A NEW METHOD FOR OBTAINING THE STAR FORMATION LAW IN GALAXIES

被引:5
作者
Heiner, Jonathan S. [1 ]
Allen, Ronald J. [2 ]
van der Kruit, Pieter C. [3 ]
机构
[1] Univ Laval, Dept Phys Genie Phys & Opt, Quebec City, PQ G1V 0A6, Canada
[2] Space Telescope Sci Inst, Baltimore, MD 21218 USA
[3] Univ Groningen, Kapteyn Astron Inst, NL-9700 AV Groningen, Netherlands
关键词
galaxies: individual (M33); galaxies: ISM; ISM: atoms; ISM: clouds; ISM: molecules; ultraviolet: galaxies; LARGE-SCALE DISSOCIATION; GIANT MOLECULAR CLOUDS; VOLUME DENSITIES; SURFACE-DENSITY; SCHMIDT-LAW; GAS; PHOTODISSOCIATION; M33; HI; MORPHOLOGY;
D O I
10.1088/0004-637X/719/2/1244
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
We present a new observational method to evaluate the exponent of the star formation law as initially formulated by Schmidt, i.e., the power-law expression assumed to relate the rate of star formation in a volume of space to the local total gas volume density present there. Total volume densities in the gas clouds surrounding an OB association are determined with a simple model which considers the atomic hydrogen as a photodissociation product on the cloud surfaces. The photodissociating photon flux incident on the cloud is computed from the far-UV luminosity of the OB association and the geometry. As an example, we have applied this "PDR Method" to a sample of star-forming regions in M33 using Very Large Array (VLA) 21 cm data for the Hi and Galaxy Evolution Explorer (GALEX) imagery in the far-UV. With these two observables, our approach provides an estimate of the total volume density of hydrogen (atomic + molecular) in the gas clouds surrounding the young star cluster. A graph in logarithmic coordinates of the cluster UV luminosity versus the total density in the surrounding gas provides a direct measure of the exponent of the star formation law. However, we show that this plot is severely affected by observational selection, which renders large areas of the diagram inaccessible to the data. An ordinary least-squares regression fit to a straight line, therefore, gives a strongly biased result. In the present case, the slope of such a fit primarily reflects the boundary defined when the 21 cm line becomes optically thick and is no longer a reliable measure of the H I column density. We use a maximum likelihood statistical approach which can deal with truncated and skewed data, and also takes account of the large uncertainties in the total gas densities which we derive. The exponent we obtain for the Schmidt law in M33 is 1.4 +/- 0.2.
引用
收藏
页码:1244 / 1249
页数:6
相关论文
共 26 条
[1]   The gas density and "Volume" Schmidt law for spiral galaxies [J].
Abramova, O. V. ;
Zasov, A. V. .
ASTRONOMY REPORTS, 2008, 52 (04) :257-269
[2]   LARGE-SCALE DISSOCIATION OF MOLECULAR GAS IN GALAXIES BY NEWLY FORMED STARS [J].
ALLEN, RJ ;
ATHERTON, PD ;
TILANUS, RPJ .
NATURE, 1986, 319 (6051) :296-298
[3]   Evidence for the large-scale dissociation of molecular gas in the inner spiral arms of M81 [J].
Allen, RJ ;
Knapen, JH ;
Bohlin, R ;
Stecher, TP .
ASTROPHYSICAL JOURNAL, 1997, 487 (01) :171-181
[4]  
Allen RJ, 2004, ASTROPHYS SPACE SC L, V319, P731
[5]   The production of HI in photodissociation regions and a comparison with CO (1-0) emission [J].
Allen, RJ ;
Heaton, HI ;
Kaufman, MJ .
ASTROPHYSICAL JOURNAL, 2004, 608 (01) :314-322
[6]   STIS spectral imagery of the OB stars in NGC 604. II. The most luminous stars [J].
Bruhweiler, FC ;
Miskey, CL ;
Neubig, MS .
ASTRONOMICAL JOURNAL, 2003, 125 (06) :3082-3096
[7]  
BUAT V, 1989, ASTRON ASTROPHYS, V223, P42
[8]   A simple model for the relationship between star formation and surface density [J].
Dobbs, C. L. ;
Pringle, J. E. .
MONTHLY NOTICES OF THE ROYAL ASTRONOMICAL SOCIETY, 2009, 396 (03) :1579-1588
[9]   PHOTO-ELECTRIC HEATING OF INTER-STELLAR GAS [J].
DRAINE, BT .
ASTROPHYSICAL JOURNAL SUPPLEMENT SERIES, 1978, 36 (04) :595-619
[10]   The volume densities of giant molecular clouds in M83 [J].
Heiner, J. S. ;
Allen, R. J. ;
Wong, O. I. ;
van der Kruit, P. C. .
ASTRONOMY & ASTROPHYSICS, 2008, 489 (02) :533-U28