Author: "Frederico Arroja" - Searchworks@Jio Institute Digital Library Search Results

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1. Planck 2018 results

Author: Antony Lewis, X. Dupac, James R. Fergusson, François R. Bouchet, Diego Molinari, E. Martínez-González, Jean-François Cardoso, L. Salvati, Jörg P. Rachen, Krzysztof M. Gorski, K. Ganga, A. Marcos-Caballero, C. Combet, Hannu Kurki-Suonio, E. Di Valentino, Jose M. Diego, L. Montier, Jan Hamann, J. F. Macías-Pérez, E. Franceschi, Charles R. Lawrence, M. Douspis, Erminia Calabrese, E. P. S. Shellard, Frederico Arroja, M. Le Jeune, P. Vielva, Andrea Zacchei, Graca Rocha, Martina Gerbino, Zhiqi Huang, Davide Maino, Adam Moss, Ricardo Genova-Santos, D. Tavagnacco, M. López-Caniego, A. A. Fraisse, M. Tenti, F. Piacentini, J.-P. Bernard, P. de Bernardis, Tiziana Trombetti, L. Toffolatti, Soumen Basak, F. Elsner, J.-L. Puget, Benjamin D. Wandelt, Julian Borrill, R. B. Barreiro, Gabriel Jung, Michele Liguori, S. Galeotta, Will Handley, F. Cuttaia, G. Polenta, R. C. Butler, K. Kiiveri, Anthony Lasenby, Alessandro Melchiorri, Reijo Keskitalo, A. J. Banday, M.-A. Miville-Deschênes, A. Renzi, P. Bielewicz, F. Oppizzi, Yashar Akrami, Anthony Challinor, B. Casaponsa, E. Keihänen, Gianmarco Maggio, B. P. Crill, Nicola Bartolo, B. Van Tent, Fabrizio Villa, Francesca Perrotta, F. K. Hansen, J. B. Kim, G. Sirri, Andrei V. Frolov, Michele Maris, J. A. Tauber, M. Savelainen, D. Herranz, A.-S. Suur-Uski, Yabebal Fantaye, Sabino Matarrese, M. Migliaccio, M. Tomasi, M. Bucher, Nicola Vittorio, J. Valiviita, V. Lindholm, W. C. Jones, Douglas Scott, R. Fernandez-Cobos, D. Paoletti, Marco Bersanelli, Torsten A. Enßlin, A. Moneti, M. Frailis, Carlo Baccigalupi, V. Pettorino, François Levrier, E. Hivon, J. Aumont, B. Racine, A. Mennella, G. Patanchon, Alessandro Gruppuso, Ingunn Kathrine Wehus, M. Reinecke, J.-M. Delouis, P. D. Meerburg, Massimiliano Lattanzi, Jose Alberto Rubino-Martin, N. Mandolesi, Chiara Sirignano, Kendrick M. Smith, Andrew H. Jaffe, Peter Meinhold, J.-M. Lamarre, A. de Rosa, G. de Zotti, B. Partridge, J. González-Nuevo, A. Ducout, Locke D. Spencer, M. Ashdown, H. K. Eriksen, Martin Kunz, Mathieu Remazeilles, Jon E. Gudmundsson, L. P. L. Colombo, Jason D. McEwen, Mario Ballardini, Peter G. Martin, George Efstathiou, Serge Gratton, Carlo Burigana, Nicoletta Krachmalnicoff, Yin-Zhe Ma, Jacques Delabrouille, Fabio Finelli, L. Pagano, N. Mauri, S. Dusini, Andrea Zonca, R. A. Sunyaev, P. B. Lilje, Luca Stanco, H. C. Chiang, K. Benabed, J. R. Bond, B. Ruiz-Granados, O. Doré, Paolo Natoli, Maresuke Shiraishi, Moritz Münchmeyer, S. Galli, Gianluca Morgante, Astrophysique, Laboratoire de physique de l'ENS - ENS Paris (LPENS (UMR_8023)), École normale supérieure - Paris (ENS Paris), Université Paris sciences et lettres (PSL)-Université Paris sciences et lettres (PSL)-Sorbonne Université (SU)-Centre National de la Recherche Scientifique (CNRS)-Université de Paris (UP)-École normale supérieure - Paris (ENS Paris), Université Paris sciences et lettres (PSL)-Université Paris sciences et lettres (PSL)-Sorbonne Université (SU)-Centre National de la Recherche Scientifique (CNRS)-Université de Paris (UP), Institut de recherche en astrophysique et planétologie (IRAP), Institut national des sciences de l'Univers (INSU - CNRS)-Université Toulouse III - Paul Sabatier (UT3), Université Fédérale Toulouse Midi-Pyrénées-Université Fédérale Toulouse Midi-Pyrénées-Observatoire Midi-Pyrénées (OMP), Météo France-Centre National d'Études Spatiales [Toulouse] (CNES)-Université Fédérale Toulouse Midi-Pyrénées-Centre National de la Recherche Scientifique (CNRS)-Institut de Recherche pour le Développement (IRD)-Météo France-Centre National d'Études Spatiales [Toulouse] (CNES)-Centre National de la Recherche Scientifique (CNRS)-Institut de Recherche pour le Développement (IRD)-Centre National de la Recherche Scientifique (CNRS), Institut d'Astrophysique de Paris (IAP), Institut national des sciences de l'Univers (INSU - CNRS)-Sorbonne Université (SU)-Centre National de la Recherche Scientifique (CNRS), University of Parma = Università degli studi di Parma [Parme, Italie], Canadian Institute for Theoretical Astrophysics (CITA), Lawrence Berkeley National Laboratory [Berkeley] (LBNL), Patrimoine, Littérature, Histoire (PLH), Université Toulouse - Jean Jaurès (UT2J), AstroParticule et Cosmologie (APC (UMR_7164)), Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Observatoire de Paris, Université Paris sciences et lettres (PSL)-Université Paris sciences et lettres (PSL)-Centre National de la Recherche Scientifique (CNRS)-Université de Paris (UP), Universidade Aberta [Lisboa], Laboratoire de Physique Subatomique et de Cosmologie (LPSC), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS)-Université Grenoble Alpes (UGA)-Institut polytechnique de Grenoble - Grenoble Institute of Technology (Grenoble INP ), Université Grenoble Alpes (UGA), Dipartimento di Fisica [Roma La Sapienza], Università degli Studi di Roma 'La Sapienza' = Sapienza University [Rome], Jet Propulsion Laboratory (JPL), NASA-California Institute of Technology (CALTECH), Institut d'astrophysique spatiale (IAS), Université Paris-Sud - Paris 11 (UP11)-Institut national des sciences de l'Univers (INSU - CNRS)-Centre National de la Recherche Scientifique (CNRS), Centre National de la Recherche Scientifique (CNRS)-Institut national des sciences de l'Univers (INSU - CNRS)-Université Pierre et Marie Curie - Paris 6 (UPMC), Laboratory for Phytosanitary Diagnostics and Forecasts, All-Russian Institute for Plant Protection, Russian Academy of Sciences [Moscow] (RAS), Institut National Polytechnique (Toulouse) (Toulouse INP), Université Fédérale Toulouse Midi-Pyrénées, Department of Atmospheric, Oceanic, and Space Sciences [Ann Arbor] (AOSS), University of Michigan [Ann Arbor], University of Michigan System-University of Michigan System, Laboratoire d'Etude du Rayonnement et de la Matière en Astrophysique (LERMA (UMR_8112)), Sorbonne Université (SU)-Institut national des sciences de l'Univers (INSU - CNRS)-Centre National de la Recherche Scientifique (CNRS)-Université de Cergy Pontoise (UCP), Université Paris-Seine-Université Paris-Seine-Observatoire de Paris, Université Paris sciences et lettres (PSL)-Université Paris sciences et lettres (PSL), ICRA and Physics Department, Dipartimento di Fisica 'G. Galilei', Universita degli Studi di Padova, University of Cambridge [UK] (CAM), Commissariat à l'énergie atomique et aux énergies alternatives (CEA), Laboratoire de Physique Nucléaire et de Hautes Énergies (LPNHE), Centre National de la Recherche Scientifique (CNRS)-Université Paris Diderot - Paris 7 (UPD7)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Pierre et Marie Curie - Paris 6 (UPMC), Astrophysique Interprétation Modélisation (AIM (UMR_7158 / UMR_E_9005 / UM_112)), Centre National de la Recherche Scientifique (CNRS)-Institut national des sciences de l'Univers (INSU - CNRS)-Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris Diderot - Paris 7 (UPD7), Commissariat à l'énergie atomique et aux énergies alternatives - Laboratoire d'Electronique et de Technologie de l'Information (CEA-LETI), Direction de Recherche Technologique (CEA) (DRT (CEA)), Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Commissariat à l'énergie atomique et aux énergies alternatives (CEA), University of Manchester [Manchester], University of British Columbia (UBC), Laboratoire de neurobiologie cellulaire et moléculaire (NBCM), Centre National de la Recherche Scientifique (CNRS), Laboratoire de Physique des 2 Infinis Irène Joliot-Curie (IJCLab), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Paris-Saclay-Centre National de la Recherche Scientifique (CNRS), Planck Collaboration, Université Paris sciences et lettres (PSL)-Université Paris sciences et lettres (PSL)-Centre National de la Recherche Scientifique (CNRS)-Sorbonne Université (SU)-Université Paris Diderot - 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CNRS)-Observatoire Midi-Pyrénées (OMP), Institut de Recherche pour le Développement (IRD)-Université Toulouse III - Paul Sabatier (UT3), Université de Toulouse (UT)-Université de Toulouse (UT)-Institut national des sciences de l'Univers (INSU - CNRS)-Centre National d'Études Spatiales [Toulouse] (CNES)-Centre National de la Recherche Scientifique (CNRS)-Météo-France -Institut de Recherche pour le Développement (IRD)-Institut national des sciences de l'Univers (INSU - CNRS)-Centre National d'Études Spatiales [Toulouse] (CNES)-Centre National de la Recherche Scientifique (CNRS)-Météo-France -Centre National de la Recherche Scientifique (CNRS), Università degli studi di Parma = University of Parma (UNIPR), Université de Toulouse (UT)-Université de Toulouse (UT), Université Paris sciences et lettres (PSL)-Université Paris sciences et lettres (PSL)-Centre National de la Recherche Scientifique (CNRS)-Université Paris Cité (UPCité), Università degli Studi di Roma 'La Sapienza' = Sapienza University [Rome] (UNIROMA), Université Paris-Sud - 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Akrami, F. Arroja, M. Ashdown, J. Aumont, C. Baccigalupi, M. Ballardini, A. J. Banday, R. B. Barreiro, N. Bartolo, S. Basak, K. Benabed, J. -P. Bernard, M. Bersanelli, P. Bielewicz, J. R. Bond, J. Borrill, F. R. Bouchet, M. Bucher, C. Burigana, R. C. Butler, E. Calabrese, J. -F. Cardoso, B. Casaponsa, A. Challinor, H. C. Chiang, L. P. L. Colombo, C. Combet, B. P. Crill, F. Cuttaia, P. de Bernardi, A. de Rosa, G. de Zotti, J. Delabrouille, J. -M. Deloui, E. Di Valentino, J. M. Diego, O. Doré, M. Douspi, A. Ducout, X. Dupac, S. Dusini, G. Efstathiou, F. Elsner, T. A. Enßlin, H. K. Eriksen, Y. Fantaye, J. Fergusson, R. Fernandez-Cobo, F. Finelli, M. Fraili, A. A. Fraisse, E. Franceschi, A. Frolov, S. Galeotta, K. Ganga, R. T. Génova-Santo, M. Gerbino, J. González-Nuevo, K. M. Górski, S. Gratton, A. Gruppuso, J. E. Gudmundsson, J. Hamann, W. Handley, F. K. Hansen, D. Herranz, E. Hivon, Z. Huang, A. H. Jaffe, W. C. Jone, G. Jung, E. Keihänen, R. Keskitalo, K. Kiiveri, J. Kim, N. Krachmalnicoff, M. Kunz, H. Kurki-Suonio, J. -M. Lamarre, A. Lasenby, M. Lattanzi, C. R. Lawrence, M. Le Jeune, F. Levrier, A. Lewi, M. Liguori, P. B. Lilje, V. Lindholm, M. López-Caniego, Y. -Z. Ma, J. F. Macías-Pérez, G. Maggio, D. Maino, N. Mandolesi, A. Marcos-Caballero, M. Mari, P. G. Martin, E. Martínez-González, S. Matarrese, N. Mauri, J. D. McEwen, P. D. Meerburg, P. R. Meinhold, A. Melchiorri, A. Mennella, M. Migliaccio, M. -A. Miville-Deschêne, D. Molinari, A. Moneti, L. Montier, G. Morgante, A. Mo, M. Münchmeyer, P. Natoli, F. Oppizzi, L. Pagano, D. Paoletti, B. Partridge, G. Patanchon, F. Perrotta, V. Pettorino, F. Piacentini, G. Polenta, J. -L. Puget, J. P. Rachen, B. Racine, M. Reinecke, M. Remazeille, A. Renzi, G. Rocha, J. A. Rubiño-Martín, B. Ruiz-Granado, L. Salvati, M. Savelainen, D. Scott, E. P. S. Shellard, M. Shiraishi, C. Sirignano, G. Sirri, K. Smith, L. D. Spencer, L. Stanco, R. Sunyaev, A. -S. Suur-Uski, J. A. Tauber, D. Tavagnacco, M. Tenti, L. Toffolatti, M. Tomasi, T. Trombetti, J. Valiviita, B. Van Tent, P. Vielva, F. Villa, N. Vittorio, B. D. Wandelt, I. K. Wehu, A. Zacchei, A. Zonca, Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS)-Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Observatoire de Paris, and PSL Research University (PSL)-PSL Research University (PSL)-Université Paris Diderot - Paris 7 (UPD7)
Subjects: High Energy Physics - Theory, cosmological model, Astronomy, Cosmic microwave background, POLARIZATION ANISOTROPIES, cosmic background radiation: polarization, Astrophysics, cosmic background radiation, Cosmic background radiation, Early Universe, 01 natural sciences, 7. Clean energy, expansion: multipole, General Relativity and Quantum Cosmology, High Energy Physics - Phenomenology (hep-ph), cosmology: theory, 3-POINT CORRELATION-FUNCTION, observations [Cosmology], data analysis [Methods], 010303 astronomy & astrophysics, TEMPERATURE, Physics, [PHYS.HTHE]Physics [physics]/High Energy Physics - Theory [hep-th], hep-th, formation, hep-ph, early Universe, CMB cold spot, inflation: model, High Energy Physics - Phenomenology, scale dependence, non-Gaussianity, symbols, Sunyaev-Zel'dovich effect, [PHYS.GRQC]Physics [physics]/General Relativity and Quantum Cosmology [gr-qc], astro-ph.CO, Trispectrum, Astrophysics - Cosmology and Nongalactic Astrophysics, Particle physics, data analysis method, Cosmology and Nongalactic Astrophysics (astro-ph.CO), satellite: Planck, gr-qc, FOS: Physical sciences, PREDICTIONS, General Relativity and Quantum Cosmology (gr-qc), Astrophysics::Cosmology and Extragalactic Astrophysics, Sunyaev–Zel'dovich effect, Separable space, NO, isocurvature, symbols.namesake, trispectrum, Settore FIS/05 - Astronomia e Astrofisica, parity: violation, gravitation: lens, statistical analysis, theory [Cosmology], Non-Gaussianity, 0103 physical sciences, BISPECTRUM, INFRARED BACKGROUND ANISOTROPIES, structure, bispectrum: scale dependence, Planck, cosmic background radiation: bispectrum, inflation, FAST ESTIMATOR, numerical calculations, non-Gaussianity: primordial, 010308 nuclear & particles physics, ISOCURVATURE PERTURBATIONS, Astronomy and Astrophysics, stability, 115 Astronomy, Space science, Inflation, methods: data analysis, boundary condition, cosmic background radiation: temperature, Cosmology: observations, Cosmology: theory, Methods: data analysis, High Energy Physics - Theory (hep-th), 13. Climate action, Space and Planetary Science, axion, [PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph], cosmology: observations, Cosmic background radiation, Cosmology: observations, Cosmology: theory, Early Universe, Inflation, Methods: data analysis, [PHYS.ASTR]Physics [physics]/Astrophysics [astro-ph], Bispectrum
Abstract: Planck Collaboration: et al., arXiv:1905.05697v1, We analyse the Planck full-mission cosmic microwave background (CMB) temperature and E-mode polarization maps to obtain constraints on primordial non-Gaussianity (NG). We compare estimates obtained from separable template-fitting, binned, and optimal modal bispectrum estimators, finding consistent values for the local, equilateral, and orthogonal bispectrum amplitudes. Our combined temperature and polarization analysis produces the following final results: fNLlocal = −0.9 ± 5.1; fNLequil = −26 ± 47; and fNLortho = −38 ± 24 (68% CL, statistical). These results include low-multipole (4 ≤ ℓ < 40) polarization data that are not included in our previous analysis. The results also pass an extensive battery of tests (with additional tests regarding foreground residuals compared to 2015), and they are stable with respect to our 2015 measurements (with small fluctuations, at the level of a fraction of a standard deviation, which is consistent with changes in data processing). Polarization-only bispectra display a significant improvement in robustness; they can now be used independently to set primordial NG constraints with a sensitivity comparable to WMAP temperature-based results and they give excellent agreement. In addition to the analysis of the standard local, equilateral, and orthogonal bispectrum shapes, we consider a large number of additional cases, such as scale-dependent feature and resonance bispectra, isocurvature primordial NG, and parity-breaking models, where we also place tight constraints but do not detect any signal. The non-primordial lensing bispectrum is, however, detected with an improved significance compared to 2015, excluding the null hypothesis at 3.5σ. Beyond estimates of individual shape amplitudes, we also present model-independent reconstructions and analyses of the Planck CMB bispectrum. Our final constraint on the local primordial trispectrum shape is gNLlocal = (−5.8 ± 6.5) × 104 (68% CL, statistical), while constraints for other trispectrum shapes are also determined. Exploiting the tight limits on various bispectrum and trispectrum shapes, we constrain the parameter space of different early-Universe scenarios that generate primordial NG, including general single-field models of inflation, multi-field models (e.g. curvaton models), models of inflation with axion fields producing parity-violation bispectra in the tensor sector, and inflationary models involving vector-like fields with directionally-dependent bispectra. Our results provide a high-precision test for structure-formation scenarios, showing complete agreement with the basic picture of the ΛCDM cosmology regarding the statistics of the initial conditions, with cosmic structures arising from adiabatic, passive, Gaussian, and primordial seed perturbations., The Planck Collaboration acknowledges the support of: ESA; CNES and CNRS/INSU-IN2P3-INP (France); ASI, CNR, and INAF (Italy); NASA and DoE (USA); STFC and UKSA (UK); CSIC, MINECO, JA, and RES (Spain); Tekes, AoF, and CSC (Finland); DLR and MPG (Germany); CSA (Canada); DTU Space (Denmark); SER/SSO (Switzerland); RCN (Norway); SFI (Ireland); FCT/MCTES (Portugal); and ERC and PRACE (EU).
Published: 2020
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2. Exploring cosmic origins with CORE: cosmological parameters

