La Radiación Del Fondo Cósmico De Microondas Abstracts
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Analysis and Measurement of Horn Antennas for CMB Experiments
Analysis and Measurement of Horn Antennas for CMB Experiments Ian Mc Auley (M.Sc. B.Sc.) A thesis submitted for the Degree of Doctor of Philosophy Maynooth University Department of Experimental Physics, Maynooth University, National University of Ireland Maynooth, Maynooth, Co. Kildare, Ireland. October 2015 Head of Department Professor J.A. Murphy Research Supervisor Professor J.A. Murphy Abstract In this thesis the author's work on the computational modelling and the experimental measurement of millimetre and sub-millimetre wave horn antennas for Cosmic Microwave Background (CMB) experiments is presented. This computational work particularly concerns the analysis of the multimode channels of the High Frequency Instrument (HFI) of the European Space Agency (ESA) Planck satellite using mode matching techniques to model their farfield beam patterns. To undertake this analysis the existing in-house software was upgraded to address issues associated with the stability of the simulations and to introduce additional functionality through the application of Single Value Decomposition in order to recover the true hybrid eigenfields for complex corrugated waveguide and horn structures. The farfield beam patterns of the two highest frequency channels of HFI (857 GHz and 545 GHz) were computed at a large number of spot frequencies across their operational bands in order to extract the broadband beams. The attributes of the multimode nature of these channels are discussed including the number of propagating modes as a function of frequency. A detailed analysis of the possible effects of manufacturing tolerances of the long corrugated triple horn structures on the farfield beam patterns of the 857 GHz horn antennas is described in the context of the higher than expected sidelobe levels detected in some of the 857 GHz channels during flight. -
A Bayesian Method for Point Source Polarisation Estimation D
A&A 651, A24 (2021) Astronomy https://doi.org/10.1051/0004-6361/202039741 & c ESO 2021 Astrophysics A Bayesian method for point source polarisation estimation D. Herranz1, F. Argüeso2,4, L. Toffolatti3,4, A. Manjón-García1,5, and M. López-Caniego6 1 Instituto de Física de Cantabria, CSIC-UC, Av. de Los Castros s/n, 39005 Santander, Spain e-mail: [email protected] 2 Departamento de Matemáticas, Universidad de Oviedo, C. Federico García Lorca 18, 33007 Oviedo, Spain 3 Departamento de Física, Universidad de Oviedo, C. Federico García Lorca 18, 33007 Oviedo, Spain 4 Instituto Universitario de Ciencias y Tecnologías Espaciales de Asturias (ICTEA), Escuela de Ingeniería de Minas, Materiales y Energía de Oviedo, C. Independencia 13, 33004 Oviedo, Spain 5 Departamento de Física Moderna, Universidad de Cantabria, 39005 Santander, Spain 6 ESAC, Camino Bajo del Castillo s/n, 28692 Villafranca del Castillo, Madrid, Spain Received 22 October 2020 / Accepted 2 March 2021 ABSTRACT The estimation of the polarisation P of extragalactic compact sources in cosmic microwave background (CMB) images is a very important task in order to clean these images for cosmological purposes –for example, to constrain the tensor-to-scalar ratio of primordial fluctuations during inflation– and also to obtain relevant astrophysical information about the compact sources themselves in a frequency range, ν ∼ 10–200 GHz, where observations have only very recently started to become available. In this paper, we propose a Bayesian maximum a posteriori approach estimation scheme which incorporates prior information about the distribution of the polarisation fraction of extragalactic compact sources between 1 and 100 GHz. -
