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The Astrophysical Journal | 2005

DETECTION OF THE BARYON ACOUSTIC PEAK IN THE LARGE-SCALE CORRELATION FUNCTION OF SDSS LUMINOUS RED GALAXIES

Daniel J. Eisenstein; Idit Zehavi; David W. Hogg; Roman Scoccimarro; Michael R. Blanton; Robert C. Nichol; Ryan Scranton; Hee-Jong Seo; Max Tegmark; Zheng Zheng; Scott F. Anderson; James Annis; Neta A. Bahcall; J. Brinkmann; Scott Burles; Francisco J. Castander; A. Connolly; István Csabai; Mamoru Doi; Masataka Fukugita; Joshua A. Frieman; Karl Glazebrook; James E. Gunn; Johnn Hendry; Gregory S. Hennessy; Zeljko Ivezic; Stephen M. Kent; Gillian R. Knapp; Huan Lin; Yeong Shang Loh

We present the large-scale correlation function measured from a spectroscopic sample of 46,748 luminous red galaxies from the Sloan Digital Sky Survey. The survey region covers 0.72h −3 Gpc 3 over 3816 square degrees and 0.16 < z < 0.47, making it the best sample yet for the study of large-scale structure. We find a well-detected peak in the correlation function at 100h −1 Mpc separation that is an excellent match to the predicted shape and location of the imprint of the recombination-epoch acoustic oscillations on the low-redshift clustering of matter. This detection demonstrates the linear growth of structure by gravitational instability between z ≈ 1000 and the present and confirms a firm prediction of the standard cosmological theory. The acoustic peak provides a standard ruler by which we can measure the ratio of the distances to z = 0.35 and z = 1089 to 4% fractional accuracy and the absolute distance to z = 0.35 to 5% accuracy. From the overall shape of the correlation function, we measure the matter density mh 2 to 8% and find agreement with the value from cosmic microwave background (CMB) anisotropies. Independent of the constraints provided by the CMB acoustic scale, we find m = 0.273 ±0.025+0.123(1+ w0)+0.137K. Including the CMB acoustic scale, we find that the spatial curvature is K = −0.010 ± 0.009 if the dark energy is a cosmological constant. More generally, our results provide a measurement of cosmological distance, and hence an argument for dark energy, based on a geometric method with the same simple physics as the microwave background anisotropies. The standard cosmological model convincingly passes these new and robust tests of its fundamental properties. Subject headings: cosmology: observations — large-scale structure of the universe — distance scale — cosmological parameters — cosmic microwave background — galaxies: elliptical and lenticular, cD


Monthly Notices of the Royal Astronomical Society | 2010

Baryon Acoustic Oscillations in the Sloan Digital Sky Survey Data Release 7 Galaxy Sample

Will J. Percival; Beth A. Reid; Daniel J. Eisenstein; Neta A. Bahcall; Tamas Budavari; Joshua A. Frieman; Masataka Fukugita; James E. Gunn; Željko Ivezić; Gillian R. Knapp; Richard G. Kron; Jon Loveday; Robert H. Lupton; Timothy A. McKay; Avery Meiksin; Robert C. Nichol; Adrian Pope; David J. Schlegel; Donald P. Schneider; David N. Spergel; Chris Stoughton; Michael A. Strauss; Alexander S. Szalay; Max Tegmark; Michael S. Vogeley; David H. Weinberg; Donald G. York; Idit Zehavi

