Final Redshift Release (DR3) and Southern Large-Scale Structures
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An Analysis Including the Latest Local Measurement of the Hubble Constant
Eur. Phys. J. C (2017) 77:882 https://doi.org/10.1140/epjc/s10052-017-5454-9 Regular Article - Theoretical Physics Constraints on inflation revisited: an analysis including the latest local measurement of the Hubble constant Rui-Yun Guo1, Xin Zhang1,2,a 1 Department of Physics, College of Sciences, Northeastern University, Shenyang 110004, China 2 Center for High Energy Physics, Peking University, Beijing 100080, China Received: 21 June 2017 / Accepted: 8 December 2017 / Published online: 18 December 2017 © The Author(s) 2017. This article is an open access publication Abstract We revisit the constraints on inflation models by current cosmological observations can be used to explore using the current cosmological observations involving the the nature of inflation. For example, the measurements of latest local measurement of the Hubble constant (H0 = CMB anisotropies have confirmed that inflation can provide 73.00 ± 1.75 km s −1 Mpc−1). We constrain the primordial a nearly scale-invariant primordial power spectrum [5–8]. power spectra of both scalar and tensor perturbations with the Although inflation took place at energy scale as high as observational data including the Planck 2015 CMB full data, 1016 GeV, where particle physics remains elusive, hundreds the BICEP2 and Keck Array CMB B-mode data, the BAO of different theoretical scenarios have been proposed. Thus data, and the direct measurement of H0. In order to relieve the selecting an actual version of inflation has become a major tension between the local determination of the Hubble con- issue in the current study. As mentioned above, the primor- stant and the other astrophysical observations, we consider dial perturbations can lead to the CMB anisotropies and LSS the additional parameter Neff in the cosmological model. -
Cosmography of the Local Universe SDSS-III Map of the Universe
Cosmography of the Local Universe SDSS-III map of the universe Color = density (red=high) Tools of the Future: roBotic/piezo fiBer positioners AstroBot FiBer Positioners Collision-avoidance testing Echidna (for SuBaru FMOS) Las Campanas Redshift Survey The first survey to reach the quasi-homogeneous regime Large-scale structure within z<0.05, sliced in Galactic plane declination “Zone of Avoidance” 6dF Galaxy Survey, Jones et al. 2009 Large-scale structure within z<0.1, sliced in Galactic plane declination “Zone of Avoidance” 6dF Galaxy Survey, Jones et al. 2009 Southern Hemisphere, colored By redshift 6dF Galaxy Survey, Jones et al. 2009 SDSS-BOSS map of the universe Image credit: Jeremy Tinker and the SDSS-III collaBoration SDSS-III map of the universe Color = density (red=high) Millenium Simulation (2005) vs Galaxy Redshift Surveys Image Credit: Nina McCurdy and Joel Primack/University of California, Santa Cruz; Ralf Kaehler and Risa Wechsler/Stanford University; Klypin et al. 2011 Sloan Digital Sky Survey; Michael Busha/University of Zurich Trujillo-Gomez et al. 2011 Redshift-space distortion in the 2D correlation function of 6dFGS along line of sight on the sky Beutler et al. 2012 Matter power spectrum oBserved by SDSS (Tegmark et al. 2006) k-3 Solid red lines: linear theory (WMAP) Dashed red lines: nonlinear corrections Note we can push linear approx to a Bit further than k~0.02 h/Mpc Baryon acoustic peaks (analogous to CMB acoustic peaks; standard rulers) keq SDSS-BOSS map of the universe Color = distance (purple=far) Image credit: -
Detection of Co Emission in Hydra I Cluster Galaxies
