Guoliang Li Shanghai Astronomic Observatory November 1st, 2006 November 1st, 2006 The giant arc statistic in the three-year WMAP cosmological model COLLABORATORS:

Slides:



Advertisements
Similar presentations
Cosmological Structure Formation A Short Course III. Structure Formation in the Non-Linear Regime Chris Power.
Advertisements

Building a Mock Universe Cosmological nbody dark matter simulations + Galaxy surveys (SDSS, UKIDSS, 2dF) Access to mock catalogues through VO Provide analysis.
Astronomical Solutions to Galactic Dark Matter Will Sutherland Institute of Astronomy, Cambridge.
Formation of Globular Clusters in  CDM Cosmology Oleg Gnedin (University of Michigan)
Galaxy alignment within cosmic structures Weipeng Lin Shanghai Astronomical Observatory, CAS, China
Why Environment Matters more massive halos. However, it is usually assumed in, for example, semianalytic modelling that the merger history of a dark matter.
Probing DM Halo Shapes Using Satellite Galaxy Kinematics Jeremy Bailin (Swinburne) Chris Power, Brad Gibson (Swinburne), Peder Norberg (ETH), Dennis Zaritsky.
Dark Halos of Fossil Groups and Clusters Observations and Simulations Ali Dariush, Trevor Ponman Graham Smith University of Birmingham, UK Frazer Pearce.
July 7, 2008SLAC Annual Program ReviewPage 1 Weak Lensing of The Faint Source Correlation Function Eric Morganson KIPAC.
Large Scale Structure of the Universe at high redshifts Large Scale Structure of the Universe at high redshifts M.Demianski, A.Doroshkevich and S.Gottloeber.
Weak-Lensing selected, X-ray confirmed Clusters and the AGN closest to them Dara Norman NOAO/CTIO 2006 November 6-8 Boston Collaborators: Deep Lens Survey.
Strong Lensing in RCS-2 Clusters Matt Bayliss University of Chicago Department of Astronomy & Astrophysics Great Lakes Cosmology Workshop 8 – June 2, 2007.
Physics 133: Extragalactic Astronomy and Cosmology Lecture 13; February
What’s new here? The accuracy of the thin lens approximation has been assessed through convergence of statistics by increasing the number of lens planes.
On the Distribution of Dark Matter in Clusters of Galaxies David J Sand Chandra Fellows Symposium 2005.
Relating Mass and Light in the COSMOS Field J.E. Taylor, R.J. Massey ( California Institute of Technology), J. Rhodes ( Jet Propulsion Laboratory) & the.
THE STRUCTURE OF COLD DARK MATTER HALOS J. Navarro, C. Frenk, S. White 2097 citations to NFW paper to date.
Weak Gravitational Lensing by Large-Scale Structure Alexandre Refregier (Cambridge) Collaborators: Richard Ellis (Caltech) