminaries Objects on the way to become stars, but extract energy primarily from gravitational contraction are called

More information

Binary and Mul,ple Stars

Binary and Mul,ple Stars Binary and Mul,ple Stars Types of Mul,ple Systems Binaries Visual SB1 SB2 Triples Heirarchical Quadruples Trapezia T Tau triple system Kohler et al 2016 Observa,ons Imaging Rayleigh Limit: Resolu,on =

More information

Theoretical ideas About Galaxy Wide Star Formation! Star Formation Efficiency!

Theoretical ideas About Galaxy Wide Star Formation! Star Formation Efficiency! Theoretical ideas About Galaxy Wide Star Formation Theoretical predictions are that galaxy formation is most efficient near a mass of 10 12 M based on analyses of supernova feedback and gas cooling times

More information

Gravitational Collapse and Star Formation

Gravitational Collapse and Star Formation Astrophysical Dynamics, VT 010 Gravitational Collapse and Star Formation Susanne Höfner Susanne.Hoefner@fysast.uu.se The Cosmic Matter Cycle Dense Clouds in the ISM Black Cloud Dense Clouds in the ISM

More information

Brown dwarf & star formation and the bottom of the IMF: a critical look

Brown dwarf & star formation and the bottom of the IMF: a critical look Brown dwarf & star formation and the bottom of the IMF: a critical look Gilles Chabrier ENS-Lyon U. Exeter Origin of stars and their planetary systems Mac Master University, June 2012 Field: Resolved objects

More information

Philamentary Structure and Velocity Gradients in the Orion A Cloud

Philamentary Structure and Velocity Gradients in the Orion A Cloud Red: CO from Mini survey Orion B Philamentary Structure and Velocity Gradients in the Orion A Cloud Spitzer Orion Cloud Survey: 10 sq. degrees in Orion A and Orion B mapped between 2004-2009 Orion A Green

More information

The First Stars. Simone Ferraro Princeton University. Sept 25, 2012

The First Stars. Simone Ferraro Princeton University. Sept 25, 2012 The First Stars Simone Ferraro Princeton University Sept 25, 2012 Outline Star forming minihalos at high z Cooling physics and chemistry Gravitational Collapse and formation of protostar Magnetic fields

More information

igure 4 of McMullin et al McMullin et al Testi & Sargent 1998 Figure 1 of Testi & Sargent 1998:

igure 4 of McMullin et al McMullin et al Testi & Sargent 1998 Figure 1 of Testi & Sargent 1998: igure 4 of McMullin et al. 1994. Figure 1 of Testi & Sargent 1998: McMullin et al. 1994 BIMA with (only!) three elements Eight configurationsàcoverage of 2 kλ to 30 kλ Naturally wtd. Beam of 11" x 6" (for

More information

Low mass star formation. Mark Thompson (with contributions from Jennifer Hatchell, Derek Ward-Thompson, Jane Greaves, Larry Morgan...

Low mass star formation. Mark Thompson (with contributions from Jennifer Hatchell, Derek Ward-Thompson, Jane Greaves, Larry Morgan... Low mass star formation Mark Thompson (with contributions from Jennifer Hatchell, Derek Ward-Thompson, Jane Greaves, Larry Morgan...) The observational state of play Multiwavelength surveys are bringing

More information

The Early Evolution of low mass stars and Brown Dwarfs. I. Baraffe University of Exeter

The Early Evolution of low mass stars and Brown Dwarfs. I. Baraffe University of Exeter The Early Evolution of low mass stars and Brown Dwarfs I. Baraffe University of Exeter 1. Some observational/theoretical facts Spread in the HRD Lithium depletion Evidence for episodic accretion - Embedded

More information

arxiv: v1 [astro-ph] 5 Jun 2008

arxiv: v1 [astro-ph] 5 Jun 2008 Draft version December 15, 2017 Preprint typeset using L A TEX style emulateapj v. 08/13/06 DRIVEN AND DECAYING TURBULENCE SIMULATIONS OF LOW-MASS STAR FORMATION: FROM CLUMPS TO CORES TO PROTOSTARS Stella

More information

! what determines the initial mass function of stars (IMF)? dn /dm

! what determines the initial mass function of stars (IMF)? dn /dm ! what determines the initial mass function of stars (IMF)? dn /dm M ! what determines the initial mass function of stars (IMF)?! What determines the total mass of stars that can form in the cloud? dn