DETECTION OF CO EMISSION IN HYDRA I CLUSTER GALAXIES W.K. Huehtmeier Max- Planek-Ins t it ut fur Radioastr onomie Auf dem Huge1 69 5300 Bonn 1 , W. Germany Abstract A survey of bright Hydra cluster spiral galaxies for the CO(1-0) transition at 115 GHa was performed with the 15m Swedish-ESO submillimeter telescope (SEST). Five out of 15 galaxies observed have been detected in the CO(1-0) line. The largest spiral galaxy in the cluster , NGC 3312, got more CO than any spiral of the Virgo cluster. This Sa-type galaxy is optically largely distorted and disrupted on one side. It is a good candidate for ram pressure stripping while passing through the cluster's central region. A comparison with global CO properties of Virgo cluster spirals shows a relatively good agreement with the detected Hydra cluster galaxies. 0 bservations Observations were performed with the 15m Swedish-ESO submillimeter telescope (SEST) at La Silla in January 1989 under favorable meteorological conditions. At a frequency of 115 GHz the half power beamwidth (HPBW) of this telescope is 43 arcsec. The cooled Schottky heterodyne receiver had a typical receiver temperature of 350 K; the system temperature was typically 650 to 900 K depending on elevation and humidity. An accousto-optic spectrometer (Zensen 1984) with a bandwidth of 500 MHz yielded a channel width of 0.69 MHz or about 1.8 km/s. In order to improve the signal-to-noise ratio of the integrated profiles usually 5 to 10 frequency channels were averaged resulting in a resolution of 9 to 18 km/s. -
Molecular Gas Content of Galaxies in the Hydra-Centaurus Supercluster
MOLECULAR GAS CONTENT OF GALAXIES IN THE HYDRA-CENTAURUS SUPERCLUSTER W.K. Huchtmeier ™ ** <$ '"" & ^ O Max-Planck-Institut fiir Radioastronomie Auf dem Hugel 69 , 5300 Bonn 1 , W. Germany • Abstract A survey of bright spiral galaxies in the Hydra-Centaurus supercluster for the CO(l-O) transition at 115 GHz was performed with the 15m Swedish-ESO submillimeter telescope (SEST). A total of 30 galaxies have been detected in the CO(l-O) transition out of 47 observed, which is a detection rate over 60%. Global physical parameters of these galaxies derived from optical, CO, HI, and IR measurements compare very well with properties of galaxies in the Virgo cluster. The Hydra I cluster (Abell 1060) is one of the nearest clusters and very similar to the Virgo cluster in many global parameters like type, population, size, and shape. Both clusters have comparable velocity dispersions (i.e. total mass) and are spiral rich. Hydra is well isolated in velocity space and appears more circular (Kwast 1966), and might be dynamically more relaxed, although the center may contain significant substructures (Fitchett and Meritt 1988) or projected foreground groups. Both clusters contain low luminosity central X-ray sources. We assume a distance of 68.4 Mpc for Hydra I in order to allow direct comparison with some (nearly) complete galaxy samples. The Centaurus cluster provides a valuable contrast to Virgo and Coma. It is intermediate in distance and in galaxy population type with a relatively well defined SO-dominated core and an extensive S-rich halo. Its richness class in the Abell scale is 1 or 2 which is richer than Virgo and poorer than Coma. -
The 6Df Galaxy Survey: Z ≈ 0 Measurements of the Growth Rate and Σ 8
Mon. Not. R. Astron. Soc. 423, 3430–3444 (2012) doi:10.1111/j.1365-2966.2012.21136.x The 6dF Galaxy Survey: z ≈ 0 measurements of the growth rate and σ 8 Florian Beutler,1 Chris Blake,2 Matthew Colless,3 D. Heath Jones,4 Lister Staveley-Smith,1,5 Gregory B. Poole,2 Lachlan Campbell,6 Quentin Parker,3,7 Will Saunders3 and Fred Watson3 1International Centre for Radio Astronomy Research (ICRAR), University of Western Australia, 35 Stirling Highway, Crawley, WA 6009, Australia 2Centre for Astrophysics & Supercomputing, Swinburne University of Technology, PO Box 218, Hawthorn, VIC 3122, Australia 3Australian Astronomical Observatory, PO Box 296, Epping, NSW 1710, Australia 4School of Physics, Monash University, Clayton, VIC 3800, Australia 5ARC Centre of Excellence for All-sky Astrophysics (CAASTRO), Australia 6Western Kentucky University, Bowling Green, KY 42101, USA 7Department of Physics and Astronomy, Faculty of Sciences, Macquarie University, NSW 2109, Sydney, Australia Accepted 2012 April 19. Received 2012 March 16; in original form 2011 November 14 ABSTRACT We present a detailed analysis of redshift-space distortions in the two-point correlation function of the 6dF Galaxy Survey (6dFGS). The K-band selected subsample which we employ in this 2 study contains 81 971 galaxies distributed over 17 000 degree with an effective redshift zeff = 0.067. By modelling the 2D galaxy correlation function, ξ(rp, π), we measure the parameter = ± γ combination f (zeff)σ 8(zeff) 0.423 0.055, where f m(z) is the growth rate of cosmic −1 structure and σ 8 is the rms of matter fluctuations in 8 h Mpc spheres. -