Author: Daniela Paoletti, Nicola Bartolo, Jens Chluba, J. Greenslade, P. Vielva, Mattia Negrello, Karl Young, Matteo Bonato, Andrea Tartari, Alessandro Paiella, Alessandro Coppolecchia, Andrea Caputo, Nicola Vittorio, V. Lindholm, Anthony Challinor, Agnieszka Pollo, Francois Boulanger, Luca Lamagna, Simone Ferraro, Martin Crook, D. McCarthy, M. López-Caniego, Ted Kisner, G. de Gasperis, L. Polastri, Alessandro Melchiorri, Josquin Errard, Rien van de Weygaert, D. Tramonte, Jose Alberto Rubino-Martin, C. J. A. P. Martins, Deanna C. Hooper, Matthieu Roman, Gianfranco De Zotti, Neil Trappe, M. Piat, Daniel Baumann, Gianluca Polenta, Jussi Valiviita, M. Tomasi, Paolo de Bernardis, Christophe Ringeval, Marco De Petris, Marco Bersanelli, Mario Zannoni, Giuseppe D'Alessandro, R. Fernandez-Cobos, Julien Lesgourgues, Paolo Natoli, Laura Salvati, Miguel Quartin, Thomas Kitching, R. Allison, Antony Lewis, K. Kiiveri, Carole Tucker, Diego Molinari, M. Kunz, Joseph J. Mohr, Ricardo Genova-Santos, C. Hervias-Caimapo, Jean-Baptiste Melin, Sebastian Grandis, Sylvain Martin, Michele Liguori, Shaul Hanany, Mario Ballardini, Vincent Vennin, Eleonora Di Valentino, Enrique Martinez-Gonzalez, Jose M. Diego, Giovanni Cabass, Hannu Kurki-Suonio, Jacques Delabrouille, J. González-Nuevo, Anthony Lasenby, F. Piacentini, Jochem J. A. Baselmans, Gemma Luzzi, S. Hagstotz, Tiziana Trombetti, Stephen M. Feeney, Alessio Notari, C. S. Carvalho, Fabio Finelli, Simone Paradiso, Silvia Masi, James G. Bartlett, Carlos Hernández-Monteagudo, Massimiliano Lattanzi, A. J. Banday, Thejs Brinckmann, Cora Dvorkin, Eric Hivon, Sebastien Clesse, Alessandro Buzzelli, Vivian Poulin, Ana Achúcarro, Martina Gerbino, M. Ashdown, A. Bonaldi, Luca Pagano, Julian Borrill, Will Handley, Martino Calvo, R. Banerji, Ivan Charles, Alessandro Monfardini, Frederico Arroja, S. Basak, Mathieu Remazeilles, Giampaolo Pisano, I. Colantoni, Silvia Galli, Gérard Vermeulen, Francesco Forastieri, Elena Giusarma, Dhiraj Kumar Hazra, François R. Bouchet, Zhen-Yi Cai, Carlo Burigana, G. Castellano, Peter A. R. Ade, Matthew Hills, Bruno Maffei, Martin Bucher, Bartjan van Tent, Guillaume Patanchon, Helsinki Institute of Physics, Department of Physics, String Theory (ITFA, IoP, FNWI), Astronomy, Institut d'Astrophysique de Paris ( IAP ), Université Pierre et Marie Curie - Paris 6 ( UPMC ) -Institut national des sciences de l'Univers ( INSU - CNRS ) -Centre National de la Recherche Scientifique ( CNRS ), Institut Lagrange de Paris, Sorbonne Universités, Laboratoire d'Annecy-le-Vieux de Physique Théorique ( LAPTH ), Université Savoie Mont Blanc ( USMB [Université de Savoie] [Université de Chambéry] ) -Centre National de la Recherche Scientifique ( CNRS ), AstroParticule et Cosmologie ( APC - UMR 7164 ), Centre National de la Recherche Scientifique ( CNRS ) -Institut National de Physique Nucléaire et de Physique des Particules du CNRS ( IN2P3 ) -Observatoire de Paris-Université Paris Diderot - Paris 7 ( UPD7 ) -Commissariat à l'énergie atomique et aux énergies alternatives ( CEA ), Institut d'astrophysique spatiale ( IAS ), Université Paris-Sud - Paris 11 ( UP11 ) -Institut national des sciences de l'Univers ( INSU - CNRS ) -Centre National de la Recherche Scientifique ( CNRS ), Institut de recherche en astrophysique et planétologie ( IRAP ), Université Paul Sabatier - Toulouse 3 ( UPS ) -Observatoire Midi-Pyrénées ( OMP ) -Centre National de la Recherche Scientifique ( CNRS ), Département de Recherche Fondamentale sur la Matière Condensée ( DRFMC ), Commissariat à l'énergie atomique et aux énergies alternatives ( CEA ), Département de Physique des Particules (ex SPP) ( DPP ), Institut de Recherches sur les lois Fondamentales de l'Univers ( IRFU ), Commissariat à l'énergie atomique et aux énergies alternatives ( CEA ) -Université Paris-Saclay-Commissariat à l'énergie atomique et aux énergies alternatives ( CEA ) -Université Paris-Saclay, Institut Néel ( NEEL ), Université Grenoble Alpes [Saint Martin d'Hères]-Centre National de la Recherche Scientifique ( CNRS ), Laboratoire de Physique Nucléaire et de Hautes Énergies ( LPNHE ), Université Pierre et Marie Curie - Paris 6 ( UPMC ) -Institut National de Physique Nucléaire et de Physique des Particules du CNRS ( IN2P3 ) -Université Paris Diderot - Paris 7 ( UPD7 ) -Centre National de la Recherche Scientifique ( CNRS ), Laboratoire de Physique Théorique d'Orsay [Orsay] ( LPT ), Université Paris-Sud - Paris 11 ( UP11 ) -Centre National de la Recherche Scientifique ( CNRS ), CORE, Di Valentino, E, Brinckmann, T, Gerbino, M, Poulin, V, Bouchet, F, Lesgourgues, J, Melchiorri, A, Chluba, J, Clesse, S, Delabrouille, J, Dvorkin, C, Forastieri, F, Galli, S, Hooper, D, Lattanzi, M, Martins, C, Salvati, L, Cabass, G, Caputo, A, Giusarma, E, Hivon, E, Natoli, P, Pagano, L, Paradiso, S, Rubiño-Martin, J, Achúcarro, A, Ade, P, Allison, R, Arroja, F, Ashdown, M, Ballardini, M, Banday, A, Banerji, R, Bartolo, N, Bartlett, J, Basak, S, Baumann, D, de Bernardis, P, Bersanelli, M, Bonaldi, A, Bonato, M, Borrill, J, Boulanger, F, Bucher, M, Burigana, C, Buzzelli, A, Cai, Z, Calvo, M, Carvalho, C, Castellano, G, Challinor, A, Charles, I, Colantoni, I, Coppolecchia, A, Crook, M, D'Alessandro, G, De Petris, M, De Zotti, G, Diego, J, Errard, J, Feeney, S, Fernandez-Cobos, R, Ferraro, S, Finelli, F, de Gasperis, G, Génova-Santos, R, González-Nuevo, J, Grandis, S, Greenslade, J, Hagstotz, S, Hanany, S, Handley, W, Hazra, D, Hernández-Monteagudo, C, Hervias-Caimapo, C, Hills, M, Kiiveri, K, Kisner, T, Kitching, T, Kunz, M, Kurki-Suonio, H, Lamagna, L, Lasenby, A, Lewis, A, Liguori, M, Lindholm, V, Lopez-Caniego, M, Luzzi, G, Maffei, B, Martin, S, Martinez-Gonzalez, E, Masi, S, Matarrese, S, Mccarthy, D, Melin, J, Mohr, J, Molinari, D, Monfardini, A, Negrello, M, Notari, A, Paiella, A, Paoletti, D, Patanchon, G, Piacentini, F, Piat, M, Pisano, G, Polastri, L, Polenta, G, Pollo, A, Quartin, M, Remazeilles, M, Roman, M, Ringeval, C, Tartari, A, Tomasi, M, Tramonte, D, Trappe, N, Trombetti, T, Tucker, C, Väliviita, J, van de Weygaert, R, Van Tent, B, Vennin, V, Vermeulen, G, Vielva, P, Vittorio, N, Young, K, Zannoni, M, Institut d'Astrophysique de Paris (IAP), Institut national des sciences de l'Univers (INSU - CNRS)-Sorbonne Université (SU)-Centre National de la Recherche Scientifique (CNRS), Laboratoire d'Annecy-le-Vieux de Physique Théorique (LAPTH), Université Savoie Mont Blanc (USMB [Université de Savoie] [Université de Chambéry])-Centre National de la Recherche Scientifique (CNRS), AstroParticule et Cosmologie (APC (UMR_7164)), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS)-Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Observatoire de Paris, PSL Research University (PSL)-PSL Research University (PSL)-Université Paris Diderot - Paris 7 (UPD7), Institut d'astrophysique spatiale (IAS), Université Paris-Sud - Paris 11 (UP11)-Institut national des sciences de l'Univers (INSU - CNRS)-Centre National de la Recherche Scientifique (CNRS), Institut de recherche en astrophysique et planétologie (IRAP), Université Toulouse III - Paul Sabatier (UT3), Université Fédérale Toulouse Midi-Pyrénées-Université Fédérale Toulouse Midi-Pyrénées-Observatoire Midi-Pyrénées (OMP), Université Fédérale Toulouse Midi-Pyrénées-Centre National de la Recherche Scientifique (CNRS), Département de Recherche Fondamentale sur la Matière Condensée (DRFMC), Commissariat à l'énergie atomique et aux énergies alternatives (CEA), Département de Physique des Particules (ex SPP) (DPP), Institut de Recherches sur les lois Fondamentales de l'Univers (IRFU), Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris-Saclay-Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris-Saclay, Institut Néel (NEEL), Université Joseph Fourier - Grenoble 1 (UJF)-Centre National de la Recherche Scientifique (CNRS)-Université Grenoble Alpes (UGA), Laboratoire de Physique Nucléaire et de Hautes Énergies (LPNHE (UMR_7585)), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Paris Diderot - Paris 7 (UPD7)-Sorbonne Université (SU)-Centre National de la Recherche Scientifique (CNRS), Laboratoire de Physique Théorique d'Orsay [Orsay] (LPT), Université Paris-Sud - Paris 11 (UP11)-Centre National de la Recherche Scientifique (CNRS), Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Observatoire de Paris, Université Paris sciences et lettres (PSL)-Université Paris sciences et lettres (PSL)-Université Paris Diderot - Paris 7 (UPD7)-Centre National de la Recherche Scientifique (CNRS), Université Paris-Sud - Paris 11 (UP11)-Institut national des sciences de l'Univers (INSU - CNRS)-Centre National de la Recherche Scientifique (CNRS)-Centre National d’Études Spatiales [Paris] (CNES), Université de Toulouse (UT)-Université de Toulouse (UT)-Institut national des sciences de l'Univers (INSU - CNRS)-Observatoire Midi-Pyrénées (OMP), Institut de Recherche pour le Développement (IRD)-Université Toulouse III - Paul Sabatier (UT3), Université de Toulouse (UT)-Université de Toulouse (UT)-Institut national des sciences de l'Univers (INSU - CNRS)-Centre National d'Études Spatiales [Toulouse] (CNES)-Centre National de la Recherche Scientifique (CNRS)-Météo-France -Institut de Recherche pour le Développement (IRD)-Institut national des sciences de l'Univers (INSU - CNRS)-Centre National d'Études Spatiales [Toulouse] (CNES)-Centre National de la Recherche Scientifique (CNRS)-Météo-France -Centre National de la Recherche Scientifique (CNRS), Cryogénie (NEEL - Cryo), Institut polytechnique de Grenoble - Grenoble Institute of Technology (Grenoble INP )-Centre National de la Recherche Scientifique (CNRS)-Université Grenoble Alpes [2016-2019] (UGA [2016-2019])-Institut polytechnique de Grenoble - Grenoble Institute of Technology (Grenoble INP )-Centre National de la Recherche Scientifique (CNRS)-Université Grenoble Alpes [2016-2019] (UGA [2016-2019]), Département de Physique des Particules (ex SPP) (DPhP), Hélium : du fondamental aux applications (NEEL - HELFA), Sorbonne Université (SU), Observatoire de Paris, Université Paris sciences et lettres (PSL)-Université Paris sciences et lettres (PSL)-Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris Diderot - Paris 7 (UPD7)-Centre National de la Recherche Scientifique (CNRS)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3), Institut national des sciences de l'Univers (INSU - CNRS)-Université Toulouse III - Paul Sabatier (UT3), Météo France-Centre National d'Études Spatiales [Toulouse] (CNES)-Université Fédérale Toulouse Midi-Pyrénées-Centre National de la Recherche Scientifique (CNRS)-Institut de Recherche pour le Développement (IRD)-Météo France-Centre National d'Études Spatiales [Toulouse] (CNES)-Centre National de la Recherche Scientifique (CNRS)-Institut de Recherche pour le Développement (IRD)-Centre National de la Recherche Scientifique (CNRS), Institut polytechnique de Grenoble - Grenoble Institute of Technology (Grenoble INP )-Centre National de la Recherche Scientifique (CNRS)-Université Grenoble Alpes [2016-2019] (UGA [2016-2019]), and Centre National de la Recherche Scientifique (CNRS)-Université Paris-Sud - Paris 11 (UP11)
Subjects: gravitation: model, [ PHYS.ASTR ] Physics [physics]/Astrophysics [astro-ph], Cosmic microwave background, cosmological parameters from CMBR, CMBR experiments, neutrino masses from cosmology, BACKGROUND ANISOTROPIES, cosmic background radiation: polarization, Astrophysics, baryon: oscillation: acoustic, NEUTRINO MASS, 01 natural sciences, COBE FIRAS INSTRUMENT, current: constraint, DESI, High Energy Physics - Phenomenology (hep-ph), CMBR experiments, CMB POLARIZATION, dark energy, 010303 astronomy & astrophysics, general relativity and quantum cosmology, QC, cosmological parameters from CMBR, neutrino masses from cosmology, media_common, helium: primordial, QB, Physics, birefringence, hep-th, formation, Astrophysics::Instrumentation and Methods for Astrophysics, hep-ph, TEMPERATURE-REDSHIFT RELATION, high energy physics - theory, inflation: model, high energy physics - phenomenology, curvature, symbols, astro-ph.CO, CMBR experiment, FUNDAMENTAL CONSTANTS, Astrophysics - Cosmology and Nongalactic Astrophysics, Cosmology and Nongalactic Astrophysics (astro-ph.CO), satellite: Planck, ANGULAR POWER SPECTRUM, Primordial fluctuations, media_common.quotation_subject, gr-qc, Dark matter, satellite, FOS: Physical sciences, General Relativity and Quantum Cosmology (gr-qc), Astrophysics::Cosmology and Extragalactic Astrophysics, NO, BROKEN LEPTON NUMBER, symbols.namesake, FIS/05 - ASTRONOMIA E ASTROFISICA, Settore FIS/05 - Astronomia e Astrofisica, FINE-STRUCTURE CONSTANT, 0103 physical sciences, ionization, LARGE-SCALE STRUCTURE, structure, Planck, Reionization, PROBING NEUTRINO MASSES, Inflation (cosmology), 010308 nuclear & particles physics, fluctuation: primordial, Astronomy and Astrophysics, dark matter: annihilation, sensitivity, 115 Astronomy, Space science, MICROWAVE-ANISOTROPY-PROBE, Universe, recombination, COLD DARK-MATTER, High Energy Physics - Theory (hep-th), 13. Climate action, Dark energy, DIGITAL SKY SURVEY, [PHYS.ASTR]Physics [physics]/Astrophysics [astro-ph], MICROWAVE BACKGROUND POLARIZATION
Abstract: We forecast the main cosmological parameter constraints achievable with the CORE space mission which is dedicated to mapping the polarisation of the Cosmic Microwave Background (CMB). CORE was recently submitted in response to ESA's fifth call for medium-sized mission proposals (M5). Here we report the results from our pre-submission study of the impact of various instrumental options, in particular the telescope size and sensitivity level, and review the great, transformative potential of the mission as proposed. Specifically, we assess the impact on a broad range of fundamental parameters of our Universe as a function of the expected CMB characteristics, with other papers in the series focusing on controlling astrophysical and instrumental residual systematics. In this paper, we assume that only a few central CORE frequency channels are usable for our purpose, all others being devoted to the cleaning of astrophysical contaminants. On the theoretical side, we assume LCDM as our general framework and quantify the improvement provided by CORE over the current constraints from the Planck 2015 release. We also study the joint sensitivity of CORE and of future Baryon Acoustic Oscillation and Large Scale Structure experiments like DESI and Euclid. Specific constraints on the physics of inflation are presented in another paper of the series. In addition to the six parameters of the base LCDM, which describe the matter content of a spatially flat universe with adiabatic and scalar primordial fluctuations from inflation, we derive the precision achievable on parameters like those describing curvature, neutrino physics, extra light relics, primordial helium abundance, dark matter annihilation, recombination physics, variation of fundamental constants, dark energy, modified gravity, reionization and cosmic birefringence. (ABRIDGED), Comment: 90 pages, 25 Figures. Revised version with new authors list and references
Published: 2018
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3. Exploring Cosmic Origins with CORE:survey requirements and mission design

Author: Karl Young, N. Mandolesi, A. Renzi, D. McCarthy, Andrea Lapi, F. Voisin, F. Oppizzi, Mark Hindmarsh, A. Mennella, Josquin Errard, S. Martin, Jose M. Diego, Enrico Pajer, Douglas Scott, A. Da Silva, Luigi Danese, R. B. Partridge, Subodh P. Patil, Créidhe O'Sullivan, A. M. C. Le Brun, Gianluca Polenta, Deanna C. Hooper, Alessandro Buzzelli, O. Perdereau, Jose Alberto Rubino-Martin, Nicolas Ponthieu, C. J. A. P. Martins, Eric Hivon, M. De Petris, Reijo Keskitalo, Bruno Maffei, Rashid Sunyaev, Michael L. Brown, Elena Giusarma, Marek Biesiada, Joanes Lizarraga, Nicola Bartolo, F. Piacentini, Stephen M. Feeney, G. de Zotti, Neil Trappe, Bin Hu, Cristian Franceschet, Matthieu Tristram, Pasquale Mazzotta, R. Allison, Hannu Kurki-Suonio, Jens Chluba, J. Greenslade, R. Fernandez-Cobos, Alicia Gomez, Stephen Serjeant, A. Catalano, Paolo Natoli, C. S. Carvalho, K. Kiiveri, David L. Clements, Diego Molinari, S. Paradiso, Martina Gerbino, Vincent Vennin, Carole Tucker, Kaustuv Basu, Alexei A. Starobinsky, Sabino Matarrese, Andrea Ravenni, L. Salvati, Eduardo Artal, G. Vermeulen, M. Piat, M. Tucci, F. Noviello, Ingunn Kathrine Wehus, Elia S. Battistelli, Matteo Bonato, R. Banerji, Ted Kisner, Jean-Baptiste Melin, Christophe Ringeval, Christopher G. R. Wallis, Benjamin D. Wandelt, Julian Borrill, Massimiliano Lattanzi, Aurelien Bideaud, Sebastien Clesse, Tiziana Trombetti, Martin Crook, Will Handley, P. de Bernardis, Ruth Durrer, Francois Boulanger, Matthieu Roman, C. Y. Tan, Sébastien Triqueneaux, Silvia Galli, G. Signorelli, A. Tartari, Gianmassimo Tasinato, S. Basak, Nicola Vittorio, D. Tramonte, V. Lindholm, Julien Lesgourgues, J. F. Macías-Pérez, E. Di Valentino, Francesco Forastieri, G. de Gasperis, Thomas Kitching, Vincent Desjacques, François R. Bouchet, Zhen-Yi Cai, Sergio Colafrancesco, Richard A. Battye, Alessandro Monfardini, F.-X. Désert, Alessandro Paiella, Jesús Torrado, Michele Liguori, Anthony Challinor, Carlo Burigana, G. Castellano, Agnieszka Pollo, Daniel Baumann, L. Pagano, Boudewijn F. Roukema, Mathieu Remazeilles, Sophie Henrot-Versille, M. Tomasi, Enrique Martinez-Gonzalez, Giampaolo Pisano, M. Kunz, Joseph J. Mohr, Ricardo Genova-Santos, P. Vielva, Mattia Negrello, Marcella Massardi, Carlo Baccigalupi, Guilaine Lagache, Marco Bersanelli, Anthony Lasenby, S. Hagstotz, Domingos Barbosa, E. Keihänen, D. Prêle, Vivian Poulin, Mario Zannoni, Alain Benoit, Ana Achúcarro, D. T. Hoang, I. Colantoni, U. Fuskeland, D. Contreras, Giovanni Cabass, Jochem J. A. Baselmans, Johannes Goupy, Jochen Weller, I. Charles, Sebastian Grandis, Giuseppe D'Alessandro, M. Ashdown, A. Bonaldi, Frederico Arroja, Guido D'Amico, Gemma Luzzi, M. A. de Avillez, Martino Calvo, Silvia Masi, Daniela Paoletti, Alessandro Coppolecchia, Andrea Caputo, L. Polastri, Alessandro Melchiorri, Jon Urrestilla, Licia Verde, Mario Ballardini, Luisa Toffolatti, Jacques Delabrouille, Alessio Notari, Maciej Bilicki, Fabio Finelli, L. A. Montier, James G. Bartlett, Guillaume Patanchon, Carlos Hernández-Monteagudo, Miguel Quartin, Cora Dvorkin, Simon Doyle, H. K. Eriksen, C. Hervias-Caimapo, R. van de Weygaert, Clive Dickinson, Peter A. R. Ade, Matthew Hills, Luca Lamagna, B. Van Tent, A. J. Banday, Thejs Brinckmann, F. J. Casas, Martin Bucher, Shaul Hanany, Jussi Valiviita, J. González-Nuevo, Diederik Roest, String Theory (ITFA, IoP, FNWI), Universitat de Barcelona, AstroParticule et Cosmologie (APC (UMR_7164)), Observatoire de Paris, PSL Research University (PSL)-PSL Research University (PSL)-Université Paris Diderot - Paris 7 (UPD7)-Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Institut d'Astrophysique de Paris (IAP), Institut national des sciences de l'Univers (INSU - CNRS)-Sorbonne Université (SU)-Centre National de la Recherche Scientifique (CNRS), Institut de recherche en astrophysique et planétologie (IRAP), Université Toulouse III - Paul Sabatier (UT3), Université Fédérale Toulouse Midi-Pyrénées-Université Fédérale Toulouse Midi-Pyrénées-Observatoire Midi-Pyrénées (OMP), Université Fédérale Toulouse Midi-Pyrénées-Centre National de la Recherche Scientifique (CNRS), Institut Néel (NEEL), Université Grenoble Alpes (UGA)-Centre National de la Recherche Scientifique (CNRS)-Université Joseph Fourier - Grenoble 1 (UJF), Institut d'astrophysique spatiale (IAS), Université Paris-Sud - Paris 11 (UP11)-Institut national des sciences de l'Univers (INSU - CNRS)-Centre National de la Recherche Scientifique (CNRS), Laboratoire de Physique Subatomique et de Cosmologie (LPSC), Université Joseph Fourier - Grenoble 1 (UJF)-Institut polytechnique de Grenoble - Grenoble Institute of Technology (Grenoble INP)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Institut Polytechnique de Grenoble - Grenoble Institute of Technology-Centre National de la Recherche Scientifique (CNRS)-Université Grenoble Alpes (UGA), Institut Nanosciences et Cryogénie (INAC), Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Grenoble Alpes (UGA), Institut de Planétologie et d'Astrophysique de Grenoble (IPAG), Centre National d'Études Spatiales [Toulouse] (CNES)-Université Grenoble Alpes (UGA)-Centre National de la Recherche Scientifique (CNRS)-Institut national des sciences de l'Univers (INSU - CNRS)-Observatoire des Sciences de l'Univers de Grenoble (OSUG), Université Savoie Mont Blanc (USMB [Université de Savoie] [Université de Chambéry])-Institut polytechnique de Grenoble - Grenoble Institute of Technology (Grenoble INP)-Institut national de recherche en sciences et technologies pour l'environnement et l'agriculture (IRSTEA)-Université Joseph Fourier - Grenoble 1 (UJF)-Institut national des sciences de l'Univers (INSU - CNRS)-Centre National de la Recherche Scientifique (CNRS)-Université Grenoble Alpes (UGA)-Université Savoie Mont Blanc (USMB [Université de Savoie] [Université de Chambéry])-Institut polytechnique de Grenoble - Grenoble Institute of Technology (Grenoble INP)-Institut national de recherche en sciences et technologies pour l'environnement et l'agriculture (IRSTEA)-Université Joseph Fourier - Grenoble 1 (UJF)-Centre National de la Recherche Scientifique (CNRS), Institut Lagrange de Paris, Sorbonne Universités, Laboratoire de l'Accélérateur Linéaire (LAL), Université Paris-Sud - Paris 11 (UP11)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Laboratoire d'Astrophysique de Marseille (LAM), Centre National de la Recherche Scientifique (CNRS)-Institut national des sciences de l'Univers (INSU - CNRS)-Aix Marseille Université (AMU)-Centre National d'Études Spatiales [Toulouse] (CNES), Astrophysique Interprétation Modélisation (AIM (UMR_7158 / UMR_E_9005 / UM_112)), Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Institut national des sciences de l'Univers (INSU - CNRS)-Université Paris Diderot - Paris 7 (UPD7)-Centre National de la Recherche Scientifique (CNRS), Département de Physique des Particules (ex SPP) (DPP), Institut de Recherches sur les lois Fondamentales de l'Univers (IRFU), Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris-Saclay-Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris-Saclay, Laboratoire d'Annecy-le-Vieux de Physique Théorique (LAPTH), Université Savoie Mont Blanc (USMB [Université de Savoie] [Université de Chambéry])-Centre National de la Recherche Scientifique (CNRS), Laboratoire de Physique Nucléaire et de Hautes Énergies (LPNHE (UMR_7585)), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Paris Diderot - Paris 7 (UPD7)-Sorbonne Université (SU)-Centre National de la Recherche Scientifique (CNRS), Centre de Recherche Astrophysique de Lyon (CRAL), École normale supérieure - Lyon (ENS Lyon)-Université Claude Bernard Lyon 1 (UCBL), Université de Lyon-Université de Lyon-Institut national des sciences de l'Univers (INSU - CNRS)-Centre National de la Recherche Scientifique (CNRS), Laboratoire de Physique Théorique d'Orsay [Orsay] (LPT), Université Paris-Sud - Paris 11 (UP11)-Centre National de la Recherche Scientifique (CNRS), CORE, Department of Physics, Helsinki Institute of Physics, Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Observatoire de Paris, Université Paris sciences et lettres (PSL)-Université Paris sciences et lettres (PSL)-Université Paris Diderot - Paris 7 (UPD7)-Centre National de la Recherche Scientifique (CNRS), Hélium : du fondamental aux applications (NEEL - HELFA), Institut polytechnique de Grenoble - Grenoble Institute of Technology (Grenoble INP )-Centre National de la Recherche Scientifique (CNRS)-Université Grenoble Alpes [2016-2019] (UGA [2016-2019])-Institut polytechnique de Grenoble - Grenoble Institute of Technology (Grenoble INP )-Centre National de la Recherche Scientifique (CNRS)-Université Grenoble Alpes [2016-2019] (UGA [2016-2019]), Université Paris-Sud - Paris 11 (UP11)-Institut national des sciences de l'Univers (INSU - CNRS)-Centre National de la Recherche Scientifique (CNRS)-Centre National d’Études Spatiales [Paris] (CNES), Cryogénie (NEEL - Cryo), Institut polytechnique de Grenoble - Grenoble Institute of Technology (Grenoble INP )-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS)-Université Grenoble Alpes [2016-2019] (UGA [2016-2019]), Laboratoire des Cryoréfrigérateurs et Cryogénie Spatiale (LCCS), Service des Basses Températures (SBT ), Université Grenoble Alpes [2016-2019] (UGA [2016-2019])-Institut de Recherche Interdisciplinaire de Grenoble (IRIG), Direction de Recherche Fondamentale (CEA) (DRF (CEA)), Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Direction de Recherche Fondamentale (CEA) (DRF (CEA)), Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Grenoble Alpes [2016-2019] (UGA [2016-2019])-Institut de Recherche Interdisciplinaire de Grenoble (IRIG), Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Commissariat à l'énergie atomique et aux énergies alternatives (CEA), Université Paris sciences et lettres (PSL)-Université Paris sciences et lettres (PSL)-Centre National de la Recherche Scientifique (CNRS)-Université Paris Cité (UPC), Université Fédérale Toulouse Midi-Pyrénées-Université Fédérale Toulouse Midi-Pyrénées-Institut national des sciences de l'Univers (INSU - CNRS)-Observatoire Midi-Pyrénées (OMP), Institut de Recherche pour le Développement (IRD)-Institut national des sciences de l'Univers (INSU - CNRS)-Centre National d'Études Spatiales [Toulouse] (CNES)-Centre National de la Recherche Scientifique (CNRS)-Université Fédérale Toulouse Midi-Pyrénées-Météo-France -Institut de Recherche pour le Développement (IRD)-Institut national des sciences de l'Univers (INSU - CNRS)-Centre National d'Études Spatiales [Toulouse] (CNES)-Centre National de la Recherche Scientifique (CNRS)-Météo-France -Centre National de la Recherche Scientifique (CNRS), Institut polytechnique de Grenoble - Grenoble Institute of Technology (Grenoble INP )-Centre National de la Recherche Scientifique (CNRS)-Université Grenoble Alpes [2016-2019] (UGA [2016-2019]), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS)-Université Grenoble Alpes (UGA)-Institut polytechnique de Grenoble - Grenoble Institute of Technology (Grenoble INP ), Université Grenoble Alpes (UGA), Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Grenoble Alpes [2016-2019] (UGA [2016-2019]), Institut national des sciences de l'Univers (INSU - CNRS)-Centre National d'Études Spatiales [Toulouse] (CNES)-Centre National de la Recherche Scientifique (CNRS)-Observatoire des Sciences de l'Univers de Grenoble (OSUG ), Institut polytechnique de Grenoble - Grenoble Institute of Technology (Grenoble INP )-Institut national des sciences de l'Univers (INSU - CNRS)-Institut national de recherche en sciences et technologies pour l'environnement et l'agriculture (IRSTEA)-Université Savoie Mont Blanc (USMB [Université de Savoie] [Université de Chambéry])-Centre National de la Recherche Scientifique (CNRS)-Université Grenoble Alpes [2016-2019] (UGA [2016-2019])-Institut polytechnique de Grenoble - Grenoble Institute of Technology (Grenoble INP )-Institut national de recherche en sciences et technologies pour l'environnement et l'agriculture (IRSTEA)-Université Savoie