article Open AccessTop 1% cited <i>Planck</i>2015 results Astronomy and Astrophysics · 2016 · Vol. 594 · pp. A20–A20
P. A. R. Ade ✉ (Cardiff University) N. Aghanim (Université Paris-Sud) M. Arnaud (Centre National de la Recherche Scientifique) Frederico Arroja (National Taiwan University) M. Ashdown (University of Cambridge) J. Aumont (Université Paris-Sud) C. Baccigalupi (Scuola Internazionale Superiore di Studi Avanzati) M. Ballardini (Istituto Nazionale di Fisica Nucleare, Sezione di Bologna) A. J. Banday (Centre National de la Recherche Scientifique) R. B. Barreiro (Universidad de Cantabria) N. Bartolo (University of Padua) E. Battaner (Universidad de Granada) K. Benabed (Centre National de la Recherche Scientifique) A. Benoı̂t (Centre National de la Recherche Scientifique) A. Benoit-Lévy (Centre National de la Recherche Scientifique) J.-P. Bernard (Centre National de la Recherche Scientifique) M. Bersanelli (University of Milan) P. Bielewicz (Centre National de la Recherche Scientifique) J. J. Bock (California Institute of Technology) A. Bonaldi (University of Manchester) L. Bonavera (Universidad de Cantabria) J. R. Bond (University of Toronto) J. Borrill (Lawrence Berkeley National Laboratory) F. R. Bouchet (Centre National de la Recherche Scientifique) F. Boulanger (Université Paris-Sud) M. Bucher (Centre National de la Recherche Scientifique) C. Burigana (University of Ferrara) R. C. Butler (National Institute for Astrophysics) E. Calabrese (University of Oxford) J.-F. Cardoso (Télécom Paris) A. Catalano (Centre National de la Recherche Scientifique) A. Challinor (University of Cambridge) A. Chamballu (Université Paris-Sud) Ranga‐Ram Chary (California Institute of Technology) H. C. Chiang (Princeton University) P. R. Christensen (Niels Brock) S. Church (Stanford University) D. L. Clements (Imperial College London) S. Colombi (Centre National de la Recherche Scientifique) L. P. L. Colombo (University of Southern California) Céline Combet (Centre National de la Recherche Scientifique) D. Contreras (University of British Columbia) F. Couchot (Université Paris-Sud) A. Coulais (Centre National de la Recherche Scientifique) B. P. Crill (California Institute of Technology) A. Curto (Universidad de Cantabria) F. Cuttaia (National Institute for Astrophysics) L. Danese (Scuola Internazionale Superiore di Studi Avanzati) R. D. Davies (University of Manchester) Roger J. Davis (University of Manchester) P. de Bernardis (Sapienza University of Rome) A. de Rosa (National Institute for Astrophysics) G. de Zotti (Scuola Internazionale Superiore di Studi Avanzati) J. Delabrouille (Centre National de la Recherche Scientifique) F.–X. Désert (Centre National de la Recherche Scientifique) J. M. Diego (Universidad de Cantabria) H. Dole (Université Paris-Sud) S. Donzelli (National Institute for Astrophysics) O. Doré (California Institute of Technology) M. Douspis (Université Paris-Sud) A. Ducout (Centre National de la Recherche Scientifique) X. Dupac (European Space Astronomy Centre) G. Efstathiou (University of Cambridge) F. Elsner (Centre National de la Recherche Scientifique) T. A. Enßlin (Max Planck Institute for Astrophysics) H. K. Eriksen (University of Oslo) J. Fergusson (University of Cambridge) F. Finelli⋆ (Istituto Nazionale di Fisica Nucleare, Sezione di Bologna) O. Forni (Centre National de la Recherche Scientifique) M. Frailis (Trieste Astronomical Observatory) A. A. Fraisse (Princeton University) E. Franceschi (National Institute for Astrophysics) A. Frejsel A. Frolov (Simon Fraser University) S. Galeotta (Trieste Astronomical Observatory) S. Galli (University of Chicago) K. Ganga (Centre National de la Recherche Scientifique) C. Gauthier (Centre National de la Recherche Scientifique) M. Giard (Centre National de la Recherche