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Showing papers by "D. Santos published in 2010"


Journal ArticleDOI
J. A. Tauber1, Nazzareno Mandolesi2, J.-L. Puget3, T. Banos4  +499 moreInstitutions (61)
TL;DR: The European Space Agency's Planck satellite, launched on 14 May 2009, is the third-generation space experiment in the field of cosmic microwave background (CMB) research as mentioned in this paper.
Abstract: The European Space Agency's Planck satellite, launched on 14 May 2009, is the third-generation space experiment in the field of cosmic microwave background (CMB) research. It will image the anisotropies of the CMB over the whole sky, with unprecedented sensitivity ( ~ 2 × 10-6) and angular resolution (~5 arcmin). Planck will provide a major source of information relevant to many fundamental cosmological problems and will test current theories of the early evolution of the Universe and the origin of structure. It will also address a wide range of areas of astrophysical research related to the Milky Way as well as external galaxies and clusters of galaxies. The ability of Planck to measure polarization across a wide frequency range (30-350 GHz), with high precision and accuracy, and over the whole sky, will provide unique insight, not only into specific cosmological questions, but also into the properties of the interstellar medium. This paper is part of a series which describes the technical capabilities of the Planck scientific payload. It is based on the knowledge gathered during the on-ground calibration campaigns of the major subsystems, principally its telescope and its two scientific instruments, and of tests at fully integrated satellite level. It represents the best estimate before launch of the technical performance that the satellite and its payload will achieve in flight. In this paper, we summarise the main elements of the payload performance, which is described in detail in the accompanying papers. In addition, we describe the satellite performance elements which are most relevant for science, and provide an overview of the plans for scientific operations and data analysis.

342 citations


Journal ArticleDOI
TL;DR: The High Frequency Instrument (HFI) is one of the two focal instruments of the Planck mission as discussed by the authors, which is designed to measure the cosmic microwave background (CMB) with a sensitivity limited only by fundamental sources: the photon noise of the CMB itself and the residuals left after the removal of foregrounds.
Abstract: Context. The High Frequency Instrument (HFI) is one of the two focal instruments of the Planck mission. It will observe the whole sky in six bands in the 100 GHz-1 THz range. Aims: The HFI instrument is designed to measure the cosmic microwave background (CMB) with a sensitivity limited only by fundamental sources: the photon noise of the CMB itself and the residuals left after the removal of foregrounds. The two high frequency bands will provide full maps of the submillimetre sky, featuring mainly extended and point source foregrounds. Systematic effects must be kept at negligible levels or accurately monitored so that the signal can be corrected. This paper describes the HFI design and its characteristics deduced from ground tests and calibration. Methods: The HFI instrumental concept and architecture are feasible only by pushing new techniques to their extreme capabilities, mainly: (i) bolometers working at 100 mK and absorbing the radiation in grids; (ii) a dilution cooler providing 100 mK in microgravity conditions; (iii) a new type of AC biased readout electronics and (iv) optical channels using devices inspired from radio and infrared techniques. Results: The Planck-HFI instrument performance exceeds requirements for sensitivity and control of systematic effects. During ground-based calibration and tests, it was measured at instrument and system levels to be close to or better than the goal specification.