Mont Blanc (USMB [Université de Savoie] [Université de Chambéry])-Centre National de la Recherche Scientifique (CNRS)-Université Grenoble Alpes [2016-2019] (UGA [2016-2019]), Aix Marseille Université (AMU)-Institut national des sciences de l'Univers (INSU - CNRS)-Centre National d'Études Spatiales [Toulouse] (CNES)-Centre National de la Recherche Scientifique (CNRS), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Sorbonne Université (SU)-Centre National de la Recherche Scientifique (CNRS), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS)-Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Observatoire de Paris, PSL Research University (PSL)-PSL Research University (PSL)-Université Paris Diderot - Paris 7 (UPD7), Université Joseph Fourier - Grenoble 1 (UJF)-Centre National de la Recherche Scientifique (CNRS)-Université Grenoble Alpes (UGA), Université Grenoble Alpes (UGA)-Commissariat à l'énergie atomique et aux énergies alternatives (CEA), Centre National de la Recherche Scientifique (CNRS)-Institut national des sciences de l'Univers (INSU - CNRS)-Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris Diderot - Paris 7 (UPD7), Université Paris sciences et lettres (PSL)-Université Paris sciences et lettres (PSL)-Centre National de la Recherche Scientifique (CNRS)-Université de Paris (UP), Institut national des sciences de l'Univers (INSU - CNRS)-Université Toulouse III - Paul Sabatier (UT3), Météo France-Centre National d'Études Spatiales [Toulouse] (CNES)-Université Fédérale Toulouse Midi-Pyrénées-Centre National de la Recherche Scientifique (CNRS)-Institut de Recherche pour le Développement (IRD)-Météo France-Centre National d'Études Spatiales [Toulouse] (CNES)-Centre National de la Recherche Scientifique (CNRS)-Institut de Recherche pour le Développement (IRD)-Centre National de la Recherche Scientifique (CNRS), Université Grenoble Alpes [2016-2019] (UGA [2016-2019])-Commissariat à l'énergie atomique et aux énergies alternatives (CEA), Centre National d'Études Spatiales [Toulouse] (CNES)-Observatoire des Sciences de l'Univers de Grenoble (OSUG ), Institut national des sciences de l'Univers (INSU - CNRS)-Université Savoie Mont Blanc (USMB [Université de Savoie] [Université de Chambéry])-Centre National de la Recherche Scientifique (CNRS)-Institut National de Recherche pour l’Agriculture, l’Alimentation et l’Environnement (INRAE)-Université Grenoble Alpes (UGA)-Institut national des sciences de l'Univers (INSU - CNRS)-Université Savoie Mont Blanc (USMB [Université de Savoie] [Université de Chambéry])-Centre National de la Recherche Scientifique (CNRS)-Institut National de Recherche pour l’Agriculture, l’Alimentation et l’Environnement (INRAE)-Université Grenoble Alpes (UGA), Sorbonne Université (SU), Centre National de la Recherche Scientifique (CNRS)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Paris-Sud - Paris 11 (UP11), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Sorbonne Université (SU)-Centre National de la Recherche Scientifique (CNRS)-Université de Paris (UP), Université de Lyon-Université de Lyon-Centre National de la Recherche Scientifique (CNRS)-Institut national des sciences de l'Univers (INSU - CNRS), Centre National de la Recherche Scientifique (CNRS)-Université Paris-Sud - Paris 11 (UP11), Université Paris sciences et lettres (PSL)-Université Paris sciences et lettres (PSL)-Centre National de la Recherche Scientifique (CNRS)-Université Paris Cité (UPCité), Delabrouille, J, de Bernardis, P, Bouchet, F, Achúcarro, A, Ade, P, Allison, R, Arroja, F, Artal, E, Ashdown, M, Baccigalupi, C, Ballardini, M, Banday, A, Banerji, R, Barbosa, D, Bartlett, J, Bartolo, N, Basak, S, Baselmans, J, Basu, K, Battistelli, E, Battye, R, Baumann, D, Benoít, A, Bersanelli, M, Bideaud, A, Biesiada, M, Bilicki, M, Bonaldi, A, Bonato, M, Borrill, J, Boulanger, F, Brinckmann, T, Brown, M, Bucher, M, Burigana, C, Buzzelli, A, Cabass, G, Cai, Z, Calvo, M, Caputo, A, Carvalho, C, Casas, F, Castellano, G, Catalano, A, Challinor, A, Charles, I, Chluba, J, Clements, D, Clesse, S, Colafrancesco, S, Colantoni, I, Contreras, D, Coppolecchia, A, Crook, M, D'Alessandro, G, D'Amico, G, da Silva, A, de Avillez, M, de Gasperis, G, De Petris, M, de Zotti, G, Danese, L, Désert, F, Desjacques, V, Valentino, E, Dickinson, C, Diego, J, Doyle, S, Durrer, R, Dvorkin, C, Eriksen, H, Errard, J, Feeney, S, Fernández-Cobos, R, Finelli, F, Forastieri, F, Franceschet, C, Fuskeland, U, Galli, S, Génova-Santos, R, Gerbino, M, Giusarma, E, Gomez, A, González-Nuevo, J, Grandis, S, Greenslade, J, Goupy, J, Hagstotz, S, Hanany, S, Handley, W, Henrot-Versillé, S, Hernández-Monteagudo, C, Hervias-Caimapo, C, Hills, M, Hindmarsh, M, Hivon, E, Hoang, D, Hooper, D, Hu, B, Keihänen, E, Keskitalo, R, Kiiveri, K, Kisner, T, Kitching, T, Kunz, M, Kurki-Suonio, H, Lagache, G, Lamagna, L, Lapi, A, Lasenby, A, Lattanzi, M, Brun, A, Lesgourgues, J, Liguori, M, Lindholm, V, Lizarraga, J, Luzzi, G, Macìas-Pérez, J, Maffei, B, Mandolesi, N, Martin, S, Martinez-Gonzalez, E, Martins, C, Masi, S, Massardi, M, Matarrese, S, Mazzotta, P, Mccarthy, D, Melchiorri, A, Melin, J, Mennella, A, Mohr, J, Molinari, D, Monfardini, A, Montier, L, Natoli, P, Negrello, M, Notari, A, Noviello, F, Oppizzi, F, O'Sullivan, C, Pagano, L, Paiella, A, Pajer, E, Paoletti, D, Paradiso, S, Partridge, R, Patanchon, G, Patil, S, Perdereau, O, Piacentini, F, Piat, M, Pisano, G, Polastri, L, Polenta, G, Pollo, A, Ponthieu, N, Poulin, V, Prêle, D, Quartin, M, Ravenni, A, Remazeilles, M, Renzi, A, Ringeval, C, Roest, D, Roman, M, Roukema, B, Rubiño-Martin, J, Salvati, L, Scott, D, Serjeant, S, Signorelli, G, Starobinsky, A, Sunyaev, R, Tan, C, Tartari, A, Tasinato, G, Toffolatti, L, Tomasi, M, Torrado, J, Tramonte, D, Trappe, N, Triqueneaux, S, Tristram, M, Trombetti, T, Tucci, M, Tucker, C, Urrestilla, J, Väliviita, J, de Weygaert, R, Tent, B, Vennin, V, Verde, L, Vermeulen, G, Vielva, P, Vittorio, N, Voisin, F, Wallis, C, Wandelt, B, Wehus, I, Weller, J, Young, K, and Zannoni, M
Subjects: CMBR experiments, CMBR polarisation, gravitational lensing, physics of the early universe, POLARIZATION, Computer science, Cosmic microwave background, cosmic background radiation: polarization, CMB, 7. Clean energy, 01 natural sciences, Cosmology, Physics, Particles & Fields, cosmic flows, CMBR polarization, astronomy and astrophysics, Cosmic physics, CMBR experiments – CMBR theory – reionization – high redshift galaxies, 010303 astronomy & astrophysics, QC, QB, COSMIC cancer database, Physics, Astrophysics::Instrumentation and Methods for Astrophysics, Nuclear & Particles Physics, cryogenics, Physical Sciences, Physics::Space Physics, Systems engineering, astro-ph.CO, proposed experiment, Astrophysics::Earth and Planetary Astrophysics, CMBR experiment, Astrophysics - Instrumentation and Methods for Astrophysics, performance, Astrophysics - Cosmology and Nongalactic Astrophysics, Astrophysics and Astronomy, Cosmology and Nongalactic Astrophysics (astro-ph.CO), CMBR experiments, CMBR polarisation, gravitational lensing, physics of the early universe, satellite, FOS: Physical sciences, Astrophysics::Cosmology and Extragalactic Astrophysics, Astronomy & Astrophysics, NO, HALF-WAVE PLATE, 0202 Atomic, Molecular, Nuclear, Particle And Plasma Physics, Mission design, Settore FIS/05 - Astronomia e Astrofisica, 0103 physical sciences, [PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det], Instrumentation and Methods for Astrophysics (astro-ph.IM), detector: design, activity report, Science & Technology, Cosmologia, 010308 nuclear & particles physics, astro-ph.IM, 115 Astronomy, Space science, sensitivity, Complementarity (physics), 0201 Astronomical And Space Sciences, angular resolution, [PHYS.ASTR]Physics [physics]/Astrophysics [astro-ph], Física còsmica
Abstract: The CORE collaboration thanks CNES, Thales Alenia Space, and Air Liquide Advanced Technologies for advice and technical support during the preparation of the CORE proposal. We also thank the ESA CDF team for the CMB Polarisation CDF study performed in March 2016, the results of which were extensively used to define the mission concept presented in this paper. J.G.N. acknowledges financial support from the Spanish MINECO for a Ramon y Cajal fellowship (RYC-2013-13256) and the I+D 2015 project AYA2015-65887-P (MINECO/FEDER). CJM is supported by an FCT Research Professorship, contract reference IF/00064/2012, funded by FCT/MCTES (Portugal) and POPH/FSE. F.J.C., R.F.-C., E.M.-G. and P.V. acknowledge support from the Spanish Ministerio de Econom´ıa y Competitividad project ESP2015-70646-C2-1-R (cofinanced with EU FEDER funds), ConsoliderIngenio 2010 project CSD2010-00064 and from the CSIC “Proyecto Intramural Especial” project 201550E091. FA is supported by the National Taiwan University (NTU) under Project No. 103R4000 and by the NTU Leung Center for Cosmology and Particle Astrophysics (LeCosPA) under Project No. FI121. BFR acknowledges support from the National Science Centre, Poland, under grant 2014/13/B/ST9/00845., Macìas-Pérez, J.F., Delabrouille, J., De Bernardis, P., Bouchet, F.R., Achúcarro, A., Ade, P.A.R., Allison, R., Arroja, F., Artal, E., Ashdown, M., Baccigalupi, C., Ballardini, M., Banday, A.J., Banerji, R., Barbosa, D., Bartlett, J., Bartolo, N., Basak, S., Baselmans, J.J.A., Basu, K., Battistelli, E.S., Battye, R., Baumann, D., Benoít, A., Bersanelli, M., Bideaud, A., Biesiada, M., Bilicki, M., Bonaldi, A., Bonato, M., Borrill, J., Boulanger, F., Brinckmann, T., Brown, M.L., Bucher, M., Burigana, C., Buzzelli, A., Cabass, G., Cai, Z.-Y., Calvo, M., Caputo, A., Carvalho, C.-S., Casas, F.J., Castellano, G., Catalano, A., Challinor, A., Charles, I., Chluba, J., Clements, D.L., Clesse, S., Colafrancesco, S., Colantoni, I., Contreras, D., Coppolecchia, A., Crook, M., D'Alessandro, G., D'Amico, G., Silva, A.D., De Avillez, M., De Gasperis, G., Petris, M.D., De Zotti, G., Danese, L., Désert, F.-X., Desjacques, V., Valentino, E.D., Dickinson, C., Diego, J.M., Doyle, S., Durrer, R., Dvorkin, C., Eriksen, H.K., Errard, J., Feeney, S., Fernández-Cobos, R., Finelli, F., Forastieri, F., Franceschet, C., Fuskeland, U., Galli, S., Génova-Santos, R.T., Gerbino, M., Giusarma, E., Gomez, A., González-Nuevo, J., Grandis, S., Greenslade, J., Goupy, J., Hagstotz, S., Hanany, S., Handley, W., Henrot-Versillé, S., Hernández-Monteagudo, C., Hervias-Caimapo, C., Hills, M., Hindmarsh, M., Hivon, E., Hoang, D.T., Hooper, D.C., Hu, B., Keihänen, E., Keskitalo, R., Kiiveri, K., Kisner, T., Kitching, T., Kunz, M., Kurki-Suonio, H., Lagache, G., Lamagna, L., Lapi, A., Lasenby, A., Lattanzi, M., Brun, A.M.C.L., Lesgourgues, J., Liguori, M., Lindholm, V., Lizarraga, J., Luzzi, G., Macìas-Pérez, J.F., Maffei, B., Mandolesi, N., Martin, S., Martinez-Gonzalez, E., Martins, C.J.A.P., Masi, S., Massardi, M., Matarrese, S., Mazzotta, P., McCarthy, D., Melchiorri, A., Melin, J.-B., Mennella, A., Mohr, J., Molinari, D., Monfardini, A., Montier, L., Natoli, P., Negrello, M., Notari, A., Noviello, F., Oppizzi, F., O'Sullivan, C., Pagano, L., Paiella, A., Pajer, E., Paoletti, D., Paradiso, S., Partridge, R.B., Patanchon, G., Patil, S.P., Perdereau, O., Piacentini, F., Piat, M., Pisano, G., Polastri, L., Polenta, G., Pollo, A., Ponthieu, N., Poulin, V., Prêle, D., Quartin, M., Ravenni, A., Remazeilles, M., Renzi, A., Ringeval, C., Roest, D., Roman, M., Roukema, B.F., Rubiño-Martin, J.-A., Salvati, L., Scott, D., Serjeant, S., Signorelli, G., Starobinsky, A.A., Sunyaev, R., Tan, C.Y., Tartari, A., Tasinato, G., Toffolatti, L., Tomasi, M., Torrado, J., Tramonte, D., Trappe, N., Triqueneaux, S., Tristram, M., Trombetti, T., Tucci, M., Tucker, C., Urrestilla, J., Väliviita, J., De Weygaert, R.V., Tent, B.V., Vennin, V., Verde, L., Vermeulen, G., Vielva, P., Vittorio, N., Voisin, F., Wallis, C., Wandelt, B., Wehus, I.K., Weller, J., Young, K., Zannoni, M.
Published: 2018
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4. Summary of the Parallel Session: 'Gravitational Waves from the Big Bang and Other Sources'