The Detection of the Imprint of Filaments on Cosmic Microwave Background Lensing
LETTERS https://doi.org/10.1038/s41550-018-0426-z The detection of the imprint of filaments on cosmic microwave background lensing Siyu He 1,2,3*, Shadab Alam4,5, Simone Ferraro6,7, Yen-Chi Chen8 and Shirley Ho1,2,3,6 Galaxy redshift surveys, such as the 2-Degree-Field Survey where n is the angular position, Πf(,nz ) is the angular posi- 1 2 (2dF) , Sloan Digital Sky Survey (SDSS) , 6-Degree-Field Survey tion of the closest point to n on the nearest filament and ρf (,nz ) 3 4 (6dF) , Galaxy And Mass Assembly survey (GAMA) and VIMOS is the uncertainty of the filament at Πf(,nz ). Using the inten- Public Extragalactic Redshift Survey (VIPERS)5, have shown that sity map at each redshift bin, we construct the filament intensity the spatial distribution of matter forms a rich web, known as the overdensity map via cosmic web6. Most galaxy survey analyses measure the ampli- tude of galaxy clustering as a function of scale, ignoring informa- In(,zz)d −Ī In(,zz)dΩ d tion beyond a small number of summary statistics. Because the ∫∫n δf()n = , Ī = , (2) matter density field becomes highly non-Gaussian as structure Ī ∫ dΩn evolves under gravity, we expect other statistical descriptions of the field to provide us with additional information. One way to study the non-Gaussianity is to study filaments, which evolve where Ωn is the solid angle at n. non-linearly from the initial density fluctuations produced in the In this work, we use the CMB lensing convergence map (pub- primordial Universe. -
UC Berkeley UC Berkeley Previously Published Works
UC Berkeley UC Berkeley Previously Published Works Title The DESI Experiment Part I: Science,Targeting, and Survey Design Permalink https://escholarship.org/uc/item/2nz5q3bt Authors Collaboration, DESI Aghamousa, Amir Aguilar, Jessica et al. Publication Date 2016-10-31 Peer reviewed eScholarship.org Powered by the California Digital Library University of California The DESI Experiment Part I: Science,Targeting, and Survey Design DESI Collaboration: Amir Aghamousa73, Jessica Aguilar76, Steve Ahlen85, Shadab Alam41;59, Lori E. Allen81, Carlos Allende Prieto64, James Annis52, Stephen Bailey76, Christophe Balland88, Otger Ballester57, Charles Baltay84, Lucas Beaufore45, Chris Bebek76, Timothy C. Beers39, Eric F. Bell28, Jos Luis Bernal66, Robert Besuner89, Florian Beutler62, Chris Blake15, Hannes Bleuler50, Michael Blomqvist2, Robert Blum81, Adam S. Bolton35;81, Cesar Briceno18, David Brooks33, Joel R. Brownstein35, Elizabeth Buckley-Geer52, Angela Burden9, Etienne Burtin12, Nicolas G. Busca7, Robert N. Cahn76, Yan-Chuan Cai59, Laia Cardiel-Sas57, Raymond G. Carlberg23, Pierre-Henri Carton12, Ricard Casas56, Francisco J. Castander56, Jorge L. Cervantes-Cota11, Todd M. Claybaugh76, Madeline Close14, Carl T. Coker26, Shaun Cole60, Johan Comparat67, Andrew P. Cooper60, M.-C. Cousinou4, Martin Crocce56, Jean-Gabriel Cuby2, Daniel P. Cunningham1, Tamara M. Davis86, Kyle S. Dawson35, Axel de la Macorra68, Juan De Vicente19, Timoth´eeDelubac74, Mark Derwent26, Arjun Dey81, Govinda Dhungana44, Zhejie Ding31, Peter Doel33, Yutong T. Duan85, Anne Ealet4, Jerry Edelstein89, Sarah Eftekharzadeh32, Daniel J. Eisenstein53, Ann Elliott45, St´ephanieEscoffier4, Matthew Evatt81, Parker Fagrelius76, Xiaohui Fan90, Kevin Fanning48, Arya Farahi40, Jay Farihi33, Ginevra Favole51;67, Yu Feng47, Enrique Fernandez57, Joseph R. Findlay32, Douglas P. Finkbeiner53, Michael J. Fitzpatrick81, Brenna Flaugher52, Samuel Flender8, Andreu Font-Ribera76, Jaime E. -
Measuring H0 from the 6Df Galaxy Survey and Future Low-Redshift Surveys