The spectroscopic Sloan Digital Sky Survey (SDSS) Data Release 7 (DR7) galaxy sample represents the final set of galaxies observed using the original SDSS target selection criteria. We analyse the clustering of galaxies within this sample, including both the luminous red galaxy and main samples, and also include the 2-degree Field Galaxy Redshift Survey data. In total, this sample comprises 893 319 galaxies over 9100 deg(2). Baryon acoustic oscillations (BAO) are observed in power spectra measured for different slices in redshift; this allows us to constrain the distance-redshift relation at multiple epochs. We achieve a distance measure at redshift z = 0.275, of r(s)(z(d))/D-V(0.275) = 0.1390 +/- 0.0037 (2.7 per cent accuracy), where r(s)(z(d)) is the comoving sound horizon at the baryon-drag epoch, D-V(z) equivalent to [(1 + z)(2)D(A)(2)cz/H(z)](1/3), D-A(z) is the angular diameter distance and H(z) is the Hubble parameter. We find an almost independent constraint on the ratio of distances D-V(0.35)/D-V(0.2) = 1.736 +/- 0.065, which is consistent at the 1.1 sigma level with the best-fitting Lambda cold dark matter model obtained when combining our z = 0.275 distance constraint with the Wilkinson Microwave Anisotropy Probe 5-year (WMAP5) data. The offset is similar to that found in previous analyses of the SDSS DR5 sample, but the discrepancy is now of lower significance, a change caused by a revised error analysis and a change in the methodology adopted, as well as the addition of more data. Using WMAP5 constraints on Omega(b)h(2) and Omega(c) h(2), and combining our BAO distance measurements with those from the Union supernova sample, places a tight constraint on Omega(m) = 0.286 +/- 0.018 and H-0 = 68.2 +/- 2.2 km s(-1) Mpc(-1) that is robust to allowing Omega(k) not equal 0 and omega not equal -1. This result is independent of the behaviour of dark energy at redshifts greater than those probed by the BAO and supernova measurements. Combining these data sets with the full WMAP5 likelihood constraints provides tight constraints on both Omega(k) = -0.006 +/- 0.008 and omega = -0.97 +/- 0.10 for a constant dark energy equation of state.


The Astronomical Journal | 2001

Evidence for reionization at z ∼ 6: Detection of a gunn-peterson trough in a z = 6.28 quasar

Robert H. Becker; Xiaohui Fan; Richard L. White; Michael A. Strauss; Vijay K. Narayanan; Robert H. Lupton; James E. Gunn; James Annis; Neta A. Bahcall; J. Brinkmann; A. J. Connolly; István Csabai; Paul C. Czarapata; Mamoru Doi; Timothy M. Heckman; Gregory S. Hennessy; Željko Ivezić; Gillian R. Knapp; D. Q. Lamb; Timothy A. McKay; Jeffrey A. Munn; Thomas Nash; Robert C. Nichol; Jeffrey R. Pier; Gordon T. Richards; Donald P. Schneider; Chris Stoughton; Alexander S. Szalay; Aniruddha R. Thakar; D. G. York

We present moderate-resolution Keck spectroscopy of quasars at z = 5.82, 5.99, and 6.28, discovered by the Sloan Digital Sky Survey (SDSS). We find that the Ly? absorption in the spectra of these quasars evolves strongly with redshift. To z ~ 5.7, the Ly? absorption evolves as expected from an extrapolation from lower redshifts. However, in the highest-redshift object, SDSSp J103027.10+052455.0 (z = 6.28), the average transmitted flux is 0.0038 ? 0.0026 times that of the continuum level over 8450 ? 20, on the optical depth to Ly? absorption at z = 6. This is a clear detection of a complete Gunn-Peterson trough, caused by neutral hydrogen in the intergalactic medium. Even a small neutral hydrogen fraction in the intergalactic medium would result in an undetectable flux in the Ly? forest region. Therefore, the existence of the Gunn-Peterson trough by itself does not indicate that the quasar is observed prior to the reionization epoch. However, the fast evolution of the mean absorption in these high-redshift quasars suggests that the mean ionizing background along the line of sight to this quasar has declined significantly from z ~ 5 to 6, and the universe is approaching the reionization epoch at z ~ 6.


The Astronomical Journal | 2001

The Luminosity Function of Galaxies in SDSS Commissioning Data

Michael R. Blanton; Julianne J. Dalcanton; Daniel J. Eisenstein; Jon Loveday; Michael A. Strauss; Mark SubbaRao; David H. Weinberg; John Anderson; James Annis; Neta A. Bahcall; Mariangela Bernardi; J. Brinkmann; Robert J. Brunner; Scott Burles; Larry N. Carey; Francisco J. Castander; Andrew J. Connolly; István Csabai; Mamoru Doi; Douglas P. Finkbeiner; Scott D. Friedman; Joshua A. Frieman; Masataka Fukugita; James E. Gunn; Gregory S. Hennessy; Robert B. Hindsley; David W. Hogg; Takashi Ichikawa; Željko Ivezić; Stephen M. Kent

In the course of its commissioning observations, the Sloan Digital Sky Survey (SDSS) has produced one of the largest redshift samples of galaxies selected from CCD images. Using 11,275 galaxies complete to r* \ 17.6 over 140 deg2, we compute the luminosity function of galaxies in the r* band over a range (for h \ 1). The result is well-described by a Schechter function with parameters [23 \ M rp \ [16 h3 Mpc~3,