Author: Frederico Arroja
Subjects: Physics, Gravitational wave, Astronomy, Session (computer science), Astrophysics
Published: 2017
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5. The Two Faces of Mimetic Horndeski Gravity: Disformal Transformations and Lagrange Multiplier

Author: Frederico Arroja
Subjects: Gravity (chemistry), symbols.namesake, Pure mathematics, Classical mechanics, Lagrange multiplier, symbols, Mathematics
Published: 2017
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6. Large-scale structure in mimetic Horndeski gravity

Author: Purnendu Karmakar, Sabino Matarrese, Nicola Bartolo, Teppei Okumura, and Frederico Arroja
Subjects: High Energy Physics - Theory, Cosmology and Nongalactic Astrophysics (astro-ph.CO), Cold dark matter, FOS: Physical sciences, Perfect fluid, General Relativity and Quantum Cosmology (gr-qc), Astrophysics::Cosmology and Extragalactic Astrophysics, power spectrum, 01 natural sciences, General Relativity and Quantum Cosmology, Many-body problem, 0103 physical sciences, dark energy theory, Statistical physics, modified gravity, 010303 astronomy & astrophysics, Physics, Newtonian potential, 010308 nuclear & particles physics, Linear system, Spectral density, Astronomy and Astrophysics, Zero sound, gravity, High Energy Physics - Theory (hep-th), Dark energy, Astrophysics - Cosmology and Nongalactic Astrophysics
Abstract: In this paper, we propose to use the mimetic Horndeski model as a model for the dark universe. Both cold dark matter (CDM) and dark energy (DE) phenomena are described by a single component, the mimetic field. In linear theory, we show that this component effectively behaves like a perfect fluid with zero sound speed and clusters on all scales. For the simpler mimetic cubic Horndeski model, if the background expansion history is chosen to be identical to a perfect fluid DE (PFDE) then the mimetic model predicts the same power spectrum of the Newtonian potential as the PFDE model with zero sound speed. In particular, if the background is chosen to be the same as that of LCDM, then also in this case the power spectrum of the Newtonian potential in the mimetic model becomes indistinguishable from the power spectrum in LCDM on linear scales. A different conclusion may be found in the case of non-adiabatic perturbations. We also discuss the distinguishability, using power spectrum measurements from LCDM N-body simulations as a proxy for future observations, between these mimetic models and other popular models of DE. For instance, we find that if the background has an equation of state equal to -0.95 then we will be able to distinguish the mimetic model from the PFDE model with unity sound speed. On the other hand, it will be hard to do this distinction with respect to the LCDM model., v1: 17 pages, 6 figures. v2: minor changes, comments added, replaced to match published version
Published: 2018
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7. CMB constraints on running non-Gaussianity

Author: Nicola Bartolo, F. Oppizzi, Frederico Arroja, Michele Liguori, and A. Renzi
Subjects: Physics, Inflation (cosmology), Spectral index, Particle physics, Cosmology and Nongalactic Astrophysics (astro-ph.CO), 010308 nuclear & particles physics, ination, Cosmic microwave background, FOS: Physical sciences, Astronomy and Astrophysics, 01 natural sciences, CMB cold spot, symbols.namesake, CMBR experiments, non-gaussianity, physics of the early universe, Non-Gaussianity, 0103 physical sciences, symbols, Planck, Curvaton, 010303 astronomy & astrophysics, Astrophysics - Cosmology and Nongalactic Astrophysics
Abstract: We develop a complete set of tools for CMB forecasting, simulation and estimation of primordial running bispectra, arising from a variety of curvaton and single-field (DBI) models of Inflation. We validate our pipeline using mock CMB running non-Gaussianity realizations and test it on real data by obtaining experimental constraints on the $f_{\rm NL}$ running spectral index, $n_{\rm NG}$, using WMAP 9-year data. Our final bounds (68\% C.L.) read $-0.6< n_{\rm NG}, Comment: 20 pages, 8 figures, 3 table
Published: 2018
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8. Cosmological perturbations in mimetic Horndeski gravity

Author: Sabino Matarrese, Nicola Bartolo, Frederico Arroja, and Purnendu Karmakar
Subjects: High Energy Physics - Theory, Cosmology and Nongalactic Astrophysics (astro-ph.CO), Differential equation, cosmological perturbation theory, gravity, modified gravity, Scalar (mathematics), Degrees of freedom (physics and chemistry), FOS: Physical sciences, General Relativity and Quantum Cosmology (gr-qc), 01 natural sciences, General Relativity and Quantum Cosmology, symbols.namesake, Friedmann–Lemaître–Robertson–Walker metric, 0103 physical sciences, Cosmological perturbation theory, 010306 general physics, modified gravity, Physics, Newtonian potential, 010308 nuclear & particles physics, Equations of motion, Astronomy and Astrophysics, gravity, Classical mechanics, High Energy Physics - Theory (hep-th), Ordinary differential equation, cosmological perturbation theory, symbols, Astrophysics - Cosmology and Nongalactic Astrophysics
Abstract: We study linear scalar perturbations around a flat FLRW background in mimetic Horndeski gravity. In the absence of matter, we show that the Newtonian potential satisfies a second-order differential equation with no spatial derivatives. This implies that the sound speed for scalar perturbations is exactly zero on this background. We also show that in mimetic $G^3$ theories the sound speed is equally zero. We obtain the equation of motion for the comoving curvature perturbation (first order differential equation) and solve it to find that the comoving curvature perturbation is constant on all scales in mimetic Horndeski gravity. We find solutions for the Newtonian potential evolution equation in two simple models. Finally we show that the sound speed is zero on all backgrounds and therefore the system does not have any wave-like scalar degrees of freedom., v1: 17 pages. v2: minor changes, typos corrected and references added. Published version. v3: equations of Appendix D corrected. No changes in the conclusions. Supersedes published version
Published: 2016

9. The two faces of mimetic Horndeski gravity: Disformal transformations and Lagrange multiplier

Author: Sabino Matarrese, Nicola Bartolo, Frederico Arroja, and Purnendu Karmakar
Subjects: High Energy Physics - Theory, Cosmology and Nongalactic Astrophysics (astro-ph.CO), FOS: Physical sciences, Perfect fluid, General Relativity and Quantum Cosmology (gr-qc), General Relativity and Quantum Cosmology, Gravitation, symbols.namesake, dark energy theory, dark matter theory, modified gravity, physics of the early universe, Barotropic fluid, Friedmann–Lemaître–Robertson–Walker metric, Mathematical physics, Physics, Equations of motion, Astronomy and Astrophysics, Invariant (physics), High Energy Physics - Theory (hep-th), Lagrange multiplier, symbols, Scalar field, Astrophysics - Cosmology and Nongalactic Astrophysics
Abstract: We show that very general scalar-tensor theories of gravity (including, e.g., Horndeski models) are generically invariant under disformal transformations. However there is a special subset, when the transformation is not invertible, that yields new equations of motion which are a generalization of the so-called "mimetic" dark matter theory recently introduced by Chamsedinne and Mukhanov. These conclusions hold true irrespective of whether the scalar field in the action of the assumed scalar-tensor theory of gravity is the same or different than the scalar field involved in the transformation. The new equations of motion for our general mimetic theory can also be derived from an action containing an additional Lagrange multiplier field. The general mimetic scalar-tensor theory has the same number of derivatives in the equations of motion as the original scalar-tensor theory. As an application we show that the simplest mimetic scalar-tensor model is able to mimic the cosmological background of a flat FLRW model with a barotropic perfect fluid with any constant equation of state., v1: 14 pages, 1 figure; v2: minor changes and references added, replaced to match published version
Published: 2015

10. On the Trispectrum of Galileon Inflation

Author: Emanuela Dimastrogiovanni, Frederico Arroja, Nicola Bartolo, Matteo Fasiello, and Cosmic Frontier
Subjects: Inflation (cosmology), Physics, High Energy Physics - Theory, Cosmology and Nongalactic Astrophysics (astro-ph.CO), Spacetime, CONSTRAINTS, FOS: Physical sciences, Astronomy and Astrophysics, Observable, Astrophysics::Cosmology and Extragalactic Astrophysics, General Relativity and Quantum Cosmology (gr-qc), Symmetry (physics), General Relativity and Quantum Cosmology, Gravitation, Theoretical physics, High Energy Physics - Theory (hep-th), cosmological perturbation theory, non-gaussianity, physics of the early universe, Perturbation theory (quantum mechanics), Trispectrum, inflation, Bispectrum, Astrophysics - Cosmology and Nongalactic Astrophysics
Abstract: We present a detailed study of the trispectrum of the curvature perturbation generated within a stable, well defined and predictive theory which comprises an inflationary phase. In this model the usual shift symmetry is enhanced up to the so-called Galileon symmetry. The appeal of this type of theories rests on being unitary and stable under quantum corrections. Furthermore, in the specific model under consideration here, these properties have been shown to approximately hold in realistic scenarios which account for curved spacetime and the coupling with gravity. In the literature, the analysis of the bispectrum of the curvature perturbation for this theory revealed non-Gaussian features which are shared by a number of inflationary models, including stable ones. It is therefore both timely and useful to investigate further and turn to observables such as the trispectrum. We find that, in a number of specific momenta configurations, the trispectrum shape-functions present strikingly different features as compared to, for example, the entire class of the so-called $P(X,\phi)$ inflationary models., Comment: 39 pages, 14 figures
Published: 2013
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11. Strong scale dependent bispectrum in the Starobinsky model of inflation

Author: Misao Sasaki and Frederico Arroja
Subjects: Inflation (cosmology), Physics, High Energy Physics - Theory, Cosmology and Nongalactic Astrophysics (astro-ph.CO), Angular frequency, Scale (ratio), FOS: Physical sciences, Astronomy and Astrophysics, General Relativity and Quantum Cosmology (gr-qc), General Relativity and Quantum Cosmology, Amplitude, High Energy Physics - Theory (hep-th), Vacuum energy, Non-Gaussianity, Cosmological perturbation theory, Statistical physics, Bispectrum, Astrophysics - Cosmology and Nongalactic Astrophysics
Abstract: We compute analytically the dominant contribution to the tree-level bispectrum in the Starobinsky model of inflation. In this model, the potential is vacuum energy dominated but contains a subdominant linear term which changes the slope abruptly at a point. We show that on large scales compared with the transition scale $k_0$ and in the equilateral limit the analogue of the non-linearity parameter scales as $(k/k_0)^2$, that is its amplitude decays for larger and larger scales until it becomes subdominant with respect to the usual slow-roll suppressed corrections. On small scales we show that the non-linearity parameter oscillates with angular frequency given by $3/k_0$ and its amplitude grows linearly towards smaller scales and can be large depending on the model parameters. We also compare our results with previous results in the literature., 14 pages, 3 figures
Published: 2012