Advancing the Physics of Cosmic Distances Proceedings IAU Symposium No. 289, 2012 c 2012 International Astronomical Union Richard de Grijs & Giuseppe Bono, eds. DOI: 00.0000/X000000000000000X Measuring H0 from the 6dF Galaxy Survey and future low-redshift surveys Matthew Colless,1 Florian Beutler,2;3 and Chris Blake4 1Australian Astronomical Observatory, P. O. Box 915, North Ryde, NSW 1670, Australia email: [email protected] 2International Centre for Radio Astronomy Research, University of Western Australia, 35 Stirling Highway, Perth, WA 6009, Australia 3Lawrence Berkeley National Laboratory, 1 Cyclotron Road, Berkeley, CA 94720, USA email: [email protected] 4Centre for Astrophysics & Supercomputing, Swinburne University of Technology, P. O. Box 218, Hawthorn, VIC 3122, Australia email: [email protected] Abstract. Baryon acoustic oscillations (BAO) at low redshift provide a precise and largely model-independent way to measure the Hubble constant, H0. The 6dF Galaxy Survey measure- −1 −1 ment of the BAO scale gives a value of H0 = 67 ± 3:2 km s Mpc , achieving a 1σ precision of 5%. With improved analysis techniques, the planned wallaby (Hi) and taipan (optical) redshift surveys are predicted to measure H0 to 1{3% precision. Keywords. cosmology: observations, surveys, distance scale, large-scale structure of universe 1. Introduction Baryon acoustic oscillations (BAO) produced by the interaction of photons and baryons in the early universe provide an absolute standard rod that is calibrated by observations of the cosmic microwave background (CMB). The BAO scale is determined by well- understood linear physics and depends only on the physical densities of dark matter and baryons. -
The 6Df Galaxy Survey Is a Very Effective Means of Determining the True Mass Distribution in the Local Universe
**TITLE** ASP Conference Series, Vol. **VOLUME***, **YEAR OF PUBLICATION** **NAMES OF EDITORS** The 6dF Galaxy Survey Ken-ichi Wakamatsu Faculty of Engineering, Gifu University, Gifu 501-1192, Japan Matthew Colless Mount Stromlo & Siding Spring Observatories, ACT 2611, Australia Tom Jarrett IPAC, Caltech, MS 100-22, Pasadena, CA 91125, USA Quentin Parker Macquarie University, Sydney 2109, Australia William Saunders Anglo-Australian Observatory, Epping NSW 2121, Australia Fred Watson Anglo-Australian Observatory, Coonabarabran NSW 2357, Australia Abstract. The 6dF Galaxy Survey (6dFGS) 1 is a spectroscopic sur- vey of the entire southern sky with |b| > 10◦, based on the 2MASS near infrared galaxy catalog. It is conducted with the 6dF multi-fiber spec- trograph attached to the 1.2-m UK Schmidt Telescope. The survey will produce redshifts for some 170,000 galaxies, and peculiar velocities for about 15,000 and is expected to be complete by June 2005. arXiv:astro-ph/0306104v1 5 Jun 2003 1. Introduction In order to reveal large-scale structures at intermediate and large distances, ex- tensive galaxy redshift surveys have been carried out, e.g. the 2dFGRS and SDSS, and the Hubble- and Subaru-deep field surveys. There is now an ur- gent need to study the large-scale structure of the Local Universe that can be compared with the above deeper surveys. However to do this required hemi- 1Member of Science Advisory Group: M. Colless (Chair; ANU, Australia), J. Huchra (CfA, USA), T. Jarrett (IPAC, USA), O. Lahav (Cambridge, UK), J. Lucey (Dahram, UK), G. Mamon (IAP, France), Q. Parker (Maquarie Univ. Australia), D. Proust (Meudon, France), E. -
MACHINE LEARNING in GALAXY GROUPS DETECTION By
MACHINE LEARNING IN GALAXY GROUPS DETECTION by RAFEE TARIQ IBRAHEM A thesis submitted to The University of Birmingham for the degree of DOCTOR OF PHILOSOPHY School of Computer Science College of Engineering and Physical Sciences The University of Birmingham May 2017 University of Birmingham Research Archive e-theses repository This unpublished thesis/dissertation is copyright of the author and/or third parties. The intellectual property rights of the author or third parties in respect of this work are as defined by The Copyright Designs and Patents Act 1988 or as modified by any successor legislation. Any use made of information contained in this thesis/dissertation must be in accordance with that legislation and must be properly acknowledged. Further distribution or reproduction in any format is prohibited without the permission of the copyright holder. Abstract The detection of galaxy groups and clusters is of great importance in the field of astrophysics. In particular astrophysicists are interested in the evolution and formation of these systems, as well as the interactions that occur within galaxy groups and clusters. In this thesis, we developed a probabilistic model capa- ble of detecting galaxy groups and clusters based on the Hough transform. We called this approach probabilistic Hough transform based on adaptive local ker- nel (PHTALK). PHTALK was tested on a 3D realistic galaxy and mass assembly (GAMA) mock data catalogue (at close redshift z < 0:1)(mock data: contains information related to galaxies’ position, redshift and other properties). We com- pared the performance of our PHTALK method with the performance of two ver- sions of the standard friends-of-friends (FoF) method. -
Large Peculiar Velocities in the Hydra Centaurus Supercluster
LARGE PECULIAR VELOCITIES IN THE HYDRA CENTAURUS SUPERCLUSTER M. Aaronson1*, G.D. Bothun2, K.G. Budge3, JA. Dawe4, R.J. Dickens5, RJ. Hall6, J.R. Lucey7, J.R. Mould3, J.D. Murray6, R.A. Schommer8, A.E. Wright6. 1 Steward Observatory, University of Arizona 2 University of Michigan 3 California Institute of Technology 4 Australian National University 5Rutherford Appleton Laboratory 6 Australian National Radio Astronomy Observatory 7Anglo Australian Observatory 8 Rutgers University ABSTRACT Six clusters forming part of the Hydra-Cen Supercluster and its ex- tension on the opposite side of the galactic plane are under study at 21 cm with the Parkes radiotélescope. The infrared Tully-Fisher relation is used to determine the relative distances of the clusters. These clusters exhibit significant and generally positive peculiar velocities ranging from essentially zero for the Hydra cluster to as much as 1000 km/sec for the Pavo and Centaurus clusters. An upper limit of 500 km/sec was previously found in the study of clusters accessible from Arecibo. Data collection is not yet complete, however, and is further subject to unstud- ied systematic errors due to present reliance on photographic galaxy diameters. Nevertheless, these preliminary results support the notion of a large scale (and pre- sumably gravit at ionally) disturbed velocity field in the second and third quadrants of the supergalactic plane. 1. INTRODUCTION Comparison of the ratios of distances of galaxies with the ratios of their recession velocities allows one to learn something about the "noise" in the Hubble flow on various scales. One is subject to the limitation, however, that distance indicators are imprecise, and the 0.4 mag scatter in the infrared Tully-Fisher (IRTF) relation translates to an uncertainty of 1000 km/sec in an individual galaxy at cz = 5000 km/sec. -
Cosmological Constraints from Cosmic Shear
DES-2016-0211 FERMILAB-PUB-17-279-PPD Dark Energy Survey Year 1 Results: Cosmological Constraints from Cosmic Shear 1, 2, 1, 2 3 4, 5 6 7, 8 6, 9, 1, 10 M. A. Troxel, ⇤ N. MacCrann, J. Zuntz, T. F. Eifler, E. Krause, S. Dodelson, D. Gruen, † J. Blazek, O. Friedrich,11, 12 S. Samuroff,13 J. Prat,14 L. F. Secco,15 C. Davis,6 A. Ferte,´ 3 J. DeRose,16, 6 A. Alarcon,17 A. Amara,18 E. Baxter,15 M. R. Becker,16, 6 G. M. Bernstein,15 S. L. Bridle,13 R. Cawthon,8 C. Chang,8 A. Choi,1 J. De Vicente,19 A. Drlica-Wagner,7 J. Elvin-Poole,13 J. Frieman,7, 8 M. Gatti,14 W. G. Hartley,20, 18 K. Honscheid,1, 2 B. Hoyle,12 E. M. Huff,5 D. Huterer,21 B. Jain,15 M. Jarvis,15 T. Kacprzak,18 D. Kirk,20 N. Kokron,22, 23 C. Krawiec,15 O. Lahav,20 A. R. Liddle,3 J. Peacock,3 M. M. Rau,12 A. Refregier,18 R. P. Rollins,13 E. Rozo,24 E. S. Rykoff,6, 9 C. Sanchez,´ 14 I. Sevilla-Noarbe,19 E. Sheldon,25 A. Stebbins,7 T. N. Varga,11, 12 P. Vielzeuf,14 M. Wang,7 R. H. Wechsler,16, 6, 9 B. Yanny,7 T. M. C. Abbott,26 F. B. Abdalla,20, 27 S. Allam,7 J. Annis,7 K. Bechtol,28 A. Benoit-Levy,´ 29, 20, 30 E. Bertin,29, 30 D. Brooks,20 E. Buckley-Geer,7 D.