More information

arxiv: v2 [astro-ph] 1 Apr 2008

arxiv: v2 [astro-ph] 1 Apr 2008 Mon. Not. R. Astron. Soc. 000, 000 000 (0000) Printed 3 December 2013 (MN LATEX style file v2.2) The star formation efficiency and its relation to variations in the initial mass function arxiv:0803.4053v2

More information

IV From cores to stars

IV From cores to stars IV From cores to stars 4.0 The Jeans condition When the supporting pressure in a region is not able to hold that region up against gravitational collapse it is said to be Jeans unstable. The Jeans length

More information

The Formation of Close Binary Stars

The Formation of Close Binary Stars The Formation of Binary Stars fa U Symposium, Vol. 200, 2001 H. Zinnecker and R. D. Mathieu, eds. The Formation of Close Binary Stars Ian A. Bonnell University of St Andrews, Physics and Astronomy, North

More information

Kengo TOMIDA Kohji Tomisaka, Masahiro N. Machida, Tomoaki Matsumoto, Satoshi Okuzumi, Yasunori Hori

Kengo TOMIDA Kohji Tomisaka, Masahiro N. Machida, Tomoaki Matsumoto, Satoshi Okuzumi, Yasunori Hori 09/19/2014 Department of Astrophysical Sciences, Princeton University Department of Physics, University of Tokyo JSPS Research Fellow Kengo TOMIDA Kohji Tomisaka, Masahiro N. Machida, Tomoaki Matsumoto,

More information

FLASH Code Tutorial. part III sink particles & feedback. Robi Banerjee Hamburger Sternwarte

FLASH Code Tutorial. part III sink particles & feedback. Robi Banerjee Hamburger Sternwarte FLASH Code Tutorial part III sink particles & feedback Robi Banerjee Hamburger Sternwarte banerjee@hs.uni-hamburg.de Motivation: modelling of dense regions in collapse simulations, e.g. star formation

More information

Ionization Feedback in Massive Star Formation

Ionization Feedback in Massive Star Formation Ionization Feedback in Massive Star Formation Thomas Peters Institut für Theoretische Astrophysik Zentrum für Astronomie der Universität Heidelberg Ralf Klessen, Robi Banerjee (ITA, Heidelberg) Mordecai-Mark

More information

Disk Formation and Jet Driving in Collapsing Cloud Cores

Disk Formation and Jet Driving in Collapsing Cloud Cores Disk Formation and Jet Driving in Collapsing Cloud Cores Masahiro Machida (Kyushu University) Star Formation Process Observations have shown that Low-velocity outflows and high-velocity jets are ubiquitous

More information

The Migration of Giant Planets in Massive Protoplanetary Discs

The Migration of Giant Planets in Massive Protoplanetary Discs The Migration of Giant Planets in Massive Protoplanetary Discs Kate E. M. Robinson A thesis submitted in partial fulfilment for the requirements for the degree of Master of Science at the University of

More information

Chapter 16 Lecture. The Cosmic Perspective Seventh Edition. Star Birth Pearson Education, Inc.

Chapter 16 Lecture. The Cosmic Perspective Seventh Edition. Star Birth Pearson Education, Inc. Chapter 16 Lecture The Cosmic Perspective Seventh Edition Star Birth 2014 Pearson Education, Inc. Star Birth The dust and gas between the star in our galaxy is referred to as the Interstellar medium (ISM).

More information

How do protostars get their mass?

How do protostars get their mass? How do protostars get their mass? Phil Myers Harvard-Smithsonian Center for Astrophysics Origin of Stellar Masses Tenerife, Spain October 18, 2010 Introduction How does nature make a star? a star of particular

More information

Stellar Birth. Stellar Formation. A. Interstellar Clouds. 1b. What is the stuff. Astrophysics: Stellar Evolution. A. Interstellar Clouds (Nebulae)

Stellar Birth. Stellar Formation. A. Interstellar Clouds. 1b. What is the stuff. Astrophysics: Stellar Evolution. A. Interstellar Clouds (Nebulae) Astrophysics: Stellar Evolution 1 Stellar Birth Stellar Formation A. Interstellar Clouds (Nebulae) B. Protostellar Clouds 2 C. Protostars Dr. Bill Pezzaglia Updated: 10/02/2006 A. Interstellar Clouds 1.

