DOCSLIB.ORG

XXIII. the Thermal Sunyaev-Zeldovich Effect-Cosmic Infrared Background Correlation

Total Page：16

File Type：pdf, Size：1020Kb

Download full-text PDF Read full-text
XXIII. the Thermal Sunyaev-Zeldovich Effect-Cosmic Infrared Background Correlation UC Santa Barbara UC Santa Barbara Previously Published Works Title Planck 2015 results: XXIII. The thermal Sunyaev-Zeldovich effect-cosmic infrared background correlation Permalink https://escholarship.org/uc/item/2wg9j8hm Authors Ade, PAR Aghanim, N Arnaud, M et al. Publication Date 2016-10-01 DOI 10.1051/0004-6361/201527418 Peer reviewed eScholarship.org Powered by the California Digital Library University of California Astronomy & Astrophysics manuscript no. powspec_szcib_ter c ESO 2015 September 23, 2015 Planck 2015 results. XXIII. The thermal Sunyaev-Zeldovich effect–cosmic infrared background correlation Planck Collaboration: P. A. R. Ade82, N. Aghanim57, M. Arnaud71, J. Aumont57, C. Baccigalupi81, A. J. Banday89;9, R. B. Barreiro62, J. G. Bartlett1;64, N. Bartolo27;63, E. Battaner90;91, K. Benabed58;88, A. Benoit-Lévy21;58;88, J.-P. Bernard89;9, M. Bersanelli30;47, P. Bielewicz78;9;81, J. J. Bock64;10, A. Bonaldi65, L. Bonavera62, J. R. Bond8, J. Borrill12;85, F. R. Bouchet58;83, C. Burigana46;28;48, R. C. Butler46, E. Calabrese87, A. Catalano72;70, A. Chamballu71;13;57, H. C. Chiang24;6, P. R. Christensen79;33, E. Churazov76;84, D. L. Clements54, L. P. L. Colombo20;64, C. Combet72, B. Comis72, F. Couchot69, A. Coulais70, B. P. Crill64;10, A. Curto62;5;67, F. Cuttaia46, L. Danese81, R. D. Davies65, R. J. Davis65, P. de Bernardis29, A. de Rosa46, G. de Zotti43;81, J. Delabrouille1, C. Dickinson65, J. M. Diego62, H. Dole57;56, S. Donzelli47, O. Doré64;10, M. Douspis57, A. Ducout58;54, X. Dupac35, G. Efstathiou59, F. Elsner21;58;88, T. A. Enßlin76, H. K. Eriksen60, F. Finelli46;48, I. Flores-Cacho9;89, O. Forni89;9, M. Frailis45, A. A. Fraisse24, E. Franceschi46, S. Galeotta45, S. Galli66, K. Ganga1, R. T. Génova-Santos61;16, M. Giard89;9, Y. Giraud-Héraud1, E. Gjerløw60, J. González-Nuevo17;62, K. M. Górski64;92, A. Gregorio31;45;51, A. Gruppuso46, J. E. Gudmundsson24, F. K. Hansen60, D. L. Harrison59;67, G. Helou10, C. Hernández-Monteagudo11;76, D. Herranz62, S. R. Hildebrandt64;10, E. Hivon58;88, M. Hobson5, A. Hornstrup14, W. Hovest76, K. M. Huffenberger22, G. Hurier57 ∗, A. H. Jaffe54, T. R. Jaffe89;9, W. C. Jones24, E. Keihänen23, R. Keskitalo12, T. S. Kisner74, R. Kneissl34;7, J. Knoche76, M. Kunz15;57;2, H. Kurki-Suonio23;41, G. Lagache4;57, J.-M. Lamarre70, M. Langer57, A. Lasenby5;67, M. Lattanzi28, C. R. Lawrence64, R. Leonardi35, F. Levrier70, P. B. Lilje60, M. Linden-Vørnle14, M. López-Caniego35;62, P. M. Lubin25, J. F. Macías-Pérez72, B. Maffei65, G. Maggio45, D. Maino30;47, D. S. Y. Mak59;67, N. Mandolesi46;28, A. Mangilli57;69, M. Maris45, P. G. Martin8, E. Martínez-González62, S. Masi29, S. Matarrese27;63;38, A. Melchiorri29;49, A. Mennella30;47, M. Migliaccio59;67, S. Mitra53;64, M.-A. Miville-Deschênes57;8, A. Moneti58, L. Montier89;9, G. Morgante46, D. Mortlock54, D. Munshi82, J. A. Murphy77, F. Nati24, P. Natoli28;3;46, F. Noviello65, D. Novikov75, I. Novikov79;75, C. A. Oxborrow14, F. Paci81, L. Pagano29;49, F. Pajot57, D. Paoletti46;48, B. Partridge40, F. Pasian45, T. J. Pearson10;55, O. Perdereau69, L. Perotto72, V. Pettorino39, F. Piacentini29, M. Piat1, E. Pierpaoli20, S. Plaszczynski69, E. Pointecouteau89;9, G. Polenta3;44, N. Ponthieu57;52, G. W. Pratt71, S. Prunet58;88, J.