Scientifique) Y. Giraud–Héraud (Centre National de la Recherche Scientifique) E. Gjerløw (University of Oslo) J. González-Nuevo (Universidad de Cantabria) K. M. Górski (Jet Propulsion Laboratory) S. Gratton (University of Cambridge) A. Gregorio (University of Trieste) A. Gruppuso (National Institute for Astrophysics) J. E. Gudmundsson (Nordic Institute for Theoretical Physics) J. Hamann (The University of Sydney) Will Handley (University of Cambridge) F. K. Hansen (University of Oslo) D. Hanson (Jet Propulsion Laboratory) D. L. Harrison (University of Cambridge) S. Henrot–Versillé (Université Paris-Sud) C. Hernández-Monteagudo (Max Planck Institute for Astrophysics) D. Herranz (Universidad de Cantabria) S. R. Hildebrandt (California Institute of Technology) E. Hivon (Centre National de la Recherche Scientifique) M. Hobson (University of Cambridge) W. A. Holmes (Jet Propulsion Laboratory) A. Hornstrup (Technical University of Denmark) W. Hovest (Max Planck Institute for Astrophysics) Zhiqi Huang (University of Toronto) K. M. Huffenberger (Florida State University) G. Hurier (Université Paris-Sud) A. H. Jaffe (Imperial College London) T. R. Jaffe (Centre National de la Recherche Scientifique) W. C. Jones (Princeton University) M. Juvela (University of Helsinki) E. Keihänen (University of Helsinki) R. Keskitalo (Lawrence Berkeley National Laboratory) J. Kim (Max Planck Institute for Astrophysics) T. S. Kisner (Lawrence Berkeley National Laboratory) R. Kneißl (Atacama Large Millimeter Submillimeter Array) J. Knoche (Max Planck Institute for Astrophysics) M. Kunz (Université Paris-Sud) H. Kurki‐Suonio (University of Helsinki) G. Lagache (Université Paris-Sud) A. Lähteenmäki (University of Helsinki) J.‐M. Lamarre (Centre National de la Recherche Scientifique) A. Lasenby (University of Cambridge) M. Lattanzi (University of Ferrara) C. R. Lawrence (Jet Propulsion Laboratory) R. Leonardi J. Lesgourgues (European Organization for Nuclear Research) F. Levrier (Centre National de la Recherche Scientifique) Antony Lewis (University of Sussex) M. Liguori (University of Padua) P. B. Lilje (University of Oslo) M. Linden-Vørnle (Technical University of Denmark) M. López-Caniego (Universidad de Cantabria) P. M. Lubin (University of California, Santa Barbara) Yin-Zhe Ma (University of British Columbia) J. F. Macías–Pérez (Centre National de la Recherche Scientifique) G. Maggio (Trieste Astronomical Observatory) D. Maino (University of Milan) N. Mandolesi (University of Ferrara) A. Mangilli (Université Paris-Sud) M. Maris (Trieste Astronomical Observatory) P. G. Martin (University of Toronto) E. Martínez-González (Universidad de Cantabria) S. Masi (Sapienza University of Rome) S. Matarrese (University of Padua) P. McGehee (California Institute of Technology) P. R. Meinhold (University of California, Santa Barbara) A. Melchiorri (Istituto Nazionale di Fisica Nucleare, Sezione di Roma I) L. Mendes (European Space Astronomy Centre) A. Mennella (University of Milan) M. Migliaccio (University of Cambridge) S. Mitra (Jet Propulsion Laboratory) M.-A. Miville-Deschênes (Université Paris-Sud) D. Molinari (Universidad de Cantabria) A. Moneti (Centre National de la Recherche Scientifique) L. Montier (Centre National de la Recherche Scientifique) G. Morgante (National Institute for Astrophysics) D. Mortlock (Imperial College London) A. Moss (University of Nottingham) Moritz Münchmeyer (Centre National de la Recherche Scientifique) D. Munshi (Cardiff University) J. A. Murphy (National University of Ireland, Maynooth) P. Naselsky F. Nati (Princeton University) P. Natoli (University of Ferrara) C. B. Netterfield (University of Toronto) H. U. Nørgaard-Nielsen (Technical University of Denmark) F. Noviello (University of Manchester) D. Novikov (Russian Academy of Sciences) I. Novikov (Russian Academy of Sciences) C. A. Oxborrow (Technical University of Denmark) F. Paci (Scuola Internazionale Superiore di Studi Avanzati) L. Pagano (Istituto Nazionale di Fisica Nucleare, Sezione di Roma I) François Pajot (Université Paris-Sud) R. Paladini (California Institute of Technology) Stefania Pandolfi (University of Copenhagen) D. Paoletti (Istituto Nazionale di Fisica Nucleare, Sezione di Bologna) F. Pasian (Trieste Astronomical Observatory) G. Patanchon (Centre National de la Recherche Scientifique) T. J. Pearson (California Institute of Technology) Hiranya V. Peiris (University College London) O. Perdereau (Université Paris-Sud) L. Perotto (Centre National de la Recherche Scientifique) F. Perrotta (Scuola Internazionale Superiore di Studi Avanzati) V. Pettorino (Heidelberg University) F. Piacentini (Sapienza University of Rome) M. Piat (Centre National de la Recherche Scientifique) E. Pierpaoli (University of Southern California) D. Pietrobon (Jet Propulsion Laboratory) S. Plaszczynski (Université Paris-Sud) É. Pointecouteau (Centre National de la Recherche Scientifique) G. Polenta (Astronomical Observatory of Rome) L. Popa (Institute of Space Science - INFLPR Subsidiary) G. W. Pratt (Centre National de la Recherche Scientifique) G. Prézeau (California Institute of Technology) S. Prunet (Centre National de la Recherche Scientifique) J.‐L. Puget (Université Paris-Sud) J. P. Rachen (Radboud University Nijmegen) W. T. Reach (Universities Space Research Association) R. Rébolo (Consejo Superior de Investigaciones Científicas) M. Reinecke (Max Planck Institute for Astrophysics) M. Remazeilles (Université Paris-Sud) C. Renault (Centre National de la Recherche Scientifique) A. Renzi (University of Rome Tor Vergata) I. Ristorcelli (Centre National de la Recherche Scientifique) G. Rocha (California Institute of Technology) C. Rosset (Centre National de la Recherche Scientifique) M. Rossetti (University of Milan) G. Roudier (Centre National de la Recherche Scientifique) M. Rowan-Robinson (Imperial College London) J. A. Rubiño-Martín (Universidad de La Laguna) B. Rusholme (California Institute of Technology) M. Sandri (National Institute for Astrophysics) D. Santos (Centre National de la Recherche Scientifique) М. Савелайнен (University of Helsinki) G. Savini (University College London) D. Scott (University of British Columbia) M. D. Seiffert (California Institute of Technology) E. P. S. Shellard (University of Cambridge) Maresuke Shiraishi (University of Padua) L. D. Spencer (Cardiff University) V. Stolyarov (Kazan Federal University) R. Stompor (Centre National de la Recherche Scientifique) R. Sudiwala (Cardiff University) R. Sunyaev (Space Research Institute) D. Sutton (University of Cambridge) A.-S. Suur-Uski (University of Helsinki) J.-F. Sygnet (Centre National de la Recherche Scientifique) J. A. Tauber (European Space Research and Technology Centre) L. Terenzi (Università degli Studi eCampus) L. Toffolatti (Universidad de Cantabria) M. Tomasi (University of Milan) M. Tristram (Université Paris-Sud) T. Trombetti (National Institute for Astrophysics) M. Tucci (University of Geneva) J. Tuovinen (Trinity College Dublin) L. Valenziano (National Institute for Astrophysics) J. Väliviita (University of Helsinki) B. Van Tent (Université Paris-Sud) P. Vielva (Universidad de Cantabria) F. Villa (National Institute for Astrophysics) L. A. Wade (Jet Propulsion Laboratory) B. D. Wandelt (Centre National de la Recherche Scientifique) I. K. Wehus (Jet Propulsion Laboratory) Martin White (University of California, Berkeley) D. Yvon (Commissariat à l'Énergie Atomique et aux Énergies Alternatives) A. Zacchei (Trieste Astronomical Observatory) J. P. Zibin (University of British Columbia) A. Zonca (University of California, Santa Barbara)
