Observation and Data Analysis Activityin SPOrt and BaR-SPOrt Exp.s Ettore Carretti Bologna 7-9 January 2004.

Slides:



Advertisements
Similar presentations
Observation of the Universe from the Moon – Elisabetta Cavazzuti – LNF May 7, 2007 ITALIAN VISION FOR MOON EXPLORATION OBSERVATION OF THE UNIVERSE FROM.
Advertisements

QUIET Q/U Imaging ExperimenT Osamu Tajima (KEK) QUIET collaboration 1.
ESO Recent Results on Reionization Chris Carilli (NRAO) LANL Cosmology School, July 2011 Review: constraints on IGM during reionization  CMB large scale.
Planck 2013 results, implications for cosmology
S-PASS, a new view of the polarized sky Gianni Bernardi SKA SA On behalf of the S-PASS team CMB2013, Okinawa, June th 2013.
Foreground cleaning in CMB experiments Carlo Baccigalupi, SISSA, Trieste.
WMAP observations: Foreground Emission Adric Riedel
Cleaned Three-Year WMAP CMB Map: Magnitude of the Quadrupole and Alignment of Large Scale Modes Chan-Gyung Park, Changbom Park (KIAS), J. Richard Gott.
Systematic effects in cosmic microwave background polarization and power spectrum estimation SKA 2010 Postgraduate Bursary Conference, Stellenbosch Institute.
Removing foregrounds from CMB maps using non-Gaussianity measurement Dr. Rajib Saha Assistant Professor Physics Department IISER Bhopal INDO-UK Scientific.
Cosmology topics, collaborations BOOMERanG, Cosmic Microwave Background LARES (LAser RElativity Satellite), General Relativity and extensions, Lense-Thirring.
Distinguishing Primordial B Modes from Lensing Section 5: F. Finelli, A. Lewis, M. Bucher, A. Balbi, V. Aquaviva, J. Diego, F. Stivoli Abstract:” If the.
WMAP. The Wilkinson Microwave Anisotropy Probe was designed to measure the CMB. –Launched in 2001 –Ended 2010 Microwave antenna includes five frequency.
Component Separation of Polarized Data Application to PLANCK Jonathan Aumont J-F. Macías-Pérez, M. Tristram, D. Santos
Zeldovich-Sakharov program at RATAN-600 “Cosmological Gene” project Ground based support of the Space CMB Missions Y.Parijskij et al Special Astrophysical.
The Cosmic Microwave Background. Maxima DASI WMAP.
Observations of anomalous dust emission (AME) with AMI
N. Ponthieu Polarization workshop, IAS, Orsay, 09/15/ N. Ponthieu (IAS) The conquest of sky polarization The upper limits era First detections Prospects.
Fifty Years of CMB Anisotropy Experiments (and Theory) ….in 15 Minutes Bruce Partridge Haverford College
Physics 133: Extragalactic Astronomy and Cosmology Lecture 14; March
Separating Cosmological B-Modes with FastICA Stivoli F. Baccigalupi C. Maino D. Stompor R. Orsay – 15/09/2005.
Simulating the Interferometer In order to simulate the performance of an interferometer, 20 by 20 degree sections were extracted from the simulated CMB.
WMAP and Polarization APS February 16, 2010 In remembrance of Andrew Lange L. Page.
Seeing the universe through redshifted 21-cm radiation Somnath Bharadwaj Physics & CTS IIT Kharagpur.
P olarized R adiation I maging and S pectroscopy M ission Probing cosmic structures and radiation with the ultimate polarimetric spectro-imaging of the.
The Implication of BICEP2 : Alternative Interpretations on its results Seokcheon Lee SNU Seminar Apr. 10 th
PHY306 1 Modern cosmology 4: The cosmic microwave background Expectations Experiments: from COBE to Planck  COBE  ground-based experiments  WMAP  Planck.
130 cMpc ~ 1 o z~ = 7.3 Lidz et al ‘Inverse’ views of evolution of large scale structure during reionization Neutral intergalactic medium via HI.
130 cMpc ~ 1 o z = 7.3 Lidz et al ‘Inverse’ views of evolution of large scale structure during reionization Neutral intergalactic medium via HI 21cm.
Polarization Surveys with the DRAO 26-m Telescope at 1.4 GHz Maik Wolleben, T. Landecker, O. Davison Dominion Radio Astrophysical Observatory W. Reich,
ASIAA NTU PHYS J.H.P.Wu & AMiBA Team To remove the ground pickup and electronic DC component in the data, we tracked the source- (P1) and tail- (P2) patches.
CMB & Foreground Polarisation CMB 2003 Workshop, Minneapolis Carlo Baccigalupi, SISSA/ISAS.
CMB observations and results Dmitry Pogosyan University of Alberta Lake Louise, February, 2003 Lecture 1: What can Cosmic Microwave Background tell us.