-L. Puget57, J. P. Rachen18;76, M. Reinecke76, M. Remazeilles65;57;1, C. Renault72, A. Renzi32;50, I. Ristorcelli89;9, G. Rocha64;10, C. Rosset1, M. Rossetti30;47, G. Roudier1;70;64, J. A. Rubiño-Martín61;16, B. Rusholme55, M. Sandri46, D. Santos72, M. Savelainen23;41, G. Savini80, D. Scott19, L. D. Spencer82, V. Stolyarov5;86;68, R. Stompor1, R. Sunyaev76;84, D. Sutton59;67, A.-S. Suur-Uski23;41, J.-F. Sygnet58, J. A. Tauber36, L. Terenzi37;46, L. Toffolatti17;62;46, M. Tomasi30;47, M. Tristram69, M. Tucci15, G. Umana42, L. Valenziano46, J. Valiviita23;41, B. Van Tent73, P. Vielva62, F. Villa46, L. A. Wade64, B. D. Wandelt58;88;26, I. K. Wehus64, N. Welikala87, D. Yvon13, A. Zacchei45, and A. Zonca25 (Affiliations can be found after the references) Preprint online version: September 23, 2015 Abstract We use Planck data to detect the cross-correlation between the thermal Sunyaev-Zeldovich (tSZ) effect and the infrared emission from the galaxies that make up the the cosmic infrared background (CIB). We first perform a stacking analysis towards Planck-confirmed galaxy clusters. We detect infrared emission produced by dusty galaxies inside these clusters and demonstrate that the infrared emission is about 50 % more extended than the +0:18 tSZ effect. Modelling the emission with a Navarro–Frenk–White profile, we find that the radial profile concentration parameter is c500 = 1:00−0:15. This indicates that infrared galaxies in the outskirts of clusters have higher infrared flux than cluster-core galaxies. We also study the cross- correlation between tSZ and CIB anisotropies, following three alternative approaches based on power spectrum analyses: (i) using a catalogue of confirmed clusters detected in Planck data; (ii) using an all-sky tSZ map built from Planck frequency maps; and (iii) using cross-spectra between Planck frequency maps. With the three different methods, we detect the tSZ-CIB cross-power spectrum at significance levels of (i) 6 σ, (ii) 3 σ, and (iii) 4 σ. We model the tSZ-CIB cross-correlation signature and compare predictions with the measurements. The amplitude of the cross-correlation relative to the fiducial model is AtSZ−CIB = 1:2 ± 0:3. This result is consistent with predictions for the tSZ-CIB cross-correlation assuming the best-fit cosmological model from Planck 2015 results along with the tSZ and CIB scaling relations. Key words. galaxies: clusters – infrared: galaxies – large-scale structure of Universe – methods: data analysis arXiv:1509.06555v1 [astro-ph.CO] 22 Sep 2015 1. Introduction tection of the cross-correlation between the thermal Sunyaev- Zeldovich (tSZ) effect (Sunyaev & Zeldovich 1969, 1972) and This paper is one of a set associated with the 2015 release of 1 the cosmic infrared background (CIB; Puget et al. 1996; Fixsen data from the Planck mission. It reports the first all-sky de- et al. 1998; Hauser et al. 1998). An increasing number of ob- ∗ Corresponding author: Guillaume Hurrier, [email protected] servational studies are measuring the tSZ effect and CIB fluctua- 1 Planck (http://www.esa.int/Planck) is a project of the tions at infrared and submillimetre wavelengths, including inves- European Space Agency (ESA) with instruments provided by two sci- tigations of the CIB with the Spitzer Space Telescope (Lagache entific consortia funded by ESA member states and led by Principal et al. 2007) and the Herschel Space Observatory (Amblard et al. Investigators from France and Italy, telescope reflectors provided 2011; Viero et al. 2012, 2015), and observations of the tSZ effect through a collaboration between ESA and a scientific consortium led with instruments such as the Atacama Pathfinder Experiment and funded by Denmark, and additional contributions from NASA (Halverson et al. 2009) and Bolocam (Sayers et al. 2011). In (USA). 2 Planck Collaboration: The tSZ–CIB cross-correlation addition, a new generation of CMB experiments can measure ing the tSZ signal from microwave data (e.g., Lieu et al. 2006; the tSZ effect and CIB at microwave frequencies (Hincks et al. Diego & Partridge 2009). 2010; Hall et al. 2010; Dunkley et al. 2011; Zwart et al. 2011; Recently, efforts have been made to model the tSZ-CIB cor- Reichardt et al. 2012; Planck Collaboration XXI 2014; Planck relation (e.g., Zahn et al. 2012; Addison et al. 2012). Using Collaboration XXX 2014). a halo model, it is possible to predict the tSZ-CIB cross- The large frequency coverage of Planck, from 30 to correlation. The halo model approach allows us to consider dis- 857 GHz, makes it sensitive to both of these important probes tinct astrophysical emission processes that trace the large-scale of large-scale structure. At intermediate frequencies, from 70 dark matter density fluctuation, but have different dependencies to 217 GHz, the sky emission is dominated by the cosmic mi- on the host halo mass and redshift. In this paper, we use mod- crowave background (CMB). At these frequencies, it is pos- els of the tSZ-CIB cross-correlation at galaxy cluster scales. We sible to detect galaxy clusters that produce a distortion of the note that the tSZ effect does not possess significant substructure CMB blackbody emission through the tSZ effect. At the angu- on the scale of galaxies, so the tSZ-CIB cross-correlation should lar resolution of Planck, this effect is mainly produced by lo- not possess a shot noise term. cal (z < 1) and massive galaxy clusters in dark matter halos Current experiments have already provided constraints on 14 the tSZ-CIB cross-correlation at low frequencies, between 100 (above 10 M ), and it has been used for several studies of clus- ter physics and cosmology (e.g., Planck Collaboration X 2011; and 250 GHz. The ACT collaboration set an upper limit ρ < 0:2 Planck Collaboration XI 2011; Planck Collaboration Int. III on the tSZ-CIB cross correlation (Dunkley et al. 2013). George 2013; Planck Collaboration Int. V 2013; Planck Collaboration et al.(2014), using SPT data and assuming a single correlation factor, obtained a tSZ-CIB correlation factor of 0:11+0:06; a zero Int. VIII 2013; Planck Collaboration Int. X 2013; Planck −0:05 Collaboration XX 2014; Planck Collaboration XXIV 2015; correlation is disfavoured at a confidence level of 99 %. Planck Collaboration XX 2014; Planck Collaboration XXIV Our objective in this paper is twofold. First, we characterize 2015). At frequencies above 353 GHz, the sky emission is the CIB emission toward tSZ-detected galaxy clusters by con- dominated by thermal emission, both Galactic and extragalac- straining the profile and redshift dependence of CIB emission tic (Planck Collaboration XI 2014; Planck Collaboration XXX from galaxy clusters.
