How Young Can a Cloud Be - PowerPoint PPT Presentation

1 / 20
About This Presentation
Title:

How Young Can a Cloud Be

Description:

CfA Star Formation Symposium 2004. How Young Can a Cloud Be ... R. Snell. G. Narayanan. D. Li. H. Arce. and GALFA consortium. N. Evans. L. Allen. P. Myers ... – PowerPoint PPT presentation

Number of Views:29
Avg rating:3.0/5.0
Slides: 21
Provided by: dili
Category:
Tags: cloud | snell | young

less

Transcript and Presenter's Notes

Title: How Young Can a Cloud Be


1
How Young Can a Cloud Be
  • HINSA as a New Molecular Cloud Probe

Di Li
2
Galactic HI Absorption
3
1954 Clear Statement re. Absorption Features
4
Past Observations-Technical Limitations
  • Haystack 120ft 25 0.5km/s (Myers et al.
    1978)
  • Green Bank 140ft 21 0.4 km/s (Knapp
    1974)
  • 76m Lovell Telescope 12 0.5 km/s (McCutcheon
    et al.1978 Montgomery et al. 1995 )
  • Effelsberg 100m 9, 0.5 km/s (Wilson Minn
    1977 Batrla et al. 1983 Poppel et al. 1983)
  • Arecibo 300m 4, 1 km/s (Baker Burton 1979,
    Bania Lockman 1984)
  • VLA DRAO 1 - 1.5, 1.3 km/s (Van der
    Werf et al. 1988, 1989 Gibson et al. 2000)

5
Arecibo Upgraded
Point-focused with secondary and tertiary Wider
bandwidth LO and better backends Central panel
patched Surface readjustment underway
6
Detecting Cold HI - HI Narrow Self Absorption
  • Called self-absorption in order to
    differentiate from absorption against continuum
    sources
  • HI Self-Absorption is different from the usual
    meaning of self, as in the case of thick tracer
    like CO.
  • In case of HI absorption caused by
    dark clouds, HINSA could be
    a less confusing alternative.

-10 -5 0 5 10 15 Vlsr
(km/s)
  • (Li Goldsmith 2003 ApJ, 585, 823)

7
HINSA Definition
  • HI Absorption with corresponding molecular
    emission and
  • ?V(HI Absorption) lt ?V(CO)
  • (Li Goldsmith 2003 ApJ, 585, 823)

8
Survey Statistics HINSA Detection Rate
  • 23 sources with clear HI NSA
  • Detection rate
  • 77
  • Similar Turbulent content HINSA vs. OH
  • Average non-thermal line width (km/s)
  • OH 0.83 HI 0.84
  • The raw line width of HI is on average 1km/s,
    less than two channels in DRAO survey. The
    average depth is less than 2 RMS noise in DRAO
    survey.
  • (Li Goldsmith 2003 ApJ, 585, 823)

9
Extremely Good Correlation of HI Narrow
Self-Absorption and Molecular Emission Lines
(Goldsmith Li 2004 submitted to ApJ)
10
The Real Globule?
The North condensation was previously unknown
and was found by mapping the HINSA and following
up with 13CO and C18O This morphology confirms
close connection between cold HI absorption and
molecular emission
position in CB catalog (Clemens Barvanis 1988)
(Goldsmith Li 2004 submitted to ApJ)
11
Three-Component Radiative Transfer
12
Two Useful Limiting Cases
  • Without foreground absorber is equivalent to an
    emitting cloud at the temperature differential
  • With optically thin foreground and TbTf

(Li Goldsmith 2003 ApJ, 585, 823 cf. Van der
Werf et al. 1988 )
13
Column Density of HI
  • Total HI column density derived from optical
    depth of the 21cm line
  • Average HI column density
  • If using C18O, the abundance HI/H2 is 0.15
  • The third most abundant species inside molecular
    clouds after only H2 and He, but before CO!

8x1018 cm-2
14
How Fast Does Star Form?
  • Conventional View
  • Core Ambipolar diffusion
  • Collapse Inside-out
  • Jets Deuterium Burning, Stellar energetic starts
    to take over
  • Accretion Disk the termination of infall will
    determine the final mass of the new star.
  • Fast Star Formation?
  • Clouds form by HI stream interaction (Hartmann et
    al. 2001)
  • Stars are formed on a dynamical time scale (Myr
    Elmegreen 2001).
  • Clouds are dispersed by stellar energy output
    (Elmegreen 2000)

15
Gas-Grain Reaction Network of H2 Formation
  • The variable set
  • The parameters set

16
HI Fractional Abundance Measures TIME since the
start of Atomic to Molecular Conversion
17
From Atoms to Stars
  • HgtH2 gt Cloud Complex gt
    CoregtProtostars
  • ALFA-Tau Spitzer c2d COMPLETE
  • Goodman
  • N. Ridge
  • S. Schnee
  • J. Foster
  • D. Li
  • (the COMPLETE team)

P. Goldsmith C. Brunt M. Heyer R. Snell G.
Narayanan D. Li H. Arce and GALFA consortium
N. Evans L. Allen P. Myers T. Burke (the
Spitzer legacy team)
18
HINSA Conclusions
  • HINSA with ?v lt 2 km s-1 is a widespread
    phenomenon associated with dark clouds .
  • The narrow line atomic hydrogen has significant
    column density N(HINSA)8x1018 cm-2, making it
    the third most abundant species of molecular
    clouds after H2 and He.
  • HINSA places a lower limit on molecular cloud
    core age at gt 5 million years
  • HINSA could be a good tracer for Zeeman
    measurement.
  • HINSA could provide a probe to galactic cosmic
    ray distribution.
  • Large scale HI, CO, and infrared surveys would
    build a picture of cloud formation and their
    evolution coupled with star formation.

19
Colder Gas in CNM
  • Phases in neutral medium (Wolfire et al. 1995
    McKee Ostriker 1977 Field et al. 1962)
  • Cold Neutral Medium T80 K
  • Warm Neutral Medium T8000 K
  • Existence for colder CNM (Tlt40 K)
  • Continuum absorption Heiles 2001, Kalbella et
    al. 1985
  • HI self-absorption (HISA) Knee Brunt 2001

20
HI Self Absorption
  • Cold feature revealed in deficiency of emission
  • GSH139-03-69
  • (Knee and Brunt, 2001)
Write a Comment
User Comments (0)
About PowerShow.com