Constraints on the neutrino mass by future precise CMB polarization and 21cm line observations Yoshihiko Oyama The Graduate University for Advanced Studies.
US Planck Data Analysis Review 1 Christopher CantalupoUS Planck Data Analysis Review 9–10 May 2006 CTP Working Group Presented by Christopher Cantalupo.
Science with a Rover-based Low-frequency Dipole Array A multi-configuration rover-borne dipole array for Low-frequency RadioAstronomy from the Moon Ettore.
21 cm Reionization Forecast and Search at GMRT
Low Frequency Background and Cosmology Xuelei Chen National Astronomical Observatories Kashigar, September 10th 2005.
MAPping the Universe ►Introduction: the birth of a new cosmology ►The cosmic microwave background ►Measuring the CMB ►Results from WMAP ►The future of.
Cosmic Microwave Background Carlo Baccigalupi, SISSA CMB lectures at TRR33, see the complete program at darkuniverse.uni-hd.de/view/Main/WinterSchoolLecture5.
Joint analysis of Archeops and WMAP observations of the CMB G. Patanchon (University of British Columbia) for the Archeops collaboration.
Galactic Radioemission – a problem for precision cosmology ? Absolute Temperatures at Short CM-Waves with a Lunar Radio Telescope Wolfgang Reich Max-Planck-Institut.
PHY306 1 Modern cosmology 4: The cosmic microwave background Expectations Experiments: from COBE to Planck  COBE  ground-based experiments  WMAP  Planck.
First Result of Urumqi 6cm Polarization Observations: Xiaohui Sun, Wolfgang Reich JinLin Han, Patricia Reich, Richard Wielebinski Partner Group of MPIfR.
Cosmic Microwave Background Carlo Baccigalupi, SISSA CMB lectures at TRR33, see the complete program at darkuniverse.uni-hd.de/view/Main/WinterSchoolLecture5.
The measurement of q 0 If objects are observed at large distances of known brightness (standard candles), we can measure the amount of deceleration since.
Anomalies of low multipoles of WMAP
Cosmic Microwave Background Carlo Baccigalupi, SISSA CMB lectures at TRR33, see the complete program at darkuniverse.uni-hd.de/view/Main/WinterSchoolLecture5.
Primordial fluctuations 20  Isotropic 3K background. The most perfect blackbody we know Dipole (3.4 mK). Our motion relative to CMB.
EBEx foregrounds and band optimization Carlo Baccigalupi, Radek Stompor.
Experimental Cosmology Group Oxford Astrophysics Overview CLOVER is a UK-led experiment to detect the B-mode polarisation of the Cosmic Microwave Background.
The Planck Satellite Hannu Kurki-Suonio University of Helsinki Finnish-Japanese Workshop on Particle Cosmology, Helsinki
Planck Report on the status of the mission Carlo Baccigalupi, SISSA.
2-Day IDAPP meeting INAF-IASF Bologna Student: Pietro Procopio Dr. Carlo Burigana University of Ferrara Dr. Nazzareno Mandolesi Internal tutor: External.
Blind Component Separation for Polarized Obseravations of the CMB Jonathan Aumont, Juan-Francisco Macias-Perez Rencontres de Moriond 2006 La.
Observations of Near Infrared Extragalactic Background (NIREBL) ISAS/JAXAT. Matsumoto Dec.2-5, 2003 Japan/Italy seminar at Niigata Univ.
FIRST LIGHT A selection of future facilities relevant to the formation and evolution of galaxies Wavelength Sensitivity Spatial resolution.
Big Bang f(HI) ~ 0 f(HI) ~ 1 f(HI) ~ History of Baryons (mostly hydrogen) Redshift Recombination Reionization z = 1000 (0.4Myr) z = 0 (13.6Gyr) z.
Reionization science from the CMB after Planck Michael Mortonson University of Chicago July 2, 2009.
Cosmic Microwave Background Carlo Baccigalupi, SISSA CMB lectures at TRR33, see the complete program at darkuniverse.uni-hd.de/view/Main/WinterSchoolLecture5.
BICEP2 Results & Its Implication on inflation models and Cosmology Seokcheon Lee 48 th Workshop on Gravitation & NR May. 16 th
The cross-correlation between CMB and 21-cm fluctuations during the epoch of reionization Hiroyuki Tashiro N. Aghanim (IAS, Paris-sud Univ.) M. Langer.
PLANCK TEAM of the DISCOVERY Center. The most mysterious problems.
Planck working group 2.1 diffuse component separation review Paris november 2005.
Cosmic Microwave Background
Nicolas Fagnoni – Cosmology on Safari – 14th February 2017
Towards the first detection using SPT polarisation
12th Marcel Grossman Meeting,
Precision cosmology, status and perspectives
Recovery of The Signal from the Epoch of Reionization
Presentation transcript:

Observation and Data Analysis Activityin SPOrt and BaR-SPOrt Exp.s Ettore Carretti Bologna 7-9 January 2004

The Science Context Most of information we have about formation, evolution and destiny of the Universe come from investigations of the Cosmic Microwave Background (CMB) –Anisotropy –Polarization –Spectrum CMB photons had last interaction with free electrons about years after the Big Bang. They are then carrying the picture of an Universe times younger, 1000 times hotter and 10 9 times denser than today. Statistic properties of such a picture are determined by the plasma physics pre- recombination (acoustic oscillations), by the physics of the early universe (early fluctuations spectrum) and both by the expansion and the geometry of the universe on large scales. This picture represents the only straight way to investigate the Early Universe and it allows to study its properties Billion years

Why observing CMBP ? Polarization Anisotropy The polarized component of the CMB provides new information on: Large angular scales (10°-20°): can disantangle models with different  better than the anisotropy Large angular scales (10°-20°): can disantangle models with different  better than the anisotropy Small angular scales (0.2°-0.4°): can provide confirmation of the inflationary frame. Small angular scales (0.2°-0.4°): can provide confirmation of the inflationary frame. E-mode peaks correspond to anisotropy minima and viceversa. DASI, WMAP.

Activity in Radio/MW Polarization week The CMBP signal is week (few uK for the E-mode; < 0.3uK for the B-Mode) and calls for: I.Experiment Design Analysis I.Experiment Design Analysis to take instrumental errors under control; II.Data Analysis II.Data Analysis to –Remove residual systematic effects; –Extract relevant scientific information. –Galactic foreground emission study (Synchrotron); III. low Synchrotron emission regions (BaR-SPOrt); III. Identification of low Synchrotron emission regions (BaR-SPOrt); IV. Calibration IV. Identification of Calibration sources; V.Theoretical studies V.Theoretical studies of the relevant astrophysics: Galaxy and CMBP.

Activity in Radio/MW Polarization: People Bernardi GianniDottorando Carretti EttoreRicercatore Casarini LucianoDottorando Cecchini StefanoI Ricercatore Cortiglioni StefanoRicercatore Macculi ClaudioAssegno di Ric. Sbarra CarlaRicercatore ex Art. 23 Sezione di Bologna IRAUNI MI-BicoccaUNI FIRENZEATNF-CSIROMPI-fR BonnIEIIT-CNR

I. Design Analysis Experiment Design Analysis Experiment Design Analysis to take instrumental errors under control: instrumental effectsAnalysis of instrumental effects on data (antenna correlation, thermal effects, …..). Definition of SpecsDefinition of Specs for all components of the system to take systematics under control w.r.t. the wanted signal (CMBP) Instrument clean enough to match data reduction software requirements Carretti E. et al. (2001) NewA, 6, 173 Carretti E. et al. (2004) submitted to A&A

I. Design Analysis (2) Carretti E. et al. (2004) submitted to A&A

II. Data Analysis: Destriping Data AnalysisData Analysis to –Remove residual systematic effects; –Extract relevant scientific information Instabilities on time scales larger than the signal modulation period generate stripes on the map: Destriping software. fast iterative version Sbarra C. et al. (2003) A&A, 401, 1215 before….after destriping

