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Early Phases of Star Formation

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divergence in the high mass slope. And between field stars and clusters (Krouper 2002) ... High Resolution Study of High Mass Filament (Orion) ... – PowerPoint PPT presentation

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Title: Early Phases of Star Formation


1
Early Phases of Star Formation
MOLECULAR CLOUDS AND STAR FORMATION Paul F.
Goldsmith California Institute of Technology Jet
Propulsion Laboratory
Deriving the Core Mass Function
Di Li Jet Propulsion Laboratory Xin Guan Yu
Dai Beijing University
  • Di Li

2
Initial Mass Function (IMF)
  • Salpeter (1955)
  • dN / dM M-2.35
  • (0.4 10 M? )
  • Scalo (1986)
  • dN / dM M-2.7
  • (1.2 20 M? )
  • Massey (2001)
  • dN / dM M-2.4 (extends high mass limit to 120
    M? )
  • Scalo (2004)
  • divergence in the high mass slope
  • And between field stars and clusters

(Krouper 2002)
3
High Mass Core Sample
4
Dynamical State
  • MBE-CR critical mass of a Bonnor Ebert Sphere
  • Teq ??mH?V2/(8ln2kB )
  • M? c? ?Br2/G0.5 mass supported by static
    magnetic field
  • Li et al. 2007, ApJ 655 351

5
Core Mass Function Current View
  • A break point in CMF
  • Higher mass part mimics Salpeter IMF
  • (Johnstone Bally 2006
  • Reid Wilson 2005
  • Mookerjea et al. 2004
  • Testi Sargent 1998,
  • Motte et al.1998)

Ward-Thompson et al. 2006, Review article for PPV
6
Orion CMF 2 vs 1 !
7
Two Power Laws -- Really?
8
Least Square Fit of Discrete Cumulative Function
  • Data sample S
  • S(mi) , i 1,2, , n
  • Kernel Function F(x)
  • generate a sample according to an assumed
    distribution, e.g., a power law with index ?
  • calculate the discrete CF
  • Interpolate CF to calculate F(x)
  • Minimize ?2 to derive ?
  • ?2 ???i (F(mi) S(mi)), i 1, 2, n

9
Bootstrap
  • Traditional Inference
  • Normally distributed population
  • ( mean M SD ?)
  • Draw random samples of size n ?normally
    distributed sample mean
  • (mean M SD ?/n0.5 )
  • Bootstrap Inference
  • One sample with unknown distribution
  • draw resamples ? the distribution of a certain
    sample statistic usually approximates that of the
    population

10
Forward Fitting
Orion B
r Oph
11
Conclusions
  • The core mass function (CMF) in Orion is
    significantly flatter than the IMF, suggesting
    environmental factors shaping the IMF.
  • Direct multiple power law fit to accumulative
    function does not work.
  • Forward fitting of past works (Motte et al. 1998
    Jonhstone et al. 2000 Kerton et al. 2001
    Johnstone et al. 2001 Tothill et al. 2002
    Beuther et al. 2001 Mookerjea et al. 2004 Reid
    Wilson 2005 Johnstone Bally 2006) indicates
    that the majority of existing core samples is
    consistent with a single power law CMF with
    indices between 0.8 and 1.6.

12
Further Work From Atoms to Stars
  • HI to H2 Transition in Low Mass Regions (Taurus)
  • ALFA-Tau survey
  • 100 d2 CO/13CO 1000 d2 HI
  • large scale HINSA gradient and correlation with
    stellar population
  • High Resolution Study of High Mass Filament
    (Orion)
  • SMA Tracks on Selected Fields, mapping
    CO/13CO/C18O, N2H 3-2 and HCO 3-2.
  • Spitzer IRAC and Mid IR programs
  • VLA and CARMA
  • Collaborators
  • P. Goldsmith, R. Snell, M. Heyer, C. Brunt, G.
    Narayanan, Y. Tang
  • Q. Zhang, C. Qi
  • T. Velusamy, K. Marsh
  • T. Robisaw, C. Heiles, J.Goldston
  • A. Goodman, H. Arce , J. Foster and more from the
    COMPLETE Team.

13
Band Function Fit to CMF
  • Band function continuous two power laws
  • Use the indices from the literature and fit only
    E0
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