The Astronomical Journal | 2006

The Sloan Digital Sky Survey Quasar Survey: Quasar Luminosity Function from Data Release 3

Gordon T. Richards; Michael A. Strauss; Xiaohui Fan; Patrick B. Hall; Sebastian Jester; Donald P. Schneider; Daniel E. Vanden Berk; Chris Stoughton; Scott F. Anderson; Robert J. Brunner; Jim Gray; James E. Gunn; Željko Ivezić; Margaret K. Kirkland; Gillian R. Knapp; Jon Loveday; Avery Meiksin; Adrian Pope; Alexander S. Szalay; Anirudda R. Thakar; Brian Yanny; Donald G. York; J. C. Barentine; Howard J. Brewington; J. Brinkmann; Masataka Fukugita; Michael Harvanek; Stephen M. Kent; S. J. Kleinman; Jurek Krzesinski

We determine the number counts and z = 0-5 luminosity function for a well-defined, homogeneous sample of quasars from the Sloan Digital Sky Survey (SDSS). We conservatively define the most uniform statistical sample possible, consisting of 15,343 quasars within an effective area of 1622 deg2 that was derived from a parent sample of 46,420 spectroscopically confirmed broad-line quasars in the 5282 deg2 of imaging data from SDSS Data Release 3. The sample extends from i = 15 to 19.1 at z 3 and to i = 20.2 for z 3. The number counts and luminosity function agree well with the results of the Two Degree Field QSO Redshift Survey (2QZ) at redshifts and luminosities at which the SDSS and 2QZ quasar samples overlap, but the SDSS data probe to much higher redshifts than does the 2QZ sample. The number density of luminous quasars peaks between redshifts 2 and 3, although uncertainties in the selection function in this range do not allow us to determine the peak redshift more precisely. Our best-fit model has a flatter bright-end slope at high redshift than at low redshift. For z < 2.4 the data are best fit by a redshift-independent slope of ? = -3.1 [?(L) ? L?]. Above z = 2.4 the slope flattens with redshift to ? -2.37 at z = 5. This slope change, which is significant at the 5 ? level, must be accounted for in models of the evolution of accretion onto supermassive black holes.


Monthly Notices of the Royal Astronomical Society | 2010

Cosmological constraints from the clustering of the Sloan Digital Sky Survey DR7 luminous red galaxies

Beth A. Reid; Will J. Percival; Daniel J. Eisenstein; Licia Verde; David N. Spergel; Ramin A. Skibba; Neta A. Bahcall; Tamas Budavari; Joshua A. Frieman; Masataka Fukugita; J. Richard Gott; James E. Gunn; Željko Ivezić; Gillian R. Knapp; Richard G. Kron; Robert H. Lupton; Timothy A. McKay; Avery Meiksin; Robert C. Nichol; Adrian Pope; David J. Schlegel; Donald P. Schneider; Chris Stoughton; Michael A. Strauss; Alexander S. Szalay; Max Tegmark; Michael S. Vogeley; David H. Weinberg; Donald G. York; Idit Zehavi

We present the power spectrum of the reconstructed halo density field derived from a sample of luminous red galaxies (LRGs) from the Sloan Digital Sky Survey (SDSS) Seventh Data Release (DR7). The halo power spectrum has a direct connection to the underlying dark matter power for k≤ 0.2 h Mpc−1, well into the quasi-linear regime. This enables us to use a factor of ∼8 more modes in the cosmological analysis than an analysis with kmax= 0.1 h Mpc−1, as was adopted in the SDSS team analysis of the DR4 LRG sample. The observed halo power spectrum for 0.02 < k < 0.2 h Mpc−1 is well fitted by our model: χ2= 39.6 for 40 degrees of freedom for the best-fitting Λ cold dark matter (ΛCDM) model. We find Ωmh2(ns/0.96)1.2= 0.141+0.101-0.012 for a power-law primordial power spectrum with spectral index ns and Ωbh2= 0.022 65 fixed, consistent with cosmic microwave background measurements. The halo power spectrum also constrains the ratio of the comoving sound horizon at the baryon-drag epoch to an effective distance to z= 0.35: rs/DV(0.35) = 0.1097+0.0039−0.0042. Combining the halo power spectrum measurement with the Wilkinson Microwave Anisotropy Probe (WMAP) 5 year results, for the flat ΛCDM model we find Ωm= 0.289 ± 0.019 and H0= 69.4 ± 1.6 km s−1 Mpc−1. Allowing for massive neutrinos in ΛCDM, we find Σmv <0.62 eV at the 95 per cent confidence level. If we instead consider the effective number of relativistic species Neff as a free parameter, we find Neff= 4.8+1.8−1.7. Combining also with the Kowalski et al. supernova sample, we find Ωtot= 1.011 ± 0.009 and w=−0.99 ± 0.11 for an open cosmology with constant dark energy equation of state w. The power spectrum and a module to calculate the likelihoods are publicly available at http://lambda.gsfc.nasa.gov/toolbox/lrgdr/.