Planck 2015 Results. XII. Full Focal Plane Simulations Planck Collaboration: P
Astronomy & Astrophysics manuscript no. A14˙Simulations c ESO 2016 August 13, 2016 Planck 2015 results. XII. Full Focal Plane simulations Planck Collaboration: P. A. R. Ade87, N. Aghanim60, M. Arnaud75, M. Ashdown71;5, J. Aumont60, C. Baccigalupi86, A. J. Banday95;9, R. B. Barreiro66, J. G. Bartlett1;68, N. Bartolo31;67, E. Battaner97;98, K. Benabed61;94, A. Benoˆıt58, A. Benoit-Levy´ 25;61;94, J.-P. Bernard95;9, M. Bersanelli34;49, P. Bielewicz84;9;86, J. J. Bock68;11, A. Bonaldi69, L. Bonavera66, J. R. Bond8, J. Borrilly14;90, F. R. Bouchet61;89, F. Boulanger60, M. Bucher1, C. Burigana48;32;50, R. C. Butler48, E. Calabrese92, J.-F. Cardoso76;1;61, G. Castex1, A. Catalano77;74, A. Challinor63;71;12, A. Chamballu75;16;60, H. C. Chiang28;6, P. R. Christensen85;37, D. L. Clements56, S. Colombi61;94, L. P. L. Colombo24;68, C. Combet77, F. Couchot73, A. Coulais74, B. P. Crill68;11, A. Curto66;5;71, F. Cuttaia48, L. Danese86, R. D. Davies69, R. J. Davis69, P. de Bernardis33, A. de Rosa48, G. de Zotti45;86, J. Delabrouille1, J.-M. Delouis61;94, F.-X. Desert´ 54, C. Dickinson69, J. M. Diego66, K. Dolag96;81, H. Dole60;59, S. Donzelli49, O. Dore´68;11, M. Douspis60, A. Ducout61;56, X. Dupac39, G. Efstathiou63, F. Elsner25;61;94, T. A. Enßlin81, H. K. Eriksen64, J. Fergusson12, F. Finelli48;50, O. Forni95;9, M. Frailis47, A. A. Fraisse28, E. Franceschi48, A. Frejsel85, S. Galeotta47, S. Galli70, K. Ganga1, T. Ghosh60, M. Giard95;9, Y. Giraud-Heraud´ 1, E. Gjerløw64, J. Gonzalez-Nuevo´ 20;66, K. -
ELIA STEFANO BATTISTELLI Curriculum Vitae
ELIA STEFANO BATTISTELLI Curriculum Vitae Place: Rome, Italy Date: 03/09/2019 Part I – General Information Full Name ELIA STEFANO BATTISTELLI Date of Birth 29/03/1973 Place of Birth Milan, Italy Citizenship Italian Work Address Physics Dep., Sapienza University of Rome, P.le Aldo Moro 5, 00185, Rome, Italy Work Phone Number +39 06 49914462 Home Address Via Romolo Gigliozzi, 173, scala B, 00128, Rome, Italy Mobile Phone Number +39 349 6592825 E-mail [email protected] Spoken Languages Italian (native), English (fluent), Spanish (fluent), French (basic) Part II – Education Type Year Institution Notes (Degree, Experience,..) University graduation 1999 Sapienza University (RM, IT) Physics 1996 University of Leeds, UK Erasmus project Post-graduate studies 2000 SIGRAV (CO, IT) Graduate School in Relativity 2000 INAF (Asiago, VI, IT) Scuola Nazionale Astrofisica 2001 INAF/INFN (FC, IT) Scuola Nazionale Astroparticelle 2004 Società Italiana Fisica (CO, IT) International Fermi School 2006 Princeton University (NJ,USA) Summer School on Gal. Cluster PhD 2004 Sapienza University (RM, IT) PhD in Astronomy (XV cycle) Training Courses 2007 University of British Columbia 40-hours course in precision (BC, CA) machining 2009 Programma Nazionale Ricerche 2 weeks training course for the in Antartide (PNRA) Antarctic activity in remote camps Qualification 2013 Ministero della Pubblica National scientific qualification for Istruzione Associate Professor 2012, SSD 02/C1 (ASN-2012) Part III – Appointments IIIA – Academic Appointments Start End Institution Position 11/2018 present Sapienza University of Rome, Physics Associate Professor;Physics Department Department (Rome, Italy) SSD 02/C1-FIS/05 (Astrophysics) 11/2015 11/2018 Sapienza University of Rome, Physics Tenure track assistant professor Department (Rome, Italy) (Ricercatore a Tempo Determinato RTD- B-type). -
