4.6 Article

THE LUMINOSITY AND MASS FUNCTIONS OF LOW-MASS STARS IN THE GALACTIC DISK. I. THE CALIBRATION REGION

Journal

ASTRONOMICAL JOURNAL
Volume 136, Issue 5, Pages 1778-1798

Publisher

IOP PUBLISHING LTD
DOI: 10.1088/0004-6256/136/5/1778

Keywords

Galaxy: stellar content; stars: late-type; stars: low-mass, brown dwarfs; stars: luminosity function, mass function; surveys

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We present measurements of the luminosity and mass functions of low-mass stars constructed from a catalog of matched Sloan Digital Sky Survey (SDSS) and Two Micron All Sky Survey (2MASS) detections. This photometric catalog contains more than 25,000 matched SDSS and 2MASS point sources spanning similar to 30 deg(2) on the sky. We have obtained follow-up spectroscopy, complete to J = 16, of more than 500 low-mass dwarf candidates within a 1 deg2 subsample, and thousands of additional dwarf candidates in the remaining 29 deg2. This spectroscopic sample verifies that the photometric sample is complete, uncontaminated, and unbiased at the 99% level globally, and at the 95% level in each color range. We use this sample to derive the luminosity and mass functions of low-mass stars over nearly a decade in mass (0.7 M-circle dot > M-* > 0.1 M-circle dot). The luminosity function of the Galactic disk is statistically consistent with that measured from volume-complete samples in the solar neighborhood. We find that the logarithmically binned mass function is best fit with an M-c = 0.29 log-normal distribution, with a 90% confidence interval of M-c = 0.20-0.50. These 90% confidence intervals correspond to linearly binned mass functions peaking between 0.27 M-circle dot and 0.12 M-circle dot, where the best fit MF turns over at 0.17 M-circle dot. A power-law fit to the entire mass range sampled here, however, returns a best fit of alpha = 1.1 (where the Salpeter slope is alpha = 2.35); a broken power law returns alpha = 2.04 at masses greater than log M = -0.5 (M = 0.32 M-circle dot), and alpha = 0.2 at lower masses. These results agree well with most previous investigations, though differences in the analytic formalisms adopted to describe those mass functions, as well as the range over which the data are fit, can give the false impression of disagreement. Given the richness of modern-day astronomical data sets, we are entering the regime whereby stronger conclusions can be drawn by comparing the actual datapoints measured in different mass functions, rather than the results of analytic analyses that impose structure on the data a priori. Having validated this method to generate a low-mass luminosity function from matched SDSS/2MASS data sets, future studies will extend this technique to the entirety of the SDSS footprint.

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