The Astronomical Journal | 2005

The Sloan Digital Sky Survey View of the Palomar-Green Bright Quasar Survey

Sebastian Jester; Donald P. Schneider; Gordon T. Richards; Richard F. Green; Maarten Schmidt; Patrick B. Hall; Michael A. Strauss; Daniel E. Vanden Berk; Chris Stoughton; James E. Gunn; J. Brinkmann; Stephen M. Kent; Douglas L. Tucker; Brian Yanny

We investigate the extent to which the Palomar-Green (PG) Bright Quasar Survey (BQS) is complete and representative of the general quasar population by comparing it with imaging and spectroscopy from the Sloan Digital Sky Survey (SDSS). A comparison of SDSS and PG photometry of both stars and quasars reveals the need to apply a color and magnitude recalibration to the PG data. Using the SDSS photometric catalog, we define the PGs parent sample of objects that are not main-sequence stars and simulate the selection of objects from this parent sample using the PG photometric criteria and errors. This simulation shows that the effective U - B cut in the PG survey is U - B 0.5 are inherently rare in bright surveys in any case). We find no evidence for any other systematic incompleteness when comparing the distributions in color, redshift, and FIRST radio properties of the BQS and a BQS-like subsample of the SDSS quasar sample. However, the application of a bright magnitude limit biases the BQS toward the inclusion of objects that are blue in g - i, in particular compared to the full range of g - i colors found among the i-band limited SDSS quasars, and even at i-band magnitudes comparable to those of the BQS objects.


The Astrophysical Journal | 2000

Identification of A-colored Stars and Structure in the Halo of the Milky Way from Sloan Digital Sky Survey Commissioning Data*

Brian Yanny; Heidi Jo Newberg; Steve Kent; Sally A. Laurent-Muehleisen; Jeffrey R. Pier; Gordon T. Richards; Chris Stoughton; John Anderson; James Annis; J. Brinkmann; Bing Chen; István Csabai; Mamoru Doi; Masataka Fukugita; Gregory S. Hennessy; Željko Ivezić; Gillian R. Knapp; Robert H. Lupton; Jeffrey A. Munn; Thomas Nash; Constance M. Rockosi; Donald P. Schneider; Donald G. York

A sample of 4208 objects with magnitude 15 < g* < 22 and colors of main-sequence A stars have been selected from 370 deg2 of Sloan Digital Sky Survey (SDSS) commissioning observations. The data is from two long, narrow stripes, each with an opening angle of greater than 60°, at Galactic latitudes 36° < |b| < 63° on the celestial equator. Relative photometric calibrations good to 2% and consistent absolute photometry allows this uniform sample to be treated statistically over the large area. An examination of the samples distribution shows that these stars trace considerable substructure in the halo. Large overdensities of A-colored stars in the north at (l, b, R) = (350°, 50°, 46 kpc) and in the south at (157, -58, 33 kpc) and extending over tens of degrees are present in the halo of the Milky Way. Ivezic et al. have detected the northern structure from a sample of RR Lyrae stars in the SDSS. Using photometry to separate the stars by surface gravity, both structures are shown to contain a sequence of low surface gravity stars consistent with identification as a blue horizontal branch (BHB). Both structures also contain a population of high surface gravity stars 2 mag fainter than the BHB stars, consistent with their identification as blue stragglers (BSs). The majority of the high surface gravity stars in the Galactic halo may be BS stars like these. A population of F stars associated with the A star excess in the southern structure is detected (the F stars in the northern structure at 46 kpc would be too faint for the SDSS to detect). From the numbers of detected BHB stars, lower limits to the implied mass of the structures are 6 × 106 M☉ and 2 × 106 M☉, although one does not yet know the full spatial extent of the structures. The fact that two such large clumps have been detected in a survey of only 1% of the sky indicates that such structures are not uncommon in the halo. Simple spheroidal parameters are fit to a complete sample of the remaining unclumped BHB stars and yield (at r < 40 kpc) a fit to a halo distribution with flattening (c/a = 0.65 ± 0.2) and a density falloff exponent of α = -3.2 ± 0.3.