297 citations


Journal ArticleDOI
S. P. Ahlen1, Niayesh Afshordi2, Niayesh Afshordi3, James Battat4, J. Billard5, Nassim Bozorgnia6, S. Burgos7, T. Caldwell8, T. Caldwell4, J. M. Carmona9, S. Cebrián9, P. Colas, T. Dafni9, E. J. Daw10, D. Dujmic4, A. Dushkin11, William Fedus4, Efrain J. Ferrer, D. Finkbeiner12, Peter H. Fisher4, J. Forbes7, T. Fusayasu13, J. Galán9, T. Gamble10, C. Ghag14, Ioannis Giomataris, Michael Gold15, Haley Louise Gomez9, M. E. Gomez16, Paolo Gondolo17, Anne M. Green18, C. Grignon5, O. Guillaudin5, C. Hagemann15, Kaori Hattori19, Shawn Wesley Henderson4, N. Higashi19, C. Ida19, F.J. Iguaz9, Andrew Inglis1, I. G. Irastorza9, Satoru Iwaki19, A. C. Kaboth4, Shigeto Kabuki19, J. Kadyk20, Nitya Kallivayalil4, H. Kubo19, Shunsuke Kurosawa19, V. A. Kudryavtsev10, T. Lamy5, Richard C. Lanza4, T. B. Lawson10, A. Lee4, E. R. Lee15, T. Lin12, D. Loomba15, Jeremy Lopez4, G. Luzón9, T. Manobu, J. Martoff21, F. Mayet5, B. Mccluskey10, E. H. Miller15, Kentaro Miuchi19, Jocelyn Monroe4, B. Morgan22, D. Muna23, A. St. J. Murphy14, Tatsuhiro Naka24, K. Nakamura19, M. Nakamura24, T. Nakano24, G.G. Nicklin10, H. Nishimura19, K. Niwa24, Sean Paling10, Joseph D. Parker19, A. Petkov7, M. Pipe10, K. Pushkin7, Matthew R. Robinson10, Arturo Rodriguez Rodriguez9, Jose Rodríguez-Quintero16, T. Sahin4, Robyn E. Sanderson4, N. Sanghi15, D. Santos5, O. Sato24, Tatsuya Sawano19, G. Sciolla4, Hiroyuki Sekiya25, Tracy R. Slatyer12, D. P. Snowden-Ifft7, N. J. C. Spooner10, A. Sugiyama26, A. Takada, M. Takahashi19, A. Takeda25, Toru Tanimori19, Kojiro Taniue19, A. Tomás9, H. Tomita1, K. Tsuchiya19, J. Turk15, E. Tziaferi10, K. Ueno19, S. E. Vahsen20, R. Vanderspek4, J D Vergados27, J.A. Villar9, H. Wellenstein11, I. Wolfe4, R. K. Yamamoto4, H. Yegoryan4 
TL;DR: The case for a dark matter detector with directional sensitivity was presented at the 2009 CYGNUS workshop on directional dark matter detection, and contributions from theorists and experimental groups in the field as mentioned in this paper.
Abstract: We present the case for a dark matter detector with directional sensitivity. This document was developed at the 2009 CYGNUS workshop on directional dark matter detection, and contains contributions from theorists and experimental groups in the field. We describe the need for a dark matter detector with directional sensitivity; each directional dark matter experiment presents their project's status; and we close with a feasibility study for scaling up to a one ton directional detector, which would cost around $150M.

224 citations


Journal ArticleDOI
TL;DR: In this article, a coherent model of the polarized Galactic synchrotron and thermal dust emissions is presented for the measurement of polarized power spectra of the CMB fluctuations with the Planck satellite mission.
Abstract: We present for the first time a coherent model of the polarized Galactic synchrotron and thermal dust emissions which are the main diffuse foreground for the measurement of the polarized power spectra of the CMB fluctuations with the Planck satellite mission. We produce 3D models of the Galactic magnetic field including regular and turbulent components, and of the distribution of matter in the Galaxy, relativistic electrons and dust grains. By integrating along the line of sight we construct maps of the polarized Galactic synchrotron and thermal dust emission for each of these models and compare them to currently available data. We consider the 408 MHz all-sky continuum survey, the 23 GHz band of the Wilkinson Microwave Anisotropy Probe and the 353 GHz Archeops data.}{The best-fit parameters obtained are consistent with previous estimates in the literature based only on synchrotron emission and pulsar rotation measurements. They allows us to reproduce the large scale structures observed on the data. Poorly understood local Galactic structures and turbulence make difficult an accurate reconstruction of the observations in the Galactic plane. Finally, using the best-fit model we are able to estimate the expected polarized foreground contamination at the Planck frequency bands. For the CMB bands, 70, 100, 143 and 217 GHz, at high Galactic latitudes although the CMB signal dominates in general, a significant foreground contribution is expected at large angular scales. In particular, this contribution will dominate the CMB signal for the B modes expected from realistic models of a background of primordial gravitational waves.

6 citations