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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


The Astrophysical Journal | 1983

Secondary standard stars for absolute spectrophotometry

J. B. Oke; James E. Gunn

Based on an adopted absolute spectral energy distribution for the primary standard star Alpha Lyrae, absolute fluxes are given for the four very metal-deficient F type subdwarfs HD 19445, HD 84937, BD + 26.2606 deg, and BD + 17.4703 deg. Somewhat inferior data are also given for HD 140283. The data are given for 40-A bands and cover the wavelength range from 3080 A to 12,000 A. The four stars, all near magnitude 9 and distributed around the sky, are intended as secondary standards for absolute spectrophotometry.


The Astrophysical Journal | 2004

The Three-Dimensional Power Spectrum of Galaxies from the Sloan Digital Sky Survey

Max Tegmark; Michael R. Blanton; Michael A. Strauss; Fiona Hoyle; David J. Schlegel; Roman Scoccimarro; Michael S. Vogeley; David H. Weinberg; Idit Zehavi; Andreas A. Berlind; Tamas Budavari; A. Connolly; Daniel J. Eisenstein; Douglas P. Finkbeiner; Joshua A. Frieman; James E. Gunn; A. Hamilton; Lam Hui; Bhuvnesh Jain; David E. Johnston; S. Kent; Huan Lin; Reiko Nakajima; Robert C. Nichol; Jeremiah P. Ostriker; Adrian Pope; Ryan Scranton; Uros Seljak; Ravi K. Sheth; Albert Stebbins

We measure the large-scale real-space power spectrum P(k) using a sample of 205,443 galaxies from the Sloan Digital Sky Survey, covering 2417 square degrees with mean redshift z~0.1. We employ a matrix-based method using pseudo-Karhunen-Loeve eigenmodes, producing uncorrelated minimum-variance measurements in 22 k-bands of both the clustering power and its anisotropy due to redshift-space distortions, with narrow and well-behaved window functions in the range 0.02 h/Mpc < k < 0.3h/Mpc. We pay particular attention to modeling, quantifying and correcting for potential systematic errors, nonlinear redshift distortions and the artificial red-tilt caused by luminosity-dependent bias. Our final result is a measurement of the real-space matter power spectrum P(k) up to an unknown overall multiplicative bias factor. Our calculations suggest that this bias factor is independent of scale to better than a few percent for k<0.1h/Mpc, thereby making our results useful for precision measurements of cosmological parameters in conjunction with data from other experiments such as the WMAP satellite. As a simple characterization of the data, our measurements are well fit by a flat scale-invariant adiabatic cosmological model with h Omega_m =0.201+/- 0.017 and L* galaxy sigma_8=0.89 +/- 0.02 when fixing the baryon fraction Omega_b/Omega_m=0.17 and the Hubble parameter h=0.72; cosmological interpretation is given in a companion paper.We measure the large-scale real-space power spectrum P(k) by using a sample of 205,443 galaxies from the Sloan Digital Sky Survey, covering 2417 effective square degrees with mean redshift z ≈ 0.1. We employ a matrix-based method using pseudo-Karhunen-Loeve eigenmodes, producing uncorrelated minimum-variance measurements in 22 k-bands of both the clustering power and its anisotropy due to redshift-space distortions, with narrow and well-behaved window functions in the range 0.02 h Mpc-1 < k < 0.3 h Mpc-1. We pay particular attention to modeling, quantifying, and correcting for potential systematic errors, nonlinear redshift distortions, and the artificial red-tilt caused by luminosity-dependent bias. Our results are robust to omitting angular and radial density fluctuations and are consistent between different parts of the sky. Our final result is a measurement of the real-space matter power spectrum P(k) up to an unknown overall multiplicative bias factor. Our calculations suggest that this bias factor is independent of scale to better than a few percent for k < 0.1 h Mpc-1, thereby making our results useful for precision measurements of cosmological parameters in conjunction with data from other experiments such as the Wilkinson Microwave Anisotropy Probe satellite. The power spectrum is not well-characterized by a single power law but unambiguously shows curvature. As a simple characterization of the data, our measurements are well fitted by a flat scale-invariant adiabatic cosmological model with h Ωm = 0.213 ± 0.023 and σ8 = 0.89 ± 0.02 for L* galaxies, when fixing the baryon fraction Ωb/Ωm = 0.17 and the Hubble parameter h = 0.72; cosmological interpretation is given in a companion paper.


