James Annis
Fermilab
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Featured researches published by James Annis.
The Astrophysical Journal | 2005
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 | 2004
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.
The Astronomical Journal | 2006
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
We describe the design, construction, and performance of the Sloan Digital Sky Survey telescope located at Apache Point Observatory. The telescope is a modified two-corrector Ritchey-Chretien design with a 2.5 m, f/2.25 primary, a 1.08 m secondary, a Gascoigne astigmatism corrector, and one of a pair of interchangeable highly aspheric correctors near the focal plane, one for imaging and the other for spectroscopy. The final focal ratio is f/5. The telescope is instrumented by a wide-area, multiband CCD camera and a pair of fiber-fed double spectrographs. Novel features of the telescope include the following: (1) A 3° diameter (0.65 m) focal plane that has excellent image quality and small geometric distortions over a wide wavelength range (3000-10,600 A) in the imaging mode, and good image quality combined with very small lateral and longitudinal color errors in the spectroscopic mode. The unusual requirement of very low distortion is set by the demands of time-delay-and-integrate (TDI) imaging. (2) Very high precision motion to support open-loop TDI observations. (3) A unique wind baffle/enclosure construction to maximize image quality and minimize construction costs. The telescope had first light in 1998 May and began regular survey operations in 2000.
Physical Review D | 2006
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
We measure the large-scale real-space power spectrum P(k) using luminous red galaxies (LRGs) in the Sloan Digital Sky Survey (SDSS) and use this measurement to sharpen constraints on cosmological parameters from the Wilkinson Microwave Anisotropy Probe (WMAP). We employ a matrix-based power spectrum estimation method using Pseudo-Karhunen-Loeve eigenmodes, producing uncorrelated minimum-variance measurements in 20 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 0.01h/Mpc 0.1h/Mpc and associated nonlinear complications, yet agree well with more aggressive published analyses where nonlinear modeling is crucial.
The Astronomical Journal | 2001
Daniel J. Eisenstein; James Annis; James E. Gunn; Alexander S. Szalay; Andrew J. Connolly; Robert C. Nichol; Neta A. Bahcall; Mariangela Bernardi; Scott Burles; Francisco J. Castander; Masataka Fukugita; David W. Hogg; Željko Ivezić; Gillian R. Knapp; Robert H. Lupton; Vijay K. Narayanan; Marc Postman; Daniel E. Reichart; Michael W. Richmond; Donald P. Schneider; David J. Schlegel; Michael A. Strauss; Mark SubbaRao; D. L. Tucker; Daniel E. Vanden Berk; Michael S. Vogeley; David H. Weinberg; Brian Yanny
We describe the target selection and resulting properties of a spectroscopic sample of luminous red galaxies (LRGs) from the imaging data of the Sloan Digital Sky Survey (SDSS). These galaxies are selected on the basis of color and magnitude to yield a sample of luminous intrinsically red galaxies that extends fainter and farther than the main flux-limited portion of the SDSS galaxy spectroscopic sample. The sample is designed to impose a passively evolving luminosity and rest-frame color cut to a redshift of 0.38. Additional, yet more luminous red galaxies are included to a redshift of ~0.5. Approximately 12 of these galaxies per square degree are targeted for spectroscopy, so the sample will number over 100,000 with the full survey. SDSS commissioning data indicate that the algorithm efficiently selects luminous (M^+_g ≈ -21.4) red galaxies, that the spectroscopic success rate is very high, and that the resulting set of galaxies is approximately volume limited out to z = 0.38. When the SDSS is complete, the LRG spectroscopic sample will fill over 1 h^(-3) Gpc^3 with an approximately homogeneous population of galaxies and will therefore be well suited to studies of large-scale structure and clusters out to z = 0.5.
The Astronomical Journal | 2001
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 Astrophysical Journal | 2002
Idit Zehavi; Michael R. Blanton; Joshua A. Frieman; David H. Weinberg; Hounjun J. Mo; Michael A. Strauss; Scott F. Anderson; James Annis; Neta A. Bahcall; Mariangela Bernardi; John W. Briggs; J. Brinkmann; Scott Burles; Larry N. Carey; Francisco J. Castander; Andrew J. Connolly; István Csabai; Julianne J. Dalcanton; Scott Dodelson; Mamoru Doi; Daniel J. Eisenstein; Michael L. Evans; Douglas P. Finkbeiner; Scott D. Friedman; Masataka Fukugita; James E. Gunn; Greg Hennessy; Robert B. Hindsley; Željko Ivezić; Stephen B. H. Kent
We present the first measurements of clustering in the Sloan Digital Sky Survey (SDSS) galaxy redshift survey. Our sample consists of 29,300 galaxies with redshifts 5700 km s-1 ≤ cz ≤ 39,000 km s-1, distributed in several long but narrow (25-5°) segments, covering 690 deg2. For the full, flux-limited sample, the redshift-space correlation length is approximately 8 h-1 Mpc. The two-dimensional correlation function ξ(rp,π) shows clear signatures of both the small-scale, fingers-of-God distortion caused by velocity dispersions in collapsed objects and the large-scale compression caused by coherent flows, though the latter cannot be measured with high precision in the present sample. The inferred real-space correlation function is well described by a power law, ξ(r) = (r/6.1 ± 0.2 h-1 Mpc)-1.75±0.03, for 0.1 h-1 Mpc ≤ r ≤ 16 h-1 Mpc. The galaxy pairwise velocity dispersion is σ12 ≈ 600 ± 100 km s-1 for projected separations 0.15 h-1 Mpc ≤ rp ≤ 5 h-1 Mpc. When we divide the sample by color, the red galaxies exhibit a stronger and steeper real-space correlation function and a higher pairwise velocity dispersion than do the blue galaxies. The relative behavior of subsamples defined by high/low profile concentration or high/low surface brightness is qualitatively similar to that of the red/blue subsamples. Our most striking result is a clear measurement of scale-independent luminosity bias at r 10 h-1 Mpc: subsamples with absolute magnitude ranges centered on M* - 1.5, M*, and M* + 1.5 have real-space correlation functions that are parallel power laws of slope ≈-1.8 with correlation lengths of approximately 7.4, 6.3, and 4.7 h-1 Mpc, respectively.