Load more

Recommended publications
  • The Silk Damping Tail of the CMB
    The Silk Damping Tail of the CMB 100 K) µ ( T ∆ 10 10 100 1000 l Wayne Hu Oxford, December 2002 Outline • Damping tail of temperature power spectrum and its use as a standard ruler • Generation of polarization through damping • Unveiling of gravitational lensing from features in the damping tail Outline • Damping tail of temperature power spectrum and its use as a standard ruler • Generation of polarization through damping • Unveiling of gravitational lensing from features in the damping tail • Collaborators: Matt Hedman Takemi Okamoto Joe Silk Martin White Matias Zaldarriaga Outline • Damping tail of temperature power spectrum and its use as a standard ruler • Generation of polarization through damping • Unveiling of gravitational lensing from features in the damping tail • Collaborators: Matt Hedman Takemi Okamoto Joe Silk Microsoft Martin White Matias Zaldarriaga http://background.uchicago.edu ("Presentations" in PDF) Damping Tail Photon-Baryon Plasma • Before z~1000 when the CMB had T>3000K, hydrogen ionized • Free electrons act as "glue" between photons and baryons by Compton scattering and Coulomb interactions • Nearly perfect fluid Anisotropy Power Spectrum Damping • Perfect fluid: no anisotropic stresses due to scattering isotropization; baryons and photons move as single fluid Damping • Perfect fluid: no anisotropic stresses due to scattering isotropization; baryons and photons move as single fluid • Fluid imperfections are related to the mean free path of the photons in the baryons −1 λC = τ˙ where τ˙ = neσT a istheconformalopacitytoThomsonscattering
    [Show full text]
  • The Reionization of Cosmic Hydrogen by the First Galaxies Abstract 1
    David Goodstein’s Cosmology Book The Reionization of Cosmic Hydrogen by the First Galaxies Abraham Loeb Department of Astronomy, Harvard University, 60 Garden St., Cambridge MA, 02138 Abstract Cosmology is by now a mature experimental science. We are privileged to live at a time when the story of genesis (how the Universe started and developed) can be critically explored by direct observations. Looking deep into the Universe through powerful telescopes, we can see images of the Universe when it was younger because of the finite time it takes light to travel to us from distant sources. Existing data sets include an image of the Universe when it was 0.4 million years old (in the form of the cosmic microwave background), as well as images of individual galaxies when the Universe was older than a billion years. But there is a serious challenge: in between these two epochs was a period when the Universe was dark, stars had not yet formed, and the cosmic microwave background no longer traced the distribution of matter. And this is precisely the most interesting period, when the primordial soup evolved into the rich zoo of objects we now see. The observers are moving ahead along several fronts. The first involves the construction of large infrared telescopes on the ground and in space, that will provide us with new photos of the first galaxies. Current plans include ground-based telescopes which are 24-42 meter in diameter, and NASA’s successor to the Hubble Space Telescope, called the James Webb Space Telescope. In addition, several observational groups around the globe are constructing radio arrays that will be capable of mapping the three-dimensional distribution of cosmic hydrogen in the infant Universe.
    [Show full text]
  • Constraining Stochastic Gravitational Wave Background from Weak Lensing of CMB B-Modes
    Prepared for submission to JCAP Constraining stochastic gravitational wave background from weak lensing of CMB B-modes Shabbir Shaikh,y Suvodip Mukherjee,y Aditya Rotti,z and Tarun Souradeepy yInter University Centre for Astronomy and Astrophysics, Post Bag 4, Ganeshkhind, Pune- 411007, India zDepartment of Physics, Florida State University, Tallahassee, FL 32304, USA E-mail: [email protected], [email protected], [email protected], [email protected] Abstract. A stochastic gravitational wave background (SGWB) will affect the CMB anisotropies via weak lensing. Unlike weak lensing due to large scale structure which only deflects pho- ton trajectories, a SGWB has an additional effect of rotating the polarization vector along the trajectory. We study the relative importance of these two effects, deflection & rotation, specifically in the context of E-mode to B-mode power transfer caused by weak lensing due to SGWB. Using weak lensing distortion of the CMB as a probe, we derive constraints on the spectral energy density (ΩGW ) of the SGWB, sourced at different redshifts, without assuming any particular model for its origin. We present these bounds on ΩGW for different power-law models characterizing the SGWB, indicating the threshold above which observable imprints of SGWB must be present in CMB. arXiv:1606.08862v2 [astro-ph.CO] 20 Sep 2016 Contents 1 Introduction1 2 Weak lensing of CMB by gravitational waves2 3 Method 6 4 Results 8 5 Conclusion9 6 Acknowledgements 10 1 Introduction The Cosmic Microwave Background (CMB) is an exquisite tool to study the universe. It is being used to probe the early universe scenarios as well as the physics of processes happening in between the surface of last scattering and the observer.