The Astronomical Journal | 2008

The Sloan Digital Sky Survey - II:supernova survey: technical summary

Joshua A. Frieman; Bruce A. Bassett; Andrew Cameron Becker; Changsu Choi; D. Cinabro; F. DeJongh; D. L. DePoy; Ben Dilday; Mamoru Doi; Peter Marcus Garnavich; Craig J. Hogan; Jon A. Holtzman; Myungshin Im; Saurabh W. Jha; Richard Kessler; Kohki Konishi; Hubert Lampeitl; John P. Marriner; J. L. Marshall; David P. McGinnis; Gajus A. Miknaitis; Robert C. Nichol; Jose Luis Palacio Prieto; Adam G. Riess; Michael W. Richmond; Roger W. Romani; Masao Sako; Donald P. Schneider; Mathew Smith; Naohiro Takanashi

The Sloan Digital Sky Survey-II (SDSS-II) has embarked on a multi-year project to identify and measure light curves for intermediate-redshift (0.05 < z < 0.35) Type Ia supernovae (SNe Ia) using repeated five-band (ugriz) imaging over an area of 300 sq. deg. The survey region is a stripe 2.5° wide centered on the celestial equator in the Southern Galactic Cap that has been imaged numerous times in earlier years, enabling construction of a deep reference image for the discovery of new objects. Supernova imaging observations are being acquired between September 1 and November 30 of 2005-7. During the first two seasons, each region was imaged on average every five nights. Spectroscopic follow-up observations to determine supernova type and redshift are carried out on a large number of telescopes. In its first two three-month seasons, the survey has discovered and measured light curves for 327 spectroscopically confirmed SNe Ia, 30 probable SNe Ia, 14 confirmed SNe Ib/c, 32 confirmed SNe II, plus a large number of photometrically identified SNe Ia, 94 of which have host-galaxy spectra taken so far. This paper provides an overview of the project and briefly describes the observations completed during the first two seasons of operation.


The Astronomical Journal | 2007

Sloan Digital Sky Survey Standard Star Catalog for Stripe 82: The Dawn of Industrial 1% Optical Photometry

Željko Ivezić; Gajus A. Miknaitis; Huan Lin; Douglas L. Tucker; Robert H. Lupton; James E. Gunn; Gillian R. Knapp; Michael A. Strauss; Branimir Sesar; Mamoru Doi; M. Tanaka; Masataka Fukugita; Jon A. Holtzman; Steve Kent; Brian Yanny; David J. Schlegel; Douglas P. Finkbeiner; Nikhil Padmanabhan; Constance M. Rockosi; Mario Juric; Nicholas A. Bond; Brian Charles Lee; Chris Stoughton; Sebastian Jester; Hugh C. Harris; Paul Harding; Heather L. Morrison; J. Brinkmann; Donald P. Schneider; Donald G. York

We describe a standard star catalog constructed using multiple SDSS photometric observations (at least four per band, with a median of 10) in the ugriz system. The catalog includes 1.01 million nonvariable unresolved objects from the equatorial stripe 82 (|δJ2000.0| < 1.266°) in the right ascension range 20h34m-4h00m and with the corresponding r-band (approximately Johnson V-band) magnitudes in the range 14-22. The distributions of measurements for individual sources demonstrate that the photometric pipeline correctly estimates random photometric errors, which are below 0.01 mag for stars brighter than 19.5, 20.5, 20.5, 20, and 18.5 in ugriz, respectively (about twice as good as for individual SDSS runs). Several independent tests of the internal consistency suggest that the spatial variation of photometric zero points is not larger than ~0.01 mag (rms). In addition to being the largest available data set with optical photometry internally consistent at the ~1% level, this catalog provides a practical definition of the SDSS photometric system. Using this catalog, we show that photometric zero points for SDSS observing runs can be calibrated within a nominal uncertainty of 2% even for data obtained through 1 mag thick clouds, and we demonstrate the existence of He and H white dwarf sequences using photometric data alone. Based on the properties of this catalog, we conclude that upcoming large-scale optical surveys such as the Large Synoptic Survey Telescope will be capable of delivering robust 1% photometry for billions of sources.

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Donald P. Schneider

Pennsylvania State University

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István Csabai

Eötvös Loránd University

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