Physics of the Cosmic Microwave Background Anisotropy∗
Physics of the cosmic microwave background anisotropy∗ Martin Bucher Laboratoire APC, Universit´eParis 7/CNRS B^atiment Condorcet, Case 7020 75205 Paris Cedex 13, France [email protected] and Astrophysics and Cosmology Research Unit School of Mathematics, Statistics and Computer Science University of KwaZulu-Natal Durban 4041, South Africa January 20, 2015 Abstract Observations of the cosmic microwave background (CMB), especially of its frequency spectrum and its anisotropies, both in temperature and in polarization, have played a key role in the development of modern cosmology and our understanding of the very early universe. We review the underlying physics of the CMB and how the primordial temperature and polarization anisotropies were imprinted. Possibilities for distinguish- ing competing cosmological models are emphasized. The current status of CMB ex- periments and experimental techniques with an emphasis toward future observations, particularly in polarization, is reviewed. The physics of foreground emissions, especially of polarized dust, is discussed in detail, since this area is likely to become crucial for measurements of the B modes of the CMB polarization at ever greater sensitivity. arXiv:1501.04288v1 [astro-ph.CO] 18 Jan 2015 1This article is to be published also in the book \One Hundred Years of General Relativity: From Genesis and Empirical Foundations to Gravitational Waves, Cosmology and Quantum Gravity," edited by Wei-Tou Ni (World Scientific, Singapore, 2015) as well as in Int. J. Mod. Phys. D (in press). -
The QUIJOTE Experiment: Project Overview and First Results
Highlights of Spanish Astrophysics VIII, Proceedings of the XI Scientific Meeting of the Spanish Astronomical Society held on September 8–12, 2014, in Teruel, Spain. A. J. Cenarro, F. Figueras, C. Hernández-Monteagudo, J. Trujillo Bueno, and L. Valdivielso (eds.) The QUIJOTE experiment: project overview and first results R. G´enova-Santos1;6, J. A. Rubi~no-Mart´ın1;6, R. Rebolo1;6;7, M. Aguiar1, F. G´omez-Re~nasco1, C. Guti´errez1;6, R. J. Hoyland1, C. L´opez-Caraballo1;6;8, A. E. Pel´aez-Santos1;6, M. R. P´erez-de-Taoro1, F. Poidevin1;6 , V. S´anchez de la Rosa1, D. Tramonte1;6, A. Vega-Moreno1, T. Viera-Curbelo1, R. Vignaga1;6, E. Mart´ınez-Gonz´alez2, R. B. Barreiro2, B. Casaponsa2, F. J. Casas2, J. M. Diego2, R. Fern´andez-Cobos2, D. Herranz2, M. L´opez-Caniego2, D. Ortiz2, P. Vielva2, E. Artal3, B. Aja3, J. Cagigas3, J. L. Cano3, L. de la Fuente3, A. Mediavilla3, J. V. Ter´an3, E. Villa3, L. Piccirillo4, R. Davies4, R. J. Davis4, C. Dickinson4, K. Grainge4, S. Harper4, B. Maffei4, M. McCulloch4, S. Melhuish4, G. Pisano4, R. A. Watson4, A. Lasenby5;9, M. Ashdown5;9, M. Hobson5, Y. Perrott5, N. Razavi-Ghods5, R. Saunders6, D. Titterington6 and P. Scott6 1 Instituto de Astrofis´ıcade Canarias, 38200 La Laguna, Tenerife, Canary Islands, Spain 2 Instituto de F´ısicade Cantabria (CSIC-Universidad de Cantabria), Avda. de los Castros s/n, 39005 Santander, Spain 3 Departamento de Ingenieria de COMunicaciones (DICOM), Laboratorios de I+D de Telecomunicaciones, Universidad de Cantabria, Plaza de la Ciencia s/n, E-39005 Santander, Spain 4 Jodrell Bank Centre for Astrophysics, Alan Turing Building, School of Physics and Astronomy, The University of Manchester, Oxford Road, Manchester, M13 9PL, U.K 5 Astrophysics Group, Cavendish Laboratory, University of Cambridge, J.J. -
