Published April 20, 2017 | Version v1
Journal article

The Correlation between Halo Mass and Stellar Mass for the Most Massive Galaxies in the Universe

  • 1. Center for Cosmology and Particle Physics, Department of Physics, New York University, New York, NY 10013 (United States)
  • 2. Department of Physics and Astronomy, University of Utah, Salt Lake City, UT 84112 (United States)
  • 3. Key Laboratory for Research in Galaxies and Cosmology, Shanghai Astronomical Observatory, Shanghai 200030 (China)
  • 4. Kavli IPMU (WPI), UTIAS, The University of Tokyo, Kashiwa, Chiba 277-8583 (Japan)
  • 5. ICG-University of Portsmouth, PO13FX Portsmouth (United Kingdom)
  • 6. School of Physics and Astronomy, University of St. Andrews, St. Andrews, KY16 9SS (United Kingdom)
  • 7. Steward Observatory, 933 N. Cherry Street, University of Arizona, Tucson, AZ 85721 (United States)
  • 8. Department of Astronomy and CERCA, Case Western Reserve University, 10900 Euclid Avenue, Cleveland, OH 44106 (United States)
  • 9. Department of Chemistry and Physics, King's College, 133 North River Street, Wilkes Barre, PA 18711 (United States)

Description

We present measurements of the clustering of galaxies as a function of their stellar mass in the Baryon Oscillation Spectroscopic Survey. We compare the clustering of samples using 12 different methods for estimating stellar mass, isolating the method that has the smallest scatter at fixed halo mass. In this test, the stellar mass estimate with the smallest errors yields the highest amplitude of clustering at fixed number density. We find that the PCA stellar masses of Chen et al. clearly have the tightest correlation with halo mass. The PCA masses use the full galaxy spectrum, differentiating them from other estimates that only use optical photometric information. Using the PCA masses, we measure the large-scale bias as a function of M for galaxies with l o g M 11.4, correcting for incompleteness at the low-mass end of our measurements. Using the abundance matching ansatz to connect dark matter halo mass to stellar mass, we construct theoretical models of b ( M ) that match the same stellar mass function but have different amounts of scatter in stellar mass at fixed halo mass, σ l o g M . Using this approach, we find σ l o g M = 0.18 0.02 + 0.01 . This value includes both intrinsic scatter as well as random errors in the stellar masses. To partially remove the latter, we use repeated spectra to estimate statistical errors on the stellar masses, yielding an upper limit to the intrinsic scatter of 0.16 dex.

Availability note (English)

Available from http://dx.doi.org/10.3847/1538-4357/aa6845

Additional details

Identifiers

Publishing Information

Journal Title
Astrophysical Journal
Journal Volume
839
Journal Issue
2
Journal Page Range
[11 p.]
ISSN
0004-637X
CODEN
ASJOAB

INIS

Country of Publication
United States
Country of Input or Organization
International Atomic Energy Agency (IAEA)
INIS RN
51034841
Subject category
S79: ASTROPHYSICS, COSMOLOGY AND ASTRONOMY;
Descriptors DEI
BARYONS; COMPARATIVE EVALUATIONS; COSMOLOGY; GALACTIC EVOLUTION; GALAXIES; LUMINOSITY; MASS; NONLUMINOUS MATTER; OSCILLATIONS; SPECTRA; UNIVERSE
Descriptors DEC
ELEMENTARY PARTICLES; EVALUATION; EVOLUTION; FERMIONS; HADRONS; MATTER; OPTICAL PROPERTIES; PHYSICAL PROPERTIES