1 Astro Particle Cosmology Studying SZ Effects with ALMA ALMA/ARC 2007 ALMA/ARC 2007 March 2, 2007 Sergio Colafrancesco Sergio Colafrancesco INAF - Osservatorio.

Slides:



Advertisements
Similar presentations
October 27, 2006 Monique ARNAUD Atelier du PNC: Cosmologie avec SKA et LOFAR Amas de galaxies Emission non thermique comme traceur de la formation et de.
Advertisements

Notes… Handouts available for today and yesterday
Discrepancy between average WMAP observed and ROSAT predicted Sunyaev- Zel'dovich Effect profiles of 31 clusters (2006 ApJ, 648, 176)
Kinetic SZ effect from galaxy cluster rotation & Another relativistic correction to the SZE JC, Gert Hütsi and Rashid Sunyaev accepted by A&A, 2005, astro-ph/
SZ effects by using high-resolution simulations Lauro Moscardini Dipartimento di Astronomia Università di Bologna, Italy Orsay,
1 The SZE in the SKA & MILLIMETRON Era. The SZE: Physics high-energy photon Internal High-E electrons - thermal (supra-thermal) - relativistic ↑ Use CMB.
Cosmic Baryons: The IGM Ue-Li Pen 彭威禮. Overview History of Cosmic Baryons: a gas with phase transitions Missing baryons simulations SZ-Power spectrum:
Kelley Liebst AST 591 School of Earth and Space Exploration Arizona State University.
Clusters of galaxies: the soft X- ray excess and Sunyaev- Zel’dovich effect Richard Lieu Jonathan Mittaz University of Alabama, Huntsville Shuang-Nan Zhang.
1 Astro Particle Cosmology OAR Roma Soft X-ray emission in Large Scale Structures: thermal or non-thermal ? Soft X-ray emission in Large Scale Structures:
SZE in WMAP Data Jose M. Diego & Bruce Partridge 2010, MNRAS, 402, 1179 La Thuile, March 2012.
Luigina Feretti Istituto di Radioastronomia CNR Bologna, Italy Radio observations of cluster mergers X-Ray and Radio Connections, Santa Fe, NM February.
“Dark Matter in Modern Cosmology” Sergio Colafrancesco.
Radio halos and relics in galaxy clusters. NGC315: giant (~ 1.3 Mpc) radio galaxy with odd radio lobe (Mack 1996; Mack et al. 1998). precessing jets (Bridle.
Mark Birkinshaw University of Bristol
Eiichiro Komatsu University of Texas at Austin A&M, May 18, 2007
Hamburg, 18 September 2008 LOFAR Wokshop1/44 Thermal and non-thermal emission from galaxy clusters: X-ray and LOFAR observations Chiara Ferrari Observatoire.
Particle Physics and Cosmology Dark Matter. What is our universe made of ? quintessence ! fire, air, water, soil !
K.S. Dawson, W.L. Holzapfel, E.D. Reese University of California at Berkeley, Berkeley, CA J.E. Carlstrom, S.J. LaRoque, D. Nagai University of Chicago,
XMM results in radio-galaxy physics Judith Croston CEA Saclay, Service d’Astrophysique EPIC consortium meeting, Ringberg, 12/04/05.
Astrophysical Jets Robert Laing (ESO). Galactic black-hole binary system Gamma-ray burst Young stellar object Jets are everywhere.
Inverse Compton Radiation Rybicki & Lightman Chapter Review of the Compton Effect 2 – Review of Thomson Scattering 3 – Klein-Nishima Cross-section.
The Structure Formation Cookbook 1. Initial Conditions: A Theory for the Origin of Density Perturbations in the Early Universe Primordial Inflation: initial.
A Primer on SZ Surveys Gil Holder Institute for Advanced Study.
Constraining Galactic Halos with the SZ-effect
Physics 133: Extragalactic Astronomy and Cosmology Lecture 11; February
Program 1.The standard cosmological model 2.The observed universe 3.Inflation. Neutrinos in cosmology.
MATTEO VIEL THE LYMAN-  FOREST: A UNIQUE TOOL FOR COSMOLOGY Bernard’s cosmic stories – Valencia, 26 June 2006 Trieste Dark matter Gas.
Gamma-ray From Annihilation of Dark Matter Particles Eiichiro Komatsu University of Texas at Austin AMS April 23, 2007 Eiichiro Komatsu University.
Modelling radio galaxies in simulations: CMB contaminants and SKA / Meerkat sources by Fidy A. RAMAMONJISOA MSc Project University of the Western Cape.
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.
Radio-loud AGN energetics with LOFAR Judith Croston LOFAR Surveys Meeting 17/6/09.
Thermal / Non-thermal plasma Interactions in Clusters The Good, the Bad & the Puzzling L. Rudnick, MN Inst. for Astrophysics, Zeldovich 100.