Implicaciones Cosmológicas De Las
DEPARTAMENTO DE F´ISICAMODERNA INSTITUTODEF´ISICA DE CANTABRIA UNIVERSIDAD DE CANTABRIA IFCA (UC-CSIC) IMPLICACIONES COSMOLOGICAS´ DE LAS ANISOTROP´IAS DE TEMPERATURA Y POLARIZACION´ DE LA RFCM Y LA ESTRUCTURA A GRAN ESCALA DEL UNIVERSO Memoria presentada para optar al t´ıtulo de Doctor otorgado por la Universidad de Cantabria por Ra´ul Fern´andez Cobos Declaraci´on de Autor´ıa Patricio Vielva Mart´ınez, Doctor en Ciencias F´ısicas y Profesor Contratado Doctor de la Universidad de Cantabria y Enrique Mart´ınez Gonz´alez, Doctor en Ciencias F´ısicas y Profesor de Investigaci´on del Consejo Superior de Investigaciones Cient´ıficas, CERTIFICAN que la presente memoria Implicaciones cosmol´ogicas de las anisotrop´ıas de temperatura y polarizaci´on de la RFCM y la estructura a gran escala del universo ha sido realizada por Ra´ul Fern´andez Cobos bajo nuestra direcci´on en el Instituto de F´ısica de Cantabria, para optar al t´ıtulo de Doctor por la Universidad de Cantabria. Consideramos que esta memoria contiene aportaciones cient´ıficas suficientemente rele- vantes como para constituir la Tesis Doctoral del interesado. En Santander, a 19 de septiembre de 2014, Patricio Vielva Mart´ınez Enrique Mart´ınez Gonz´alez A mis padres. Creo que seremos inmortales, que sembraremos las estrellas y viviremos eternamente en la carne de nuestros hijos. Ray Bradbury. Agradecimientos La realizaci´on de esta tesis doctoral ha servido de excusa para llevar a cabo un proyecto mucho m´as amplio, que se ha saldado con unos a˜nos de impagable crecimiento personal y del que estas p´aginas constituyen solo la peque˜na parte tangible. -
Optimal Reconstruction of Cosmological Density Fields by Benjamin A. Horowitz a Dissertation Submitted in Partial Satisfaction O
Optimal Reconstruction of Cosmological Density Fields By Benjamin A. Horowitz Adissertationsubmittedinpartialsatisfactionofthe requirements for the degree of Doctor of Philosophy in Physics in the Graduate Division of the University of California, Berkeley Committee in charge: Professor Uros Seljak, Chair Professor Aaron Parson Professor Martin White Fall 2019 Optimal Reconstruction of Cosmological Density Fields Copyright 2019 by Benjamin A. Horowitz 1 Abstract Optimal Reconstruction of Cosmological Density Fields by Benjamin A. Horowitz Doctor of Philosophy in Physics University of California, Berkeley Professor Uros Seljak, Chair Akeyobjectiveofmoderncosmologyistodeterminethecompositionanddistributionof matter in the universe. While current observations seem to match the standard cosmological model with remarkable precision, there remains tensions between observations as well as mysteries relating to the true nature of dark matter and dark energy. Despite the recent in- creased availability of cosmological data across a wide redshift, these tensions have remained or been further worsened. With the explosion of astronomical data in the coming decade, it has become increasingly critical to extract the maximum possible amount of information available across all available scales. As the available volume for analysis increases, we are no longer sample variance limited and existing summary