Abstract We present the implications for cosmic inflation of the Planck measurements of the cosmic microwave background (CMB) anisotropies in both temperature and polarization based on the full Planck survey, which includes more than twice the integration time of the nominal survey used for the 2013 release papers. The Planck full mission temperature data and a first release of polarization data on large angular scales measure the spectral index of curvature perturbations to be n s = 0.968 0.006 and tightly constrain its scale dependence to dn s /dln k = -0.003 0.007 when combined with the Planck lensing likelihood. When the Planck high-polarization data are included, the results are consistent and uncertainties are further reduced. The upper bound on the tensor-to-scalar ratio is r 0.002 < 0.11 (95% CL). This upper limit is consistent with the B-mode polarization constraint r < 0.12 (95% CL) obtained from a joint analysis of the BICEP2/Keck Array and Planck data. These results imply that V() 2 and natural inflation are now disfavoured compared to models predicting a smaller tensor-to-scalar ratio, such as R 2 inflation. We search for several physically motivated deviations from a simple power-law spectrum of curvature perturbations, including those motivated by a reconstruction of the inflaton potential not relying on the slow-roll approximation. We find that such models are not preferred, either according to a Bayesian model comparison or according to a frequentist simulation-based analysis. Three independent methods reconstructing the primordial power spectrum consistently recover a featureless and smooth P R (k) over the range of scales 0.008 Mpc -1 < k < 0.1 Mpc -1 . At large scales, each method finds deviations from a power law, connected to a deficit at multipoles 20-40 in the temperature power spectrum, but at an uncompelling statistical significance owing to the large cosmic variance present at these multipoles. By combining power spectrum and non-Gaussianity bounds, we constrain models with generalized Lagrangians, including Galileon models and axion monodromy models. The Planck data are consistent with adiabatic primordial perturbations, and the estimated values for the parameters of the base cold dark matter (CDM) model are not significantly altered when more general initial conditions are admitted. In correlated mixed adiabatic and isocurvature models, the 95% CL upper bound for the non-adiabatic contribution to the observed CMB temperature variance is | non-adi | < 1.9%, 4.0%, and 2.9% for CDM, neutrino density, and neutrino velocity isocurvature modes, respectively. We have tested inflationary models producing an anisotropic modulation of the primordial curvature power spectrum finding that the dipolar modulation in the CMB temperature field induced by a CDM isocurvature perturbation is not preferred at a statistically significant level. We also establish tight constraints on a possible quadrupolar modulation of the curvature perturbation. These results are consistent with the Planck 2013 analysis based on the nominal mission data and further constrain slow-roll single-field inflationary models, as expected from the increased precision of Planck data using the full set of observations.
Funding U.S. Department of Energy National Aeronautics and Space Administration UK Space Agency European Space Agency Science Foundation Ireland Partnership for Advanced Computing in Europe AISBL Centre National d’Etudes Spatiales Tekes Max-Planck-Gesellschaft China Scholarship Council Centre National de la Recherche Scientifique Ministério da Ciência, Tecnologia e Ensino Superior Office of Science Science and Technology Facilities Council Fundação para a Ciência e a Tecnologia Institut National de Physique Nucléaire et de Physique des Particules