More information

arxiv: v1 [astro-ph.sr] 29 Jul 2011

arxiv: v1 [astro-ph.sr] 29 Jul 2011 Mon. Not. R. Astron. Soc. 000, 000 000 (0000) Printed 2 August 2011 (MN LATEX style file v2.2) arxiv:1108.0009v1 [astro-ph.sr] 29 Jul 2011 Collapse of a molecular cloud core to stellar densities: the formation

More information

Observational signatures of proto brown dwarf formation in protostellar disks

Observational signatures of proto brown dwarf formation in protostellar disks Mem. S.A.It. Vol. 84, 88 c SAIt 213 Memorie della Observational signatures of proto brown dwarf formation in protostellar disks O. V. Zakhozhay 1, E. I. Vorobyov 2,3, and M. M. Dunham 4 1 Main Astronomical

More information

Simulations of massive magnetized dense core collapse

Simulations of massive magnetized dense core collapse Simulations of massive magnetized dense core collapse Matthias González Benoît Commerçon, Neil Vaytet Raphaël Mignon-Risse Laboratoire AIM, Université Paris Diderot-CEA-CNRS, CEA Saclay Outline 1 Context

More information

Clicker Question: Clicker Question: What is the expected lifetime for a G2 star (one just like our Sun)?

Clicker Question: Clicker Question: What is the expected lifetime for a G2 star (one just like our Sun)? How Long do Stars Live (as Main Sequence Stars)? A star on Main Sequence has fusion of H to He in its core. How fast depends on mass of H available and rate of fusion. Mass of H in core depends on mass

More information

Other stellar types. Open and globular clusters: chemical compositions

Other stellar types. Open and globular clusters: chemical compositions Other stellar types Some clusters have hotter stars than we find in the solar neighbourhood -- O, B, A stars -- as well as F stars, and cooler stars (G, K, M) Hence we can establish intrinsic values (M

More information

Chapter 8: The Family of Stars

Chapter 8: The Family of Stars Chapter 8: The Family of Stars Motivation We already know how to determine a star s surface temperature chemical composition surface density In this chapter, we will learn how we can determine its distance

More information

The Evolution of the Multiplicity of Embedded Protostars II: Binary Separation Distribution & Analysis 1

The Evolution of the Multiplicity of Embedded Protostars II: Binary Separation Distribution & Analysis 1 The Evolution of the Multiplicity of Embedded Protostars II: Binary Separation Distribution & Analysis 1 Michael S. Connelley 1, Bo Reipurth 2, and Alan T. Tokunaga 3 ABSTRACT We present the Class I protostellar

More information

The protostellar luminosity problem: historical perspective. Lee Hartmann, University of Michigan

The protostellar luminosity problem: historical perspective. Lee Hartmann, University of Michigan The protostellar luminosity problem: historical perspective Lee Hartmann, University of Michigan A subject made possible by IRAS... embedded objects are not more luminous than CTTS L(bol)s imply dm/dt

More information

!"#$%&'(#)*'+*,+ %#--./&+0&'-&+1*"&-+ 0*2'+(*+! #"#1(&".9.'$+:"*(*1;<(&"-+

!#$%&'(#)*'+*,+ %#--./&+0&'-&+1*&-+ 0*2'+(*+! ##1(&.9.'$+:*(*1;<(&-+ !"#$%&'(#)*'+*,+ %#--./&+0&'-&+1*"&-+ 0*2'+(*+!3444+567+ 18#"#1(&".9.'$+:"*(*1;

More information

Components of Galaxies Stars What Properties of Stars are Important for Understanding Galaxies?

Components of Galaxies Stars What Properties of Stars are Important for Understanding Galaxies? Components of Galaxies Stars What Properties of Stars are Important for Understanding Galaxies? Temperature Determines the λ range over which the radiation is emitted Chemical Composition metallicities

More information

Origin of high-mass protostars in Cygnus-X

Origin of high-mass protostars in Cygnus-X T. Csengeri Service d Astrophysique, CEA-Saclay Supervisor: Co-advisor: Collaborators: S. Bontemps N. Schneider F. Motte F. Gueth P. Hennebelle S. Dib Ph. André 7. April 2010 - From stars to Galaxies,