statistics (as well as related estima- tors) need to be re-examined. Fortunately, parallel with the construction of these surveys there is significant development in the computational techniques used to analyze that data. Algorithmic developments over the past decade and expansion of computational resources allow large cosmological simulations to be run with relative simplicity and parallel theoretical developments motivate increased interest in recovering the underlying large scale structure of the universe beyond the power spectra. -
A Bit of History Satellites Balloons Ground-Based
Experimental Landscape ● A Bit of History ● Satellites ● Balloons ● Ground-Based Ground-Based Experiments There have been many: ABS, ACBAR, ACME, ACT, AMI, AMiBA, APEX, ATCA, BEAST, BICEP[2|3]/Keck, BIMA, CAPMAP, CAT, CBI, CLASS, COBRA, COSMOSOMAS, DASI, MAT, MUSTANG, OVRO, Penzias & Wilson, etc., PIQUE, Polatron, Polarbear, Python, QUaD, QUBIC, QUIET, QUIJOTE, Saskatoon, SP94, SPT, SuZIE, SZA, Tenerife, VSA, White Dish & more! QUAD 2017-11-17 Ganga/Experimental Landscape 2/33 Balloons There have been a number: 19 GHz Survey, Archeops, ARGO, ARCADE, BOOMERanG, EBEX, FIRS, MAX, MAXIMA, MSAM, PIPER, QMAP, Spider, TopHat, & more! BOOMERANG 2017-11-17 Ganga/Experimental Landscape 3/33 Satellites There have been 4 (or 5?): Relikt, COBE, WMAP, Planck (+IRTS!) Planck 2017-11-17 Ganga/Experimental Landscape 4/33 Rockets & Airplanes For example, COBRA, Berkeley-Nagoya Excess, U2 Anisotropy Measurements & others... It’s difficult to get integration time on these platforms, so while they are still used in the infrared, they are no longer often used for the http://aether.lbl.gov/www/projects/U2/ CMB. 2017-11-17 Ganga/Experimental Landscape 5/33 (from R. Stompor) Radek Stompor http://litebird.jp/eng/ 2017-11-17 Ganga/Experimental Landscape 6/33 Other Satellite Possibilities ● US “CMB Probe” ● CORE-like – Studying two possibilities – Discussions ongoing ● Imager with India/ISRO & others ● Spectrophotometer – Could include imager – Inputs being prepared for AND low-angular- the Decadal Process resolution spectrophotometer? https://zzz.physics.umn.edu/ipsig/ -
The Effect of a Scanning Flat Fold Mirror on a CMB B-Mode Experiment
The effect of a scanning flat fold mirror on a CMB B-mode experiment William F. Grainger, Chris E. North, Peter. A. R. Ade Astronomy Instrumentation Group, Cardiff University. (Dated: November 19, 2018) We investigate the possibility of using a flat-fold beam steering mirror for a CMB B-mode exper- iment. An aluminium flat-fold mirror is found to add ∼0.075% polarization, which varies in a scan synchronous way. Time-domain simulations of a realistic scanning pattern are performed, and the effect on the power-spectrum illustrated and a possible method of correction applied. I. INTRODUCTION a fiducal scan strategy and simulation pipeline. Results from this pipeline are then presented and discussed, along with other potential problems in Section IV. The prevailing ΛCDM cosmological model has been very successful in explaining many observations of the universe. However, inflation - exponential expansion II. METHOD within the first 10−35 s - has many uncertain details; indeed it lacks strong∼ confirmation. Inflationary models predict a background of gravity waves [1, 9, 20, 22, 23] For this investigation, we consider a horn fed receiver which produce a curl-like, or “B-mode” pattern of po- and compact range antenna (CRA), placed in a ground- larization on the cosmic microwave background (CMB) screen, nominally observing the horizon. The output on scales greater than 1◦, which cannot be produced by beam of the CRA is then steered to the sky with a single, density perturbations [11, 25]. The amplitude of this sig- flat, fold mirror. Although the flat mirror would be large; 4 4 m, such a system can be considered. -