The Astronomical Journal | 2001
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 Astrophysical Journal | 2007
Benjamin P. Koester; Timothy A. McKay; James Annis; Risa H. Wechsler; August E. Evrard; L. E. Bleem; M. R. Becker; David E. Johnston; E. Sheldon; Robert C. Nichol; Christopher J. Miller; Ryan Scranton; Neta A. Bahcall; John C. Barentine; Howard J. Brewington; Jonathan Brinkmann; Michael Harvanek; Scott J. Kleinman; Jurek Krzesinski; Daniel C. Long; Atsuko Nitta; Donald P. Schneider; S. Sneddin; W. Voges; Donald G. York
We present a catalog of galaxy clusters selected using the maxBCG red-sequence method from Sloan Digital Sky Survey photometric data. This catalog includes 13,823 clusters with velocity dispersions greater than 400 km s-1 and is the largest galaxy cluster catalog assembled to date. They are selected in an approximately volume-limited way from a 0.5 Gpc3 region covering 7500 deg2 of sky between redshifts 0.1 and 0.3. Each cluster contains between 10 and 190 E/S0 ridgeline galaxies brighter than 0.4L* within a scaled radius R200. The tight relation between ridgeline color and redshift provides an accurate photometric redshift estimate for every cluster. Photometric redshift errors are shown by comparison to spectroscopic redshifts to be small (Δ ≃ 0:01), essentially independent of redshift, and well determined throughout the redshift range. Runs of maxBCG on realistic mock catalogs suggest that the sample is more than 90% pure and more than 85% complete for clusters with masses ≥ 1 x 1014 M⊙. Spectroscopic measurements of cluster members are used to examine line-of-sight projection as a contaminant in the identification of brightest cluster galaxies and cluster member galaxies. Spectroscopic data are also used to demonstrate the correlation between optical richness and velocity dispersion. Comparison to the combined NORAS and REFLEX X-rayYselected cluster catalogs shows that X-rayYluminous clusters are found among the optically richer maxBCG clusters. This paper is the first in a series that will consider the properties of these clusters, their galaxy populations, and their implications for cosmology.
The Astronomical Journal | 2013
Stephen A. Smee; James E. Gunn; Alan Uomoto; N. A. Roe; David J. Schlegel; Constance M. Rockosi; Michael A. Carr; French Leger; Kyle S. Dawson; Matthew D. Olmstead; J. Brinkmann; Russell Owen; Robert H. Barkhouser; K. Honscheid; Paul Harding; Dan Long; Robert H. Lupton; Craig Loomis; Lauren Anderson; James Annis; Mariangela Bernardi; Vaishali Bhardwaj; Dmitry Bizyaev; Adam S. Bolton; Howard J. Brewington; John W. Briggs; Scott Burles; James G. Burns; Francisco J. Castander; Andrew J. Connolly
We present the design and performance of the multi-object fiber spectrographs for the Sloan Digital Sky Survey (SDSS) and their upgrade for the Baryon Oscillation Spectroscopic Survey (BOSS). Originally commissioned in Fall 1999 on the 2.5 m aperture Sloan Telescope at Apache Point Observatory, the spectrographs produced more than 1.5 million spectra for the SDSS and SDSS-II surveys, enabling a wide variety of Galactic and extra-galactic science including the first observation of baryon acoustic oscillations in 2005. The spectrographs were upgraded in 2009 and are currently in use for BOSS, the flagship survey of the third-generation SDSS-III project. BOSS will measure redshifts of 1.35 million massive galaxies to redshift 0.7 and Lyα absorption of 160,000 high redshift quasars over 10,000 deg2 of sky, making percent level measurements of the absolute cosmic distance scale of the universe and placing tight constraints on the equation of state of dark energy. The twin multi-object fiber spectrographs utilize a simple optical layout with reflective collimators, gratings, all-refractive cameras, and state-of-the-art CCD detectors to produce hundreds of spectra simultaneously in two channels over a bandpass covering the near-ultraviolet to the near-infrared, with a resolving power R = λ/FWHM ~ 2000. Building on proven heritage, the spectrographs were upgraded for BOSS with volume-phase holographic gratings and modern CCD detectors, improving the peak throughput by nearly a factor of two, extending the bandpass to cover 360 nm < λ < 1000 nm, and increasing the number of fibers from 640 to 1000 per exposure. In this paper we describe the original SDSS spectrograph design and the upgrades implemented for BOSS, and document the predicted and measured performances.