12. Large and strong scale dependent bispectrum in single field inflation from a sharp feature in the mass

Author: Antonio Enea Romano, Frederico Arroja, and Misao Sasaki
Subjects: High Energy Physics - Theory, Physics, Inflation (cosmology), Nuclear and High Energy Physics, Cosmology and Nongalactic Astrophysics (astro-ph.CO), Scale (ratio), Field (physics), Heaviside step function, FOS: Physical sciences, Spectral density, General Relativity and Quantum Cosmology (gr-qc), Kinetic term, General Relativity and Quantum Cosmology, symbols.namesake, Classical mechanics, High Energy Physics - Theory (hep-th), symbols, Statistical physics, Scalar field, Bispectrum, Astrophysics - Cosmology and Nongalactic Astrophysics
Abstract: We study an inflationary model driven by a single minimally coupled standard kinetic term scalar field with a step in its mass modeled by an Heaviside step function. We present an analytical approximation for the mode function of the curvature perturbation, obtain the power spectrum analytically and compare it with the numerical result. We show that, after the scale set by the step, the spectrum contains damped oscillations that are well described by our analytical approximation. We also compute the dominant contribution to the bispectrum in the equilateral and the squeezed limits and find new shapes. In the equilateral and squeezed limits the bispectrum oscillates and it has a linear growth envelope towards smaller scales. The bispectrum size can be large depending on the model parameters., 18 pages, 10 figures; v2: Plots and captions of figs. 7 and 10 corrected
Published: 2011
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13. A note on the role of the boundary terms for the non-Gaussianity in general k-inflation

Author: Frederico Arroja and Takahiro Tanaka
Subjects: Inflation (cosmology), Physics, High Energy Physics - Theory, Cosmology and Nongalactic Astrophysics (astro-ph.CO), Field (physics), FOS: Physical sciences, Boundary (topology), Astronomy and Astrophysics, General Relativity and Quantum Cosmology (gr-qc), Kinetic term, Astrophysics::Cosmology and Extragalactic Astrophysics, Inflaton, General Relativity and Quantum Cosmology, Theoretical physics, High Energy Physics - Theory (hep-th), Non-Gaussianity, Scalar field, Bispectrum, Astrophysics - Cosmology and Nongalactic Astrophysics
Abstract: In this short note we clarify the role of the boundary terms in the calculation of the leading order tree-level bispectrum in a fairly general minimally coupled single field inflationary model, where the inflaton's Lagrangian is a general function of the scalar field and its first derivatives. This includes k-inflation, DBI-inflation and standard kinetic term inflation as particular cases. These boundary terms appear when simplifying the third order action by using integrations by parts. We perform the calculation in the comoving gauge obtaining explicitly all total time derivative interactions and show that a priori they cannot be neglected. The final result for the bispectrum is equal to the result present in the literature which was obtained using the field redefinition., 8 pages, no figures; v2: Minor changes and note added at the end of the conclusion. Replaced to match published version
Published: 2011

14. A note on the equivalence of a barotropic perfect fluid with a K-essence scalar field

Author: Frederico Arroja and Misao Sasaki
Subjects: Physics, High Energy Physics - Theory, Nuclear and High Energy Physics, Cosmology and Nongalactic Astrophysics (astro-ph.CO), FOS: Physical sciences, Scalar potential, Perfect fluid, Kinetic term, General Relativity and Quantum Cosmology (gr-qc), Conservative vector field, General Relativity and Quantum Cosmology, Physics::Fluid Dynamics, Classical mechanics, High Energy Physics - Theory (hep-th), Incompressible flow, Barotropic fluid, Fluid dynamics, Scalar field, Mathematical physics, Astrophysics - Cosmology and Nongalactic Astrophysics
Abstract: In this short note, we obtain the necessary and sufficient condition for a class of non-canonical single scalar field models to be exactly equivalent to barotropic perfect fluids, under the assumption of an irrotational fluid flow. An immediate consequence of this result is that the non-adiabatic pressure perturbation in this class of scalar field systems vanishes exactly at all orders in perturbation theory and on all scales. The Lagrangian for this general class of scalar field models depends on both the kinetic term and the value of the field. However, after a field redefinition, it can be effectively cast in the form of a purely kinetic K-essence model., Comment: 4 pages, 1 figure; v2: References and footnotes 3 and 4 added. Replaced to match published version
Published: 2010
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15. Full quantum trispectrum in multifield DBI inflation

Author: Kazuya Koyama, Frederico Arroja, and Shuntaro Mizuno
Subjects: Physics, Nuclear and High Energy Physics, Cosmology and Gravitation, Amplitude, Quantum mechanics, Curvature perturbation, Trispectrum, Astrophysics::Cosmology and Extragalactic Astrophysics, String theory, Quantum
Abstract: We compute the leading order connected four-point function of the primordial curvature perturbation coming from the four-point function of the fields in multifield DBI-inflation models. We confirm that the consistency relations in the squeezed limit and in the counter-collinear limit hold as in single-field models thanks to special properties of the DBI action. We also study the momentum dependence of the trispectra coming from the adiabatic, mixed and purely entropic contributions separately and we find that they have different momentum dependence. This means that if the amount of the transfer from the entropy perturbations to the curvature perturbation is significantly large, the trispectrum can distinguish multifield DBI-inflation models from single-field DBI-inflation models. A large amount of transfer ${T}_{\mathcal{R}\mathcal{S}}\ensuremath{\gg}1$ suppresses the tensor-to-scalar ratio $r\ensuremath{\propto}{T}_{\mathcal{R}\mathcal{S}}^{\ensuremath{-}2}$ and the amplitude of the bispectrum ${f}_{\mathrm{NL}}^{\mathrm{equi}}\ensuremath{\propto}{T}_{\mathcal{R}\mathcal{S}}^{\ensuremath{-}2}$ and so it can ease the severe observational constraints on the DBI-inflation model based on string theory. On the other hand, it enhances the amplitude of the trispectrum ${\ensuremath{\tau}}_{\mathrm{NL}}^{\mathrm{equi}}\ensuremath{\propto}{T}_{\mathcal{R}\mathcal{S}}^{2}{f}_{\mathrm{NL}}^{\mathrm{equi}\text{ }2}$ for a given amplitude of the bispectrum.
Published: 2009
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16. Pathological behaviour of the scalar graviton in Ho\v{r}ava-Lifshitz gravity

Author: Frederico Arroja and Kazuya Koyama
Subjects: Physics, High Energy Physics - Theory, Cosmology and Gravitation, Nuclear and High Energy Physics, 010308 nuclear & particles physics, Hořava–Lifshitz gravity, General relativity, Graviton, Scalar (physics), 01 natural sciences, General Relativity and Quantum Cosmology, High Energy Physics::Theory, De Sitter universe, Speed of sound, 0103 physical sciences, Minkowski space, 010306 general physics, Quantum, Mathematical physics, Astrophysics - Cosmology and Nongalactic Astrophysics
Abstract: We confirm the recent claims that, in the infrared limit of Ho\v{r}ava-Lifshitz gravity, the scalar graviton becomes a ghost if the sound speed squared is positive on the flat de Sitter and Minkowski background. In order to avoid the ghost and tame the instability, the sound speed squared should be negative and very small, which means that the flow parameter $\lambda$ should be very close to its General Relativity (GR) value. We calculate the cubic interactions for the scalar graviton which are shown to have a similar structure with those of the curvature perturbation in k-inflation models. The higher order interactions become increasing important for a smaller sound speed squared, that is, when the theory approaches GR. This invalidates any linearized analysis and any predictability is lost in this limit as quantum corrections are not controllable. This pathological behaviour of the scalar graviton casts doubt on the validity of the projectable version of the theory., Comment: 7 pages, references added; v3: Typos corrected, minor changes to text and precise determination of the strong coupling scale. Replaced to match published version.
Published: 2009
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17. Full trispectrum in single field DBI inflation

Author: Shuntaro Mizuno, Frederico Arroja, Kazuya Koyama, and Takahiro Tanaka
Subjects: Inflation (cosmology), Physics, Cosmology and Gravitation, Nuclear and High Energy Physics, Field (physics), Interaction overview diagram, Scalar (mathematics), Four-momentum, Astrophysics::Cosmology and Extragalactic Astrophysics, Inflaton, General Relativity and Quantum Cosmology, Classical mechanics, Trispectrum, Scalar field, Mathematical physics
Abstract: We compute the tree-level connected four-point function of the primordial curvature perturbation for a fairly general minimally coupled single field inflationary model, where the inflaton’s Lagrangian is a general function of the scalar field and its first derivatives. This model includes K inflation and DBI inflation as particular cases. We show that, at the leading order in the slow-roll expansion and in the small sound speed limit, there are two important tree-level diagrams for the trispectrum. One is a diagram where a scalar mode is exchanged and the other is a diagram where the interaction occurs at a point, i.e. a contact interaction diagram. The scalar exchange contribution is comparable to the contact interaction contribution. For the DBI-inflation model, in the so-called equilateral configuration, the scalar exchange trispectrum is maximized when the angles between the four momentum vectors are equal and in this case the amplitude of the trispectrum from the scalar exchange is 1 order of magnitude higher than the contact interaction trispectrum.
Published: 2009
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18. Lorentz boost and non-Gaussianity in multifield DBI inflation

Author: Frederico Arroja, Takahiro Tanaka, Shuntaro Mizuno, and Kazuya Koyama
Subjects: High Energy Physics - Theory, Inflation (cosmology), Physics, Cosmology and Gravitation, Nuclear and High Energy Physics, Cosmology and Nongalactic Astrophysics (astro-ph.CO), Slow roll, Lorentz transformation, FOS: Physical sciences, General Relativity and Quantum Cosmology (gr-qc), Rest frame, General Relativity and Quantum Cosmology, symbols.namesake, Classical mechanics, High Energy Physics - Theory (hep-th), Brane cosmology, symbols, Trispectrum, Brane, Adiabatic process, Astrophysics - Cosmology and Nongalactic Astrophysics
Abstract: We show that higher-order actions for cosmological perturbations in the multi-field DBI-inflation model are obtained by a Lorentz boost from the rest frame of the brane to the frame where the brane is moving. We confirm that this simple method provides the same third- and fourth- order actions at leading order in slow-roll and in the small sound speed limit as those obtained by the usual ADM formalism. As an application, we compute the leading order connected four-point function of the primordial curvature perturbation coming from the intrinsic fourth-order contact interaction in the multi-field DBI-inflation model. At the third order, the interaction Hamiltonian arises purely by the boost from the second-order action in the rest frame of the brane. The boost acts on the adiabatic and entropy modes in the same way thus there exists a symmetry between the adiabatic and entropy modes. But at fourth order this symmetry is broken due to the intrinsic fourth-order action in the rest frame and the difference between the Lagrangian and the interaction Hamiltonian. Therefore, contrary to the three-point function, the momentum dependence of the purely adiabatic component and the components including the entropic contributions are different in the four-point function. This suggests that the trispectrum can distinguish the multi-field DBI-inflation model from the single field DBI-inflation model., 11 pages, no figures, v2:references added. Accepted for publication in PRD
Published: 2009
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19. Cosmological matching conditions for gravitational waves at second order