Data Analysis (2) Cosmological parameter extraction for the forthcoming experiments SPOrt and BaR-SPOrt (e.g. optical depth  ): in progress.Cosmological parameter extraction for the forthcoming experiments SPOrt and BaR-SPOrt (e.g. optical depth  ): in progress. Measurements of Foreground properties: Angular Power Spectra of synchrotron emissionMeasurements of Foreground properties: Angular Power Spectra of synchrotron emission Galactic Foreground Separation from CMBP signalGalactic Foreground Separation from CMBP signal Tucci M. et al. (2000) NewA, 5, 181 Bruscoli M. et al. (2002) NewA, 7, 171 Power Spectra of Galactic synchrotron extrapolated to 60 and 90 GHz and compared to CMBP E-ModePower Spectra of Galactic synchrotron extrapolated to 60 and 90 GHz and compared to CMBP E-Mode

Frequency 32 GHz  GHz  GHz  0.02 About 100 times lower than the CMBP signal III. Observations of Low Emission Areas: the BOOMERanG 1.4 GHz Selected target! No polarization Observations in low Galactic emission region existed;No polarization Observations in low Galactic emission region existed; First detection of diffuse signal at a so low emission level (ATCA-ATNF).First detection of diffuse signal at a so low emission level (ATCA-ATNF). Mean Emission is found to be: I p ~ 11.6 mKMean Emission is found to be: I p ~ 11.6 mK Extrapolations are promising for CMBPExtrapolations are promising for CMBP Bernardi et al., ApJL, 594, L5, astro-ph/

Activity of observation of low polarized synchrotron emission areas: Observations of the BOOMERanG patch at 2.3 and 5 GHz (already performed in June 2003 and December 2003);Observations of the BOOMERanG patch at 2.3 and 5 GHz (already performed in June 2003 and December 2003); Observations of the DASI patch at 1.4 GHz (already performed in July 2003)Observations of the DASI patch at 1.4 GHz (already performed in July 2003) Observations of the BaR-SPOrt Northern target at 1.4 GHz (Low emission area at RA = 11 h, DEC = 42°)Observations of the BaR-SPOrt Northern target at 1.4 GHz (Low emission area at RA = 11 h, DEC = 42°) Already done with Effelsberg Telescope April Already done with Effelsberg Telescope April Observations: Work in progress… I PI

IV. Calibrators: Moon Observations Calibration Identification of Calibration sources challengeFinding CMBP calibrators is a challenge for Experimenters – no dipole – no planets very faint.Polarized calibrators (as 3C286) are very faint. the MoonA solution: the Moon Observation at 8.3 GHz (MEDICINA) Polarized intensity is really high: - Peak at  10 K on arcmin scale -  5 mK integrated on 7° SPOrt beam In progress: Observations at 22, 32 and 90 GHz in next future. Poppi S. et al. (2002) AIP Conf. Proc. 609, 187

V. Theoretical Analysis Theoretical studies Theoretical studies of the relevant astrophysics: Galaxy and CMBP. Synchrotron emission lack of dataSynchrotron emission likely represents the most important foreground noise (spinning dust?), but…. lack of data at high Galactic latitutes and in the MW range: synch emission template –Development of a polarized synch emission template –Analysis high Galactic latitudes –Analysis of the observed data at high Galactic latitudes Study of re-ionization scenariosStudy of re-ionization scenarios at the epoch of formation of first galaxies. Bernardi G. et al. (2003) MNRAS, 344, 347Bernardi G. et al. (2004) MNRAS, submitted

Activity in Radio/MW Polarization I.Experiment Design Analysis I.Experiment Design Analysis to take instrumental errors under control; II.Data Analysis II.Data Analysis to –Remove residual systematic effects; –Extract relevant scientific information. –Galactic foreground emission study (Synchrotron); III. low Synchrotron emission regions (BaR-SPOrt); III. Identification of low Synchrotron emission regions (BaR-SPOrt); IV. Calibration IV. Identification of Calibration sources; V.Theoretical studies V.Theoretical studies of the relevant astrophysics: Galaxy and CMBP.