    [Show full text]
  • Cosmic Microwave Background
    1 29. Cosmic Microwave Background 29. Cosmic Microwave Background Revised August 2019 by D. Scott (U. of British Columbia) and G.F. Smoot (HKUST; Paris U.; UC Berkeley; LBNL). 29.1 Introduction The energy content in electromagnetic radiation from beyond our Galaxy is dominated by the cosmic microwave background (CMB), discovered in 1965 [1]. The spectrum of the CMB is well described by a blackbody function with T = 2.7255 K. This spectral form is a main supporting pillar of the hot Big Bang model for the Universe. The lack of any observed deviations from a 7 blackbody spectrum constrains physical processes over cosmic history at redshifts z ∼< 10 (see earlier versions of this review). Currently the key CMB observable is the angular variation in temperature (or intensity) corre- lations, and to a growing extent polarization [2–4]. Since the first detection of these anisotropies by the Cosmic Background Explorer (COBE) satellite [5], there has been intense activity to map the sky at increasing levels of sensitivity and angular resolution by ground-based and balloon-borne measurements. These were joined in 2003 by the first results from NASA’s Wilkinson Microwave Anisotropy Probe (WMAP)[6], which were improved upon by analyses of data added every 2 years, culminating in the 9-year results [7]. In 2013 we had the first results [8] from the third generation CMB satellite, ESA’s Planck mission [9,10], which were enhanced by results from the 2015 Planck data release [11, 12], and then the final 2018 Planck data release [13, 14]. Additionally, CMB an- isotropies have been extended to smaller angular scales by ground-based experiments, particularly the Atacama Cosmology Telescope (ACT) [15] and the South Pole Telescope (SPT) [16].
    [Show full text]
  • Secondary Cosmic Microwave Background Anisotropies in A
    THE ASTROPHYSICAL JOURNAL, 508:435È439, 1998 December 1 ( 1998. The American Astronomical Society. All rights reserved. Printed in U.S.A. SECONDARY COSMIC MICROWAVE BACKGROUND ANISOTROPIES IN A UNIVERSE REIONIZED IN PATCHES ANDREIGRUZINOV AND WAYNE HU1 Institute for Advanced Study, School of Natural Sciences, Princeton, NJ 08540 Received 1998 March 17; accepted 1998 July 2 ABSTRACT In a universe reionized in patches, the Doppler e†ect from Thomson scattering o† free electrons gener- ates secondary cosmic microwave background (CMB) anisotropies. For a simple model with small patches and late reionization, we analytically calculate the anisotropy power spectrum. Patchy reioniza- tion can, in principle, be the main source of anisotropies on arcminute scales. On larger angular scales, its contribution to the CMB power spectrum is a small fraction of the primary signal and is only barely detectable in the power spectrum with even an ideal, i.e., cosmic variance limited, experiment and an extreme model of reionization. Consequently, patchy reionization is unlikely to a†ect cosmological parameter estimation from the acoustic peaks in the CMB. Its detection on small angles would help determine the ionization history of the universe, in particular, the typical size of the ionized region and the duration of the reionization process. Subject headings: cosmic microwave background È cosmology: theory È intergalactic medium È large-scale structure of universe 1. INTRODUCTION tion below the degree scale. Such e†ects rely on modulating the Doppler e†ect with spatial variations in the optical It is widely believed that the cosmic microwave back- depth. Incarnations of this general mechanism include the ground (CMB) will become the premier laboratory for the Vishniac e†ect from linear density variations (Vishniac study of the early universe and classical cosmology.
    [Show full text]
  • Observational Prospects I Have Cut This Lecture Back to Be Mostly About BAO Because I Still Have Holdover Topics from Previous Lectures to Cover
    Precision Cosmology with Large Scale Structure David Weinberg Precision Cosmology With Large Scale Structure David Weinberg, Ohio State University ICTP Cosmology Summer School 2015 Lecture 3: Observational Prospects I have cut this lecture back to be mostly about BAO because I still have holdover topics from previous lectures to cover. Where are we now? CMB Planck: All sky (40,000 deg2), near cosmic-variance limited for temperature anisotropy, noise lim- ited for polarization. ACT and SPT: Higher resolution experiments over smaller areas (hundreds or thousands of deg2), frequency coverage for Sunyaev-Zeldovich as well as primary anisotropy, polarization. Smaller area high-sensitivity experiments for B-mode polarization (e.g., BICEP). Type Ia Supernovae Data sets are compilations of surveys of different redshift ranges, local to z 1.2. ≈ “Compilation” requires enormous effort to bring different data sets to common calibration and analysis. Union 2.1, broad compilation. JLA – local samples, SDSS-II from z = 0.1 0.4, SNLS (Canada-France-Hawaii Telescope) from z = 0.4 1, HST at z > 1. − − Approaching 1000 SNe (740 for JLA). Optical imaging/weak lensing SDSS – 104 deg2, 5 bands (ugriz), depth r 22, weak lensing source density approximately − 1 arcmin 2; SDSS “Stripe 82” went 2 magnitudes≈ deeper over 200 deg2 Pan-STARRS – 3 104 deg2, depth comparable to SDSS × CFHTLens – 150 deg2, Dark Energy Survey (DES) is ongoing, discussed at the end. Redshift surveys SDSS-I/II: 106 galaxies, broadly selected, median z = 0.1 ; 105 luminous red galaxies (LRGs) sparsely sampling structure to z = 0.45 SDSS-III BOSS: 1.5 106 luminous galaxies, z = 0.2 0.7, 7 effective volume of SDSS-I/II LRGs; spectra of 160,000 quasars× at z = 2 4 for Lyα forest− analysis× − Clusters Variety of cluster catalogs selected by different methods.
    [Show full text]
  • Cosmology with Matter Diffusion
    Prepared for submission to JCAP Cosmology with matter diffusion Simone Calogeroa and Hermano Veltenb aMathematical Sciences, Chalmers University of Technology, Gothenburg University, S-412 96 Gothenburg, Sweden bUniversidade Federal do Esp´ırito Santo, Av. Fernando Ferrari, Goiabeiras, Vit´oria, Brasil E-mail: [email protected], [email protected] Abstract. We construct a viable cosmological model based on velocity diffusion of matter particles. In order to ensure the conservation of the total energy-momentum tensor in the presence of diffusion, we include a cosmological scalar field φ which we identify with the dark energy component of the universe. The model is characterized by only one new degree of freedom, the diffusion parameter σ. The standard ΛCDM model can be recovered by setting σ = 0. If diffusion takes place (σ > 0) the dynamics of the matter and of the dark energy fields are coupled. We argue that the existence of a diffusion mechanism in the universe may serve as a theoretical motivation for interacting models. We constrain the background dynamics of the diffusion model with Supernovae, H(z) and BAO data. We also perform a perturbative analysis of this model in order to understand structure formation in the universe. We calculate the impact of diffusion both on the CMB spectrum, with particular attention to the integrated Sachs-Wolfe signal, and on the matter power spectrum P (k). The latter analysis places strong constraints on the magnitude of the diffusion mechanism but does not rule out the model. Keywords: Cosmology, diffusion,
    [Show full text]
  • Nonparametric Inference for the Cosmic Microwave Background Christopher R
    Nonparametric Inference for the Cosmic Microwave Background Christopher R. Genovese,1 Christopher J. Miller,2 Robert C. Nichol,3 Mihir Arjunwadkar,4 and Larry Wasserman5 Carnegie Mellon University The Cosmic Microwave Background (CMB), which permeates the entire Universe, is the radiation left over from just 390,000 years after the Big Bang. On very large scales, the CMB radiation ¯eld is smooth and isotropic, but the existence of structure in the Universe { stars, galaxies, clusters of galaxies, ::: { suggests that the ¯eld should fluctuate on smaller scales. Recent observations, from the Cosmic Microwave Background Explorer to the Wilkin- son Microwave Anisotropy Project, have strikingly con¯rmed this prediction. CMB fluctuations provide clues to the Universe's structure and composition shortly after the Big Bang that are critical for testing cosmological models. For example, CMB data can be used to determine what portion of the Universe is composed of ordinary matter versus the mysterious dark matter and dark energy. To this end, cosmologists usually summarize the fluctuations by the power spectrum, which gives the variance as a function of angular frequency. The spectrum's shape, and in particular the location and height of its peaks, relates directly to the parameters in the cosmological models. Thus, a critical statistical question is how accurately can these peaks be estimated. We use recently developed techniques to construct a nonpara- metric con¯dence set for the unknown CMB spectrum. Our esti- mated spectrum, based on minimal assumptions, closely matches 1Research supported by NSF Grants SES 9866147 and NSF-ACI-0121671. 2Research supported by NSF-ACI-0121671.