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 | 1998

The Sloan Digital Sky Survey Photometric Camera

James E. Gunn; Michael A. Carr; C. Rockosi; M. Sekiguchi; K. Berry; Brian R. Elms; E. de Haas; Željko Ivezić; Gillian R. Knapp; Robert H. Lupton; George Pauls; R. Simcoe; R. Hirsch; D. Sanford; Shu I. Wang; D. G. York; Frederick H. Harris; J. Annis; L. Bartozek; William N. Boroski; Jon Bakken; M. Haldeman; Stephen M. Kent; Scott Holm; Donald J. Holmgren; D. Petravick; Angela Prosapio; Ron Rechenmacher; Mamoru Doi; Masataka Fukugita

We have constructed a large-format mosaic CCD camera for the Sloan Digital Sky Survey. The camera consists of two arrays, a photometric array that uses 30 2048 × 2048 SITe/Tektronix CCDs (24 μm pixels) with an effective imaging area of 720 cm2 and an astrometric array that uses 24 400 × 2048 CCDs with the same pixel size, which will allow us to tie bright astrometric standard stars to the objects imaged in the photometric camera. The instrument will be used to carry out photometry essentially simultaneously in five color bands spanning the range accessible to silicon detectors on the ground in the time-delay–and–integrate (TDI) scanning mode. The photometric detectors are arrayed in the focal plane in six columns of five chips each such that two scans cover a filled stripe 25 wide. This paper presents engineering and technical details of the camera.


Monthly Notices of the Royal Astronomical Society | 2012

The clustering of galaxies in the SDSS-III Baryon Oscillation Spectroscopic Survey: baryon acoustic oscillations in the Data Release 9 spectroscopic galaxy sample

Lauren Anderson; Eric Aubourg; S. Bailey; Florian Beutler; Vaishali Bhardwaj; Michael R. Blanton; Adam S. Bolton; J. Brinkmann; Joel R. Brownstein; A. Burden; Chia-Hsun Chuang; Antonio J. Cuesta; Kyle S. Dawson; Daniel J. Eisenstein; S. Escoffier; James E. Gunn; Hong Guo; Shirley Ho; K. Honscheid; Cullan Howlett; D. Kirkby; Robert H. Lupton; Marc Manera; Claudia Maraston; Cameron K. McBride; Olga Mena; Francesco Montesano; Robert C. Nichol; Sebastián E. Nuza; Matthew D. Olmstead

We present a one per cent measurement of the cosmic distance scale from the detections of the baryon acoustic oscillations in the clustering of galaxies from the Baryon Oscillation Spectroscopic Survey (BOSS), which is part of the Sloan Digital Sky Survey III (SDSS-III). Our results come from the Data Release 11 (DR11) sample, containing nearly one million galaxies and covering approximately


The Astronomical Journal | 2006

The 2.5 m Telescope of the Sloan Digital Sky Survey

James E. Gunn; Walter A. Siegmund; Edward J. Mannery; Russell Owen; Charles L. Hull; R. French Leger; Larry N. Carey; Gillian R. Knapp; Donald G. York; William N. Boroski; Stephen M. Kent; Robert H. Lupton; Constance M. Rockosi; Michael L. Evans; Patrick Waddell; John Anderson; James Annis; John C. Barentine; Larry M. Bartoszek; Steven Bastian; Stephen B. Bracker; Howard J. Brewington; Charles Briegel; J. Brinkmann; Yorke J. Brown; Michael A. Carr; Paul C. Czarapata; Craig Drennan; Thomas W. Dombeck; Glenn R. Federwitz

8\,500


Physical Review D | 2006

Cosmological constraints from the SDSS luminous red galaxies

Max Tegmark; Daniel J. Eisenstein; Michael A. Strauss; David H. Weinberg; Michael R. Blanton; Joshua A. Frieman; Masataka Fukugita; James E. Gunn; A. Hamilton; Gillian R. Knapp; Robert C. Nichol; Jeremiah P. Ostriker; Nikhil Padmanabhan; Will J. Percival; David J. Schlegel; Donald P. Schneider; Roman Scoccimarro; Uros Seljak; Hee-Jong Seo; M. E. C. Swanson; Alexander S. Szalay; Michael S. Vogeley; Jaiyul Yoo; Idit Zehavi; Kevork N. Abazajian; Scott F. Anderson; James Annis; Neta A. Bahcall; Bruce A. Bassett; Andreas A. Berlind

square degrees and the redshift range


The Astrophysical Journal | 1965

On the Density of Neutral Hydrogen in Intergalactic Space

James E. Gunn; Bruce A. Peterson

0.2<z<0.7


The Astrophysical Journal | 2008

The Milky Way Tomography with SDSS. I. Stellar Number Density Distribution

Mario Juric; Željko Ivezić; Alyson M. Brooks; Robert H. Lupton; David J. Schlegel; Douglas P. Finkbeiner; Nikhil Padmanabhan; Nicholas A. Bond; Branimir Sesar; Constance M. Rockosi; Gillian R. Knapp; James E. Gunn; T. Sumi; Donald P. Schneider; John C. Barentine; Howard J. Brewington; J. Brinkmann; Masataka Fukugita; Michael Harvanek; S. J. Kleinman; Jurek Krzesinski; Dan Long; Eric H. Neilsen; Atsuko Nitta; Stephanie A. Snedden; Donald G. York

. We also compare these results with those from the publicly released DR9 and DR10 samples. Assuming a concordance

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Donald P. Schneider

Pennsylvania State University

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David J. Schlegel

Lawrence Berkeley National Laboratory

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