More information

arxiv: v2 [astro-ph.co] 18 Jun 2012

arxiv: v2 [astro-ph.co] 18 Jun 2012 Mon. Not. R. Astron. Soc. 000, 1 8 (2010) Printed 14 October 2018 (MN LATEX style file v2.2) Variable Accretion Rates and Fluffy First Stars arxiv:1112.4157v2 [astro-ph.co] 18 Jun 2012 Rowan J. Smith 1,

More information

Stellar Populations: Resolved vs. unresolved

Stellar Populations: Resolved vs. unresolved Outline Stellar Populations: Resolved vs. unresolved Individual stars can be analyzed Applicable for Milky Way star clusters and the most nearby galaxies Integrated spectroscopy / photometry only The most

More information

The formation of Brown dwarf :

The formation of Brown dwarf : The formation of Brown dwarf : What do we (not) know/understand? Gilles Chabrier CRAL, ENS-Lyon/U. Exeter Which dominant mechanism(s) determine(s) the IMF? 1) what do OBSERVATIONS say? II) which dominant

More information

Dynamics of Astrophysical Discs

Dynamics of Astrophysical Discs Dynamics of Astrophysical Discs 16 lectures, 3 example classes http://www.damtp.cam.ac.uk/user/hl278/dad.html Henrik Latter e-mail: hl278@cam.ac.uk 16 lectures Tu. Th. 10 Course Outline Office: F1.19 hl278@cam.

More information

Limits on the primordial stellar multiplicity

Limits on the primordial stellar multiplicity A&A 439, 565 569 (2005) DOI: 10.1051/0004-6361:20052654 c ESO 2005 Astronomy & Astrophysics Limits on the primordial stellar multiplicity S. P. Goodwin 1 and P. Kroupa 2,3 1 School of Physics & Astronomy,

More information

Collapse of magnetized dense cores. Is there a fragmentation crisis?

Collapse of magnetized dense cores. Is there a fragmentation crisis? Collapse of magnetized dense cores Is there a fragmentation crisis? Patrick Hennebelle (ENS-Observatoire de Paris) Collaborators: Benoît Commerçon, Andréa Ciardi, Sébastien Fromang, Romain Teyssier, Philippe

More information

Implications of protostellar disk fragmentation

Implications of protostellar disk fragmentation Implications of protostellar disk fragmentation Eduard Vorobyov: The Institute of Astronomy, The University of Vienna, Vienna, Austria Collaborators: Shantanu Basu, The University of Western Ontario, Canada

More information

Observational Programme in Kent

Observational Programme in Kent Observational Programme in Kent ASTRO-F, WFCAM, SCUBA-2, SALT UKIRT: individual protostellar outflows SAO/MMT/LBT: individual high- mass protostars NTT/Calar Alto + SEST: rho Ophiuchus 2MASS/NTT: Rosette

More information

Thermodynamics of GMCs and the initial conditions for star formation

Thermodynamics of GMCs and the initial conditions for star formation Thermodynamics of GMCs and the initial conditions for star formation Paul Clark & Simon Glover ITA, Zentrum für Astronomie der Universität Heidelberg RUPRECHT - KARLS - UNIVERSITÄT HEIDELBERG EXZELLENZUNIVERSITÄT

More information

Magnetic fields in the early phase of massive star formation

Magnetic fields in the early phase of massive star formation Magnetic fields in the early phase of massive star formation FLASH workshop in Hamburg 16.2.2012 Daniel Seifried Hamburger Sternwarte, University of Hamburg (Robi Banerjee, Ralf Klessen, Ralph Pudritz,

More information

The stellar mass spectrum from non-isothermal gravoturbulent fragmentation

The stellar mass spectrum from non-isothermal gravoturbulent fragmentation A&A 435, 611 623 (2005) DOI: 10.1051/0004-6361:20042178 c ESO 2005 Astronomy & Astrophysics The stellar mass spectrum from non-isothermal gravoturbulent fragmentation A.-K. Jappsen 1, R. S. Klessen 1,R.B.Larson

More information

UNDERSTANDING THE IMF

UNDERSTANDING THE IMF UNDERSTANDING THE IMF Richard B. Larson Department of Astronomy, Yale University Box 208101, New Haven, CT 06520-8101, USA larson@astro.yale.edu Abstract It is suggested that the thermal physics of star-forming

More information

Brown Dwarf Formation and Jet Propagation in Core Collapse Simulations

Brown Dwarf Formation and Jet Propagation in Core Collapse Simulations Brown Dwarf Formation and Jet Propagation in Core Collapse Simulations Knot Knot Cavity (proto-b.d) Observation Riaz et al. (2017) Masahiro N Machida (Kyushu Univ.) Clumps B.D mass object Simulation Collaborators:

More information

Remember from Stefan-Boltzmann that 4 2 4

Remember from Stefan-Boltzmann that 4 2 4 Lecture 17 Review Most stars lie on the Main sequence of an H&R diagram including the Sun, Sirius, Procyon, Spica, and Proxima Centauri. This figure is a plot of logl versus logt. The main sequence is

More information

Filling the Cosmos with (Virtual) Stars. Mark Krumholz, UC Santa Cruz HiPACC Computational Astronomy Journalism Boot Camp, June 26, 2012

Filling the Cosmos with (Virtual) Stars. Mark Krumholz, UC Santa Cruz HiPACC Computational Astronomy Journalism Boot Camp, June 26, 2012 Filling the Cosmos with (Virtual) Stars Mark Krumholz, UC Santa Cruz HiPACC Computational Astronomy Journalism Boot Camp, June 26, 2012 Outline What is the interstellar medium, and how is it related to

More information

astro-ph/ Nov 94

astro-ph/ Nov 94 Mon. Not. R. Astron. Soc. 000, 000{000 (1994) The formation of close binary systems Ian A. Bonnell and Matthew R. Bate Institute of Astronomy, Madingley Road, Cambridge, CB3 0HA Accepted 1994 August 31.

More information

The turbulent formation of stars

The turbulent formation of stars The turbulent formation of stars Christoph Federrath Citation: Physics Today 71, 6, 38 (2018); doi: 10.1063/PT.3.3947 View online: https://doi.org/10.1063/pt.3.3947 View Table of Contents: http://physicstoday.scitation.org/toc/pto/71/6

More information

Energy. mosquito lands on your arm = 1 erg. Firecracker = 5 x 10 9 ergs. 1 stick of dynamite = 2 x ergs. 1 ton of TNT = 4 x ergs

Energy. mosquito lands on your arm = 1 erg. Firecracker = 5 x 10 9 ergs. 1 stick of dynamite = 2 x ergs. 1 ton of TNT = 4 x ergs Energy mosquito lands on your arm = 1 erg Firecracker = 5 x 10 9 ergs 1 stick of dynamite = 2 x 10 13 ergs 1 ton of TNT = 4 x 10 16 ergs 1 atomic bomb = 1 x 10 21 ergs Magnitude 8 earthquake = 1 x 10 26

More information

The Birth and Evolution of Brown Dwarfs

The Birth and Evolution of Brown Dwarfs The Birth and Evolution of Brown Dwarfs Tutorial for the CSPF, or should it be CSSF (Center for Stellar and Substellar Formation)? Eduardo L. Martin, IfA Outline Basic definitions Scenarios of Brown Dwarf

More information

Lecture 20: Deuterium Burning and Hydrogen Burning

Lecture 20: Deuterium Burning and Hydrogen Burning Lecture 20: Deuterium Burning and Hydrogen Burning G Star M Dwarf L Dwarf T Dwarf Hydrogen Burning Deuterium Burning Only Decreasing Luminosity Increasing Time Protostars: Accretes mass throughout protostellar

More information

The Milky Way, Hubble Law, the expansion of the Universe and Dark Matter Chapter 14 and 15 The Milky Way Galaxy and the two Magellanic Clouds.

The Milky Way, Hubble Law, the expansion of the Universe and Dark Matter Chapter 14 and 15 The Milky Way Galaxy and the two Magellanic Clouds. The Milky Way, Hubble Law, the expansion of the Universe and Dark Matter Chapter 14 and 15 The Milky Way Galaxy and the two Magellanic Clouds. Image taken from the European Southern Observatory in Chile

More information

Pre Main-Sequence Evolution

Pre Main-Sequence Evolution Stellar Astrophysics: Stellar Evolution Pre Main-Sequence Evolution The free-fall time scale is describing the collapse of the (spherical) cloud to a protostar 1/2 3 π t ff = 32 G ρ With the formation

More information

Accretion phase of star formation in clouds with different metallicities

Accretion phase of star formation in clouds with different metallicities doi:10.1093/mnras/stu2633 Accretion phase of star formation in clouds with different metallicities Masahiro N. Machida and Teppei Nakamura Department of Earth and Planetary Sciences, Faculty of Sciences,

More information