    [Show full text]
  • Astro2020 Science White Paper Probing the Origin of Our Universe Through Cosmic Microwave Background Constraints on Gravitational Waves
    Astro2020 Science White Paper Probing the origin of our Universe through cosmic microwave background constraints on gravitational waves Thematic Areas: Planetary Systems Star and Planet Formation Formation and Evolution of Compact Objects X Cosmology and Fundamental Physics Stars and Stellar Evolution Resolved Stellar Populations and their Environments Galaxy Evolution Multi-Messenger Astronomy and Astrophysics Principal Author: Name: Sarah Shandera Institution: The Pennsylvania State University Email: [email protected] Phone: (814)863-9595 Co-authors: Peter Adshead (U. Illinois), Mustafa Amin (Rice University), Emanuela Dimastrogiovanni (University of New South Wales), Cora Dvorkin (Harvard University), Richard Easther (University of Auckland), Matteo Fasiello (Institute of Cosmology and Gravitation, University of Portsmouth), Raphael Flauger (University of California, San Diego), John T. Giblin, Jr (Kenyon College), Shaul Hanany (University of Minnesota), Lloyd Knox (Univerisity of California, Davis), Eugene Lim (King’s College London), Liam McAllister (Cornell University), Joel Meyers (Southern Methodist University), Marco Peloso (University of Padova, and INFN, Sezione di Padova), Graca Rocha (Jet Propulsion Laboratory), Maresuke Shiraishi (National Institute of Technology, Kagawa College), Lorenzo Sorbo (University of Massachusetts, Amherst), Scott Watson (Syracuse University) Endorsers: Zeeshan Ahmed1, David Alonso2, Robert Armstrong3, Mario Ballardini4, Darcy Barron5, Nicholas Battaglia6, Daniel Baumann7;8, Charles Bennett9,
    [Show full text]
  • Primordial Gravitational Waves from Cosmic Inflation
    Mathematical Tripos Part III Essay #75 (colour in electronic version) Submied 5th May 2017, updated 26th August 2017 Primordial Gravitational Waves from Cosmic Inflation Mike S. Wang DAMTP, University of Cambridge Abstract. Cosmic inflation generates primordial gravitational waves (PGWs) through the same physical process that seeds all structure formation in the observable universe. We will demonstrate this mechanism in detail and relate it to the distinctive signatures PGWs could leave in the observable temperature anisotropies and polarisation of the cosmic microwave background (CMB). The detection of primordial gravitational waves is of great significance to validating and understanding inflationary physics, and we shall see why CMB polarisation oers a promising path. In the end, we will remark on the unique observational challenges and prospects of probing primordial gravitational waves in future experiments. Keywords. Inflation, primordial gravitational waves (theory), gravitational waves and CMBR polarisation, power spectrum, gravitational waves / experiments. Contents I A Brief Overview 1 II The Inflation Paradigm and Generation of Gravitational Waves 1 II.1 Dynamics of single-field slow-roll inflation ...............................1 II.2 antum fluctuations and the primordial power spectrum ......................2 II.3 Scalar, vector and tensor perturbations in the FLRW background ...................3 III CMB Signatures from Primordial Gravitational Waves 5 III.1 Temperature anisotropies from PGWs ..................................5 III.2 Polarisation from PGWs ..........................................9 IV B-Mode Polarisation: A Promising Route for Detecting PGWs? 12 IV.1 Cosmological sources of B-mode polarisation .............................. 12 IV.2 Statistical aspects of B-mode polarisation ................................ 13 V A “Smoking Gun”: Physical Significance of PGW Discovery 14 V.1 Alternatives to inflation .........................................
