4.7 Article

STAR FORMATION IN MASSIVE CLUSTERS VIA THE WILKINSON MICROWAVE ANISOTROPY PROBE AND THE SPITZER GLIMPSE SURVEY

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ASTROPHYSICAL JOURNAL
卷 709, 期 1, 页码 424-435

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IOP PUBLISHING LTD
DOI: 10.1088/0004-637X/709/1/424

关键词

Galaxy: fundamental parameters; H II regions; ISM: bubbles; stars: formation

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We use the Wilkinson Microwave Anisotropy Probe (WMAP) maximum entropy method foreground emission map combined with previously determined distances to giant H II regions to measure the free-free flux at Earth and the free-free luminosity of the Galaxy. We find a total flux f(nu) = 54, 211 Jy and a flux from 88 sources of f(nu) = 36, 043 Jy. The bulk of the sources are at least marginally resolved, with mean radii similar to 60 pc, electron density n(e) similar to 9 cm(-3), and filling factor phi(HII) approximate to 0.005 (over the Galactic gas disk). The total dust-corrected ionizing photon luminosity is Q = 3.2 x 10(53) +/- 5.1 x 10(52) photons s(-1), in good agreement with previous estimates. We use GLIMPSE and Midcourse Space Experiment (MSX) 8 mu m images to show that the bulk of the free-free luminosity is associated with bubbles having radii r similar to 5-100 pc, with a mean of similar to 20 pc. These bubbles are leaky, so that ionizing photons emitted inside the bubble escape and excite free-free emission beyond the bubble walls, producing WMAP sources that are larger than the 8 mu m bubbles. We suggest that the WMAP sources are the counterparts of the extended low density H II regions described by Mezger. The 18 most luminous WMAP sources emit half the total Galactic ionizing flux. These 18 sources have 4 x 10(51) s(-1) less than or similar to Q less than or similar to 1.6 x 10(52) s(-1), corresponding to 6 x 10(4) M-circle dot less than or similar to M-* less than or similar to 2 x 10(5) M-circle dot; half to two thirds of this will be in the central massive star cluster. We convert the measurement of Q to a Galactic star formation rate (SFR) M-* = 1.3 +/- 0.2 M-circle dot yr(-1), where the errors reflect only the error in free-free luminosity. We point out, however, that our inferred M-* is highly dependent on the exponent Gamma approximate to 1.35 of the high-mass end of the stellar initial mass function. For 1.21 < Gamma < 1.5, we find 0.9M(circle dot) yr(-1) < M-* < 2.2 M-circle dot yr(-1). We also determine a SFR of 0.14 M-circle dot yr(-1) for the Large Magellanic Cloud and 0.015 M-circle dot yr(-1) for the Small Magellanic Cloud.

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