Author: Hooshyar Assadullahi, David Wands, Frederico Arroja, and Kazuya Koyama
Subjects: Physics, Tensor contraction, Weyl tensor, Cosmology and Gravitation, Nuclear and High Energy Physics, Cosmology and Nongalactic Astrophysics (astro-ph.CO), Gravitational wave, FOS: Physical sciences, General Relativity and Quantum Cosmology (gr-qc), General Relativity and Quantum Cosmology, symbols.namesake, Exact solutions in general relativity, Hypersurface, Classical mechanics, Lanczos tensor, symbols, Adiabatic process, Tensor density, Astrophysics - Cosmology and Nongalactic Astrophysics
Abstract: We compute the second-order matching conditions for tensor metric perturbations at an abrupt change in the equation of state. For adiabatic perturbations on large scales the matching hypersurface coincides with a uniform-density hypersurface. We show that in the uniform-density gauge both the tensor perturbation and its time-derivative are continuous in this case. For non-adiabatic perturbations, the matching hypersurface need not coincide with a uniform-density hypersurface and the tensor perturbation in the uniform-density gauge may be discontinuous. However, we show that in the Poisson gauge both the tensor perturbation and its time-derivative are continuous for adiabatic or non-adiabatic perturbations. As an application we solve the evolution equation for second-order tensor perturbations on large scales for a constant equation of state and we use the matching conditions to evolve the solutions through the transition from an inflationary era to a radiation era. We show that in the radiation era the resulting free part of the large-scale tensor perturbation (constant mode) is slow-roll suppressed in both the uniform-density and Poisson gauges. Thus, we conclude that second-order gravitational waves from slow-roll inflation are suppressed., Comment: 19 pages, no figures. v2: References and minor comments added. Published version in PRD
Published: 2009
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20. Non-gaussianity from the bispectrum in general multiple field inflation

Author: Frederico Arroja, Shuntaro Mizuno, and Kazuya Koyama
Subjects: High Energy Physics - Theory, Cosmology and Gravitation, FOS: Physical sciences, Curvature perturbation, Kinetic term, General Relativity and Quantum Cosmology (gr-qc), Astrophysics, 01 natural sciences, General Relativity and Quantum Cosmology, Non-Gaussianity, Speed of sound, 0103 physical sciences, Cosmological perturbation theory, Statistical physics, 010306 general physics, Adiabatic process, Entropy (arrow of time), Physics, Inflation (cosmology), 010308 nuclear & particles physics, Astrophysics (astro-ph), Astronomy and Astrophysics, Classical mechanics, High Energy Physics - Theory (hep-th), Bispectrum
Abstract: We study the non-gaussianity from the bispectrum in multi-field inflation models with a general kinetic term. The models include the multi-field K-inflation and the multi-field Dirac-Born-Infeld (DBI) inflation as special cases. We find that, in general, the sound speeds for the adiabatic and entropy perturbations are different and they can be smaller than 1. Then the non-gaussianity can be enhanced. The multi-field DBI-inflation is shown to be a special case where both sound speeds are the same due to a special form of the kinetic term. We derive the exact second and third order actions including metric perturbations. In the small sound speed limit and at leading order in the slow-roll expansion, we derive the three point function for the curvature perturbation which depends on both adiabatic and entropy perturbations. The contribution from the entropy perturbations has a different momentum dependence if the sound speed for the entropy perturbations is different from the adiabatic one, which provides a possibility to distinguish the multi-field models from single field models. On the other hand, in the multi-field DBI case, the contribution from the entropy perturbations has the same momentum dependence as the pure adiabatic contributions and it only changes the amplitude of the three point function. This could help to ease the constraints on the DBI-inflation models., Comment: 16 pages, no figure
Published: 2008
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21. Non-Gaussianity from the trispectrum in general single field inflation

Author: Frederico Arroja and Kazuya Koyama
Subjects: High Energy Physics - Theory, Cosmology and Gravitation, Nuclear and High Energy Physics, FOS: Physical sciences, General Relativity and Quantum Cosmology (gr-qc), Astrophysics::Cosmology and Extragalactic Astrophysics, Astrophysics, Curvature, Kinetic energy, 01 natural sciences, General Relativity and Quantum Cosmology, Cosmology, symbols.namesake, Non-Gaussianity, 0103 physical sciences, 010306 general physics, Mathematical physics, Physics, Slow roll, 010308 nuclear & particles physics, Astrophysics (astro-ph), Inflaton, Classical mechanics, High Energy Physics - Theory (hep-th), symbols, Trispectrum, Hamiltonian (quantum mechanics)
Abstract: We compute the fourth order action in perturbation theory for scalar and second order tensor perturbations for a minimally coupled single field inflationary model, where the inflaton's lagrangian is a general function of the field's value and its kinetic energy. We obtain the fourth order action in two gauges, the comoving gauge and the uniform curvature gauge. Using the comoving gauge action we calculate the trispectrum at leading order in slow-roll, finding agreement with a previously known result in the literature. We point out that in general to obtain the correct leading order trispectrum one cannot ignore second order tensor perturbations as previously done by others. The next-to-leading order corrections may become detectable depending on the shape and we provide the necessary formalism to calculate them., Comment: v2: reference added, typos corrected, replaced to match published version v3: arguments on the full 4th order interaction hamiltonian corrected
Published: 2008
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22. Low energy effective theory on a regularized brane in 6D gauged chiral supergravity

Author: Tsutomu Kobayashi, Frederico Arroja, Tetsuya Shiromizu, and Kazuya Koyama
Subjects: Physics, High Energy Physics - Theory, Cosmology and Gravitation, 010308 nuclear & particles physics, Supergravity, Astrophysics (astro-ph), FOS: Physical sciences, Astronomy and Astrophysics, General Relativity and Quantum Cosmology (gr-qc), Astrophysics, 01 natural sciences, General Relativity and Quantum Cosmology, High Energy Physics - Theory (hep-th), 0103 physical sciences, Brane cosmology, Effective field theory, Dilaton, Brane, 010306 general physics, Scalar field, Effective action, Mathematical physics, Cosmological constant problem
Abstract: We derive the low energy effective theory on a brane in six-dimensional chiral supergravity. The conical 3-brane singularities are resolved by introducing cylindrical codimension one 4-branes whose interiors are capped by a regular spacetime. The effective theory is described by the Brans-Dicke (BD) theory with the BD parameter given by $\omega_{\rm BD}=1/2$. The BD field is originated from a modulus which is associated with the scaling symmetry of the system. If the dilaton potentials on the branes preserve the scaling symmetry, the scalar field has an exponential potential in the Einstein frame. We show that the time dependent solutions driven by the modulus in the four-dimensional effective theory can be lifted up to the six-dimensional exact solutions found in the literature. Based on the effective theory, we discuss a possible way to stabilize the modulus to recover standard cosmology and also study the implication for the cosmological constant problem., Comment: 12 pages, 1 figure
Published: 2007
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23. On the 4D effective theory in warped compactifications with fluxes and branes

Author: Kazuya Koyama, Frederico Arroja, and Kayoko Koyama
Subjects: Physics, High Energy Physics - Theory, Nuclear and High Energy Physics, Compactification (physics), 010308 nuclear & particles physics, Supergravity, FOS: Physical sciences, Equations of motion, 01 natural sciences, Moduli, Classical mechanics, High Energy Physics - Theory (hep-th), 0103 physical sciences, Effective field theory, Brane cosmology, Warped geometry, 010306 general physics, Effective action, Mathematical physics
Abstract: We present a systematic way to derive the four-dimensional effective theories for warped compactifications with fluxes and branes in the ten-dimensional type IIB supergravity. The ten-dimensional equations of motion are solved using the gradient expansion method and the effective four-dimensional equations of motions are derived by imposing the consistency condition that the total derivative terms with respect to the six-dimensional internal coordinates vanish when integrated over the internal manifold. By solving the effective four-dimensional equations, we can find the gravitational backreaction to the warped geometry due to the dynamics of moduli fields, branes and fluxes., 12 pages
Published: 2006

24. Moduli instability in warped compactification - 4D effective theory approach

Author: Frederico Arroja and Kazuya Koyama
Subjects: High Energy Physics - Theory, Physics, Cosmology and Gravitation, Physics and Astronomy (miscellaneous), Compactification (physics), 010308 nuclear & particles physics, FOS: Physical sciences, General Relativity and Quantum Cosmology (gr-qc), 01 natural sciences, General Relativity and Quantum Cosmology, Moduli, Theoretical physics, Exact solutions in general relativity, High Energy Physics - Theory (hep-th), 0103 physical sciences, Effective field theory, Brane cosmology, Warped geometry, Brane, 010306 general physics, Ansatz
Abstract: We consider a 5D BPS dilatonic two brane model which reduces to the Randall-Sundrum model or the Horava-Witten theory for a particular choice of parameters. Recently new dynamical solutions were found by Chen et al., which describe a moduli instability of the warped geometry. Using a 4D effective theory derived by solving the 5D equations of motion, based on the gradient expansion method, we show that the exact solution of Chen et. al. can be reproduced within the 4D effective theory and we identify the origin of the moduli instability. We revisit the gradient expansion method with a new metric ansatz to clarify why the 4D effective theory solution can be lifted back to an exact 5D solution. Finally we argue against a recent claim that the 4D effective theory allows a much wider class of solutions than the 5D theory and provide a way to lift solutions in the 4D effective theory to 5D solutions perturbatively in terms of small velocities of the branes., Comment: 11 pages; v2: typos corrected, comment added in section 5, replaced to match published version
Published: 2006
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25. Living with ghosts in Hořava-Lifshitz gravity

Author: Sabir Ramazanov, Luigi Pilo, Sabino Matarrese, Frederico Arroja, and Marco Celoria
Subjects: High Energy Physics - Theory, Gravity (chemistry), Nuclear and High Energy Physics, Cosmology and Nongalactic Astrophysics (astro-ph.CO), General relativity, Hořava–Lifshitz gravity, Lorentz transformation, Dark matter, FOS: Physical sciences, General Relativity and Quantum Cosmology (gr-qc), 01 natural sciences, General Relativity and Quantum Cosmology, symbols.namesake, Theoretical physics, 0103 physical sciences, Models of Quantum Gravity, 010306 general physics, Gauge symmetry, Physics, 010308 nuclear & particles physics, Cosmology of Theories beyond the SM, Gauge Symmetry, High Energy Physics - Theory (hep-th), symbols, Quantum gravity, False vacuum, Astrophysics - Cosmology and Nongalactic Astrophysics
Abstract: We consider the branch of the projectable Horava-Lifshitz model which exhibits ghost instabilities in the low energy limit. It turns out that, due to the Lorentz violating structure of the model and to the presence of a finite strong coupling scale, the vacuum decay rate into photons is tiny in a wide range of phenomenologically acceptable parameters. The strong coupling scale, understood as a cutoff on ghosts' spatial momenta, can be raised up to $\Lambda \sim 10$ TeV. At lower momenta, the projectable Horava-Lifshitz gravity is equivalent to General Relativity supplemented by a fluid with a small positive sound speed squared ($10^{-42}\lesssim$) $c^2_s \lesssim 10^{-20}$, that could be a promising candidate for the Dark Matter. Despite these advantages, the unavoidable presence of the strong coupling obscures the implementation of the original Horava's proposal on quantum gravity. Apart from the Horava-Lifshitz model, conclusions of the present work hold also for the mimetic matter scenario, where the analogue of the projectability condition is achieved by a non-invertible conformal transformation of the metric., Comment: 33 pages, 1 figure. The proof of an equivalence between the IR limit of the projectable Horava-Lifshitz gravity and the mimetic matter scenario is given in Appendix A. Version accepted for publication in JHEP
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25 results on '"Frederico Arroja"'

1. Planck 2018 results

2. Exploring cosmic origins with CORE: cosmological parameters

3. Exploring Cosmic Origins with CORE:survey requirements and mission design

4. Summary of the Parallel Session: 'Gravitational Waves from the Big Bang and Other Sources'

5. The Two Faces of Mimetic Horndeski Gravity: Disformal Transformations and Lagrange Multiplier

6. Large-scale structure in mimetic Horndeski gravity

7. CMB constraints on running non-Gaussianity

8. Cosmological perturbations in mimetic Horndeski gravity

9. The two faces of mimetic Horndeski gravity: Disformal transformations and Lagrange multiplier

10. On the Trispectrum of Galileon Inflation

11. Strong scale dependent bispectrum in the Starobinsky model of inflation

12. Large and strong scale dependent bispectrum in single field inflation from a sharp feature in the mass

13. A note on the role of the boundary terms for the non-Gaussianity in general k-inflation

14. A note on the equivalence of a barotropic perfect fluid with a K-essence scalar field

15. Full quantum trispectrum in multifield DBI inflation

16. Pathological behaviour of the scalar graviton in Ho\v{r}ava-Lifshitz gravity

17. Full trispectrum in single field DBI inflation

18. Lorentz boost and non-Gaussianity in multifield DBI inflation

19. Cosmological matching conditions for gravitational waves at second order

20. Non-gaussianity from the bispectrum in general multiple field inflation

21. Non-Gaussianity from the trispectrum in general single field inflation

22. Low energy effective theory on a regularized brane in 6D gauged chiral supergravity

23. On the 4D effective theory in warped compactifications with fluxes and branes

24. Moduli instability in warped compactification - 4D effective theory approach

25. Living with ghosts in Hořava-Lifshitz gravity

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25 results on '"Frederico Arroja"'

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