The Thirty Gigahertz Instrument Receiver for the Q-U-I Joint Tenerife Experiment: Concept and Experimental Results Enrique Villa,1,A) Juan L
REVIEW OF SCIENTIFIC INSTRUMENTS 86, 024702 (2015) The thirty gigahertz instrument receiver for the Q-U-I Joint Tenerife experiment: Concept and experimental results Enrique Villa,1,a) Juan L. Cano,1 Jaime Cagigas,1 David Ortiz,2 Francisco J. Casas,2 Ana R. Pérez,1 Beatriz Aja,1 J. Vicente Terán,1 Luisa de la Fuente,1 Eduardo Artal,1 Roger Hoyland,3 and Ángel Mediavilla1 1Departamento Ingeniería de Comunicaciones, Universidad de Cantabria, Plaza de la Ciencia s/n, Santander 39005, Spain 2Instituto de Física de Cantabria, Avda. Los Castros s/n, Santander 39005, Spain 3Instituto de Astrofísica de Canarias, Vía Láctea s/n, La Laguna 38205, Spain (Received 12 December 2014; accepted 19 January 2015; published online 4 February 2015) This paper presents the analysis, design, and characterization of the thirty gigahertz instrument receiver developed for the Q-U-I Joint Tenerife experiment. The receiver is aimed to obtain polarization data of the cosmic microwave background radiation from the sky, obtaining the Q, U, and I Stokes parameters of the incoming signal simultaneously. A comprehensive analysis of the theory behind the proposed receiver is presented for a linearly polarized input signal, and the functionality tests have demonstrated adequate results in terms of Stokes parameters, which validate the concept of the receiver based on electronic phase switching. C 2015 AIP Publishing LLC. [http://dx.doi.org/10.1063/1.4907015] I. INTRODUCTION the moment right after the Big Bang.6 Among ground-based projects, QUIET7 and FARADAY8 have developed sensitive The Cosmic Microwave Background (CMB) is the ther- radiometers based on the schemes of previous receivers per- mal radiation from the Big Bang explosion, which fills the forming high-quality sky maps. -
The Large Scale Polarization Explorer (LSPE) for CMB Measurements: Performance Forecast
Prepared for submission to JCAP The large scale polarization explorer (LSPE) for CMB measurements: performance forecast The LSPE collaboration G. Addamo,a P. A. R. Ade,b C. Baccigalupi,c A. M. Baldini,d P. M. Battaglia,e E. S. Battistelli, f;g A. Baù,h P. de Bernardis, f;g M. Bersanelli,i; j M. Biasotti,k;l A. Boscaleri,m B. Caccianiga, j S. Caprioli,i; j F. Cavaliere,i; j F. Cei, f;n K. A. Cleary,o F. Columbro, f;g G. Coppi,p A. Coppolecchia, f;g F. Cuttaia,q G. D’Alessandro, f;g G. De Gasperis,r;s M. De Petris, f;g V. Fafone,r;s F. Farsian,c L. Ferrari Barusso,k;l F. Fontanelli,k;l C. Franceschet,i; j T.C. Gaier,u L. Galli,d F. Gatti,k;l R. Genova-Santos,t;v M. Gerbino,D;C M. Gervasi,h;w T. Ghigna,x D. Grosso,k;l A. Gruppuso,q;H R. Gualtieri,G F. Incardona,i; j M. E. Jones,x P. Kangaslahti,o N. Krachmalnicoff,c L. Lamagna, f;g M. Lattanzi,D;C M. Lumia,a R. Mainini,h D. Maino,i; j S. Mandelli,i; j M. Maris,y S. Masi, f;g S. Matarrese,z A. May,A L. Mele, f;g P. Mena,B A. Mennella,i; j R. Molina,B D. Molinari,q;E;C;D G. Morgante,q U. Natale,C;D F. Nati,h P. Natoli,C;D L. Pagano,C;D A. Paiella, f;g F.