    [Show full text]
  • The Cosmic Microwave Background Radiation Provided by CERN Document Server
    View metadata, citation and similar papers at core.ac.uk brought to you by CORE The Cosmic Microwave Background Radiation provided by CERN Document Server Eric Gawiser 1 Department of Physics, University of California, Berkeley, CA 94720 and Joseph Silk Department of Physics, Astrophysics, 1 Keble Road, University of Oxford, OX1 3NP, UK and Departments of Physics and Astronomy and Center for Particle Astrophysics, University of California, Berkeley, CA 94720 Abstract We summarize the theoretical and observational status of the study of the Cosmic Microwave Background radiation. Its thermodynamic spectrum is a robust prediction of the Hot Big Bang cosmology and has been confirmed observationally. There are now 76 observations of Cosmic Microwave Back- ground anisotropy, which we present in a table with references. We discuss the theoretical origins of these anisotropies and explain the standard jargon associated with their observation. 1 Origin of the Cosmic Background Radiation Our present understanding of the beginning of the universe is based upon the remarkably successful theory of the Hot Big Bang. We believe that our uni- verse began about 15 billion years ago as a hot, dense, nearly uniform sea of radiation a minute fraction of its present size (formally an infinitesimal sin- gularity). If inflation occurred in the first fraction of a second, the universe became matter dominated while expanding exponentially and then returned to radiation domination by the reheating caused by the decay of the inflaton. Baryonic matter formed within the first second, and the nucleosynthesis of the lightest elements took only a few minutes as the universe expanded and cooled.
    [Show full text]
  • Large-Scale Structure and Integrated Sachs–Wolfe Effect in Decaying Vacuum Cosmology
    MNRAS 452, 2220–2224 (2015) doi:10.1093/mnras/stv1443 Large-scale structure and integrated Sachs–Wolfe effect in decaying vacuum cosmology H. Velten,1,2‹ H. A. Borges,3,4 S. Carneiro,3‹ R. Fazolo1 and S. Gomes1 1Departamento de F´ısica, Universidade Federal do Esp´ırito Santo, 29075-910 Vitoria,´ ES, Brazil 2CPT, Aix Marseille Universite,´ UMR 7332, F-13288 Marseille, France 3Instituto de F´ısica, Universidade Federal da Bahia, 40210-340 Salvador, BA, Brazil 4Institute of Cosmology and Gravitation, University of Portsmouth, Portsmouth PO1 3FX, UK Accepted 2015 June 26. Received 2015 June 12; in original form 2015 April 17 ABSTRACT The concordance particle creation model – a class of (t) Cold Dark Matter (CDM) cosmolo- gies – is studied using large-scale structure (LSS) formation, with particular attention to the integrated Sachs–Wolfe effect. The evolution of the gravitational potential and the amplitude of the cross-correlation of the cosmic microwave background (CMB) signal with LSS sur- veys are calculated in detail. We properly include in our analysis the peculiarities involving the baryonic dynamics of the (t)CDM model which were not included in previous works. Although both the (t)CDM and the standard cosmology are in agreement with available data for the CMB–LSS correlation, the former presents a slightly higher signal which can be identified with future data. Key words: dark energy – dark matter. ˙ =− 1 INTRODUCTION from which it is not difficult to show that ρm. The back- ground expansion is given by Although the great success of the standard CDM cosmological = − + −3/2 model in describing most observations, we are still distant from H H0 1 m0 m0a , (2) the full understanding of the cosmic dynamics.
    [Show full text]