The Science Case for Band 1 James Di Francesco Herzberg Institute of Astrophysics Victoria, BC, Canada.
How can CMB help constraining dark energy? Licia Verde ICREA & Institute of space Sciences (ICE CSIC-IEEC)
Cosmology 2002/20031 Distribution of objects, Fluxes etc The Geometry and q 0 Prof. Guido Chincarini The idea of this chapter that will be upgraded as.
Summary(3) -- Dynamics in the universe -- T. Ohashi (Tokyo Metropolitan U) 1.Instrumentation for dynamics 2.Cluster hard X-rays 3.X-ray cavities 4.Dark.
Using the Sunyaev-Zeldovich Effect to Determine H o and the Baryon Fraction by Michael McElwain Astronomy 278: Anisotropy and Large Scale Structure in.
Lecture 5: Matter Dominated Universe: CMB Anisotropies and Large Scale Structure Today, matter is assembled into structures: filaments, clusters, galaxies,
University of Durham Institute for Computational Cosmology Carlos S. Frenk Institute for Computational Cosmology, Durham Galaxy clusters.
Sunyaev-Zel'dovich effect CMB anisotropies: S-Z effect and how it is used in practice The theoretical foundation of the Sunyaev-Zel'dovich effect.
SUNYAEV-ZELDOVICH EFFECT. OUTLINE  What is SZE  What Can we learn from SZE  SZE Cluster Surveys  Experimental Issues  SZ Surveys are coming: What.
The Origin and Acceleration of Cosmic Rays in Clusters of Galaxies HWANG, Chorng-Yuan 黃崇源 Graduate Institute of Astronomy NCU Taiwan.
LOFAR & Particle Acceleration: Radio Galaxies & Galaxy Clusters
GH2005 Gas Dynamics in Clusters II Craig Sarazin Dept. of Astronomy University of Virginia A85 Chandra (X-ray) Cluster Merger Simulation.
SZ effect and ALMA workshops Lauro Moscardini Dipartimento di Astronomia Università di Bologna, Italy IAS, Orsay, 7-8 April 2005.
SZ review The microwave background radiation and the Sunyaev- Zel’dovich effect Mark Birkinshaw.
Relativistic Corrections to the Sunyaev-Zeldovich Effect for Clusters of Galaxies Satoshi Nozawa Josai Junior College for Women 1/33 Collaborators: N.
EANAM 2006,Daejeon,Korea Recovering the SZ Redshift Information by SZ-galaxy Cross Correlation Jiawei Shao, Pengjie Zhang, Weipeng Lin, Yipeng Jing 邵家伟,张鹏杰,林伟鹏,景益鹏.
X-ray Astronomy School 2002 Clusters of Galaxies (and some Cosmology) Scientific and Data Analysis Issues Keith Arnaud NASA/GSFC and UMCP.
Giuseppina Coppola1 First predicted by the Russian scientists Sunayaev and Zel’dovich in Galaxy Clusters have hot gas that produce electrons by bremsstahlung.
Astrophysics from the Moon in the Radio Band Gianfranco Brunetti INAF - IRA, Bologna.
1 Suparna Roychowdhury Groups of galaxies in nearby universe, Santiago, Chile, december, 2005 Astronomy Group, Raman Research Institute Bangalore,
Fermi LAT Discovery of Gamma-rays from the Giant Radio Lobes of Centaurus A C.C. Teddy Cheung (NRC/NRL) Lukasz Stawarz (ISAS/JAXA) Yasushi Fukazawa (Hiroshima)
CLUSTERS OF GALAXIES IGM, and Scaling Laws. Emission Processes of Clusters of Galaxies in the X-ray Band.
NuSTAR, ITS BACKGROUND AND CLUSTERS OF GALAXIES FABIO GASTALDELLO INAF, IASF-Milano And The Galaxy Clusters NuSTAR Team.
Study of Proto-clusters by Cosmological Simulation Tamon SUWA, Asao HABE (Hokkaido Univ.) Kohji YOSHIKAWA (Tokyo Univ.)
The interplay of GeV electrons & magnetic fields: The interplay of GeV electrons & magnetic fields: interesting aspects in galaxies, radio galaxies and.
Non-Thermal Radiation Chapter 8. Our Goal: Synchrotron Radiation -Produced by relativistic electrons moving an a magnetic field -Sometimes referred to.
Biased total mass of CC galaxy clusters by SZE measurements Andrea Conte Astronomy PhD, XXIII Cycle “Sapienza” University of Rome. School of Astrophysics.
asdfasdfasdf 5sasdfasasdf
AY202a Galaxies & Dynamics Lecture 18: Galaxy Clusters & Cosmology
M. De Petris – Sept. 25th, 2015 Exploring kinetic Sunyaev-Zel’dovich Effect with MUSIC clusters of galaxies Marco De Petris “Sapienza” University.
Cosmological constraints from tSZ-X cross-correlation
Polarization of Cluster Radio Sources with LOFAR
Karl Mannheim – ITPA Würzburg
Cooperate with X-L. Chen , Q. Yuan, X-J. Bi, Z-Q. Shen
Lecture 2 IGM, Scaling Laws Clusters Cosmology Connection
Eiichiro Komatsu University of Texas at Austin A&M, May 18, 2007
Presentation transcript:

1 Astro Particle Cosmology Studying SZ Effects with ALMA ALMA/ARC 2007 ALMA/ARC 2007 March 2, 2007 Sergio Colafrancesco Sergio Colafrancesco INAF - Osservatorio Astronomico di Roma INAF - Osservatorio Astronomico di Roma

SZ effect: the standard lore thermal NR e - I 0 (x) I(x)

The origin of the SZ effect 1957 A.S. Kompaneets publishes his Compton scattering Fokker-Planck equation 1969 Ya. B. Zel’dovich & R. Sunyaev derive the SZ effect (i.e., applied the Kompaneets eq.) for a thermal intracluster plasma Non-coherent Compton Scattering Fall-out effect of the Cold War (derived by A.S. Kompaneets in Soviet Union  1950 but was classified due to bomb research until 1956)

SZ effect: …more than basics thermal NR e - relativistic e - I 0 (x) I(x) I rel (x)

Intensity change Spectral shape Thermal Relativistic SZE: general derivation Redistribution function Pressure [ Colafrancesco & al. 2003, A&A, 397, 27]

SZE: other sources Kinematic SZE +V p -V p 2.5/h Mpc Rees-Sciama E measures V across line of sight butterfly shape for each cluster amplitude a few  K spectrum same as CMB (Nottale 1984) VtVt

Power-law Maxwellian Astrophysical relevance Thermal particles E e  0.1 – 10 keV WIMPs M   10–500 GeV Cosmic rays E e  16GeV B  1/2 ( GHz ) 1/2 3C294 3C432 DRACO 1ES B-fields Acceleration procs. Galaxy clusters AGN jets/cavitiesDM naturePlasma physics WHIM

Cosmological relevance Galaxy clusters AGN jets/cavitiesDM naturePlasma physics Hubble diagram Cluster counts Cluster velocities T CMB (z)SUSY DM Non-SUSY DM Baryon fraction WHIM Excluded by SZE in Coma Excluded by BBN Excluded by WMAP 3C432 MeV DM sterile …

The e  distribution in clusters 50GeV = M  100 GeV 200 GeV 500 GeV T=0.1 keV T=8.2 keV Radio-halo electrons COMA : warm gas + hot gas + radio halo + DM halo

The SZE from various e  pops. SZ rel SZ DM SZ kin SZ warm SZ th [ Colafrancesco 2007, New Astr.Rev, 51, 394 ]

SZE & cavities in clusters [Colafrancesco. 2005, A&A, 435, L9]

SZE from radio-galaxy jets [Colafrancesco. 2007, MNRAS, in press]

SZE in DM halos SZ th SZ rel SZ DM SZ kin SZ warm A structure with: Hot gas Warm gas Rel. Plasma DM Distant & V r

SZE in DM halos SZ th SZ warm SZ rel SZ DM A structure with: Hot gas Warm gas Rel. Plasma DM Nearby (V r ≈ 0)

SZE in DM halos SZ th SZ warm SZ DM A structure with: Hot gas Warm gas DM Nearby (V r ≈ 0)

SZE in DM halos SZ DM A structure with: DM Nearby (V r ≈ 0)

CMB maps & DRACO

SZ DM in Draco [Culverhouse, Ewans & Colafrancesco 2006, MNRAS, 368, 659] SZX-rays

The cluster 1ES DM clump A) M = M  DM clump A) M = M  DM clump B) M = M  DM clump B) M = M  Gas clump A) T = 14 keV Gas clump A) T = 14 keV Gas clump B) T = 6 keV Gas clump B) T = 6 keV

The SZ DM from 1ES

Isolating SZ DM at  223 GHz Frequency (M  = 20 GeV)Neutralino mass ( =223 GHz) [Colafrancesco et al. 2007, A&A, 467, L1]

SZE science: requirements SZE Resolution: 1” – 10’  = 10 – 500 GHz GHz

RG jets Shocks, V Cavities DM B-field Cosmology

SZE: ALMA resolution

SZE: ALMA FOV & resolution ALMA vs SZ non-th ALMA vs SZ cavity ALMA vs SZ DM 250 arcsec arcsec Cavity

SZE: ALMA -coverage SZ th SZ DM ALMA vs SZ non-th ALMA vs SZ cavity ALMA vs SZ DM SZ rel SZ warm SZ kin Band 3 Band 6Band 7 Band 9 ALMA reference -bands Band 386 – 116 GHz Band 6211 – 275 GHz Band 7275 – 370 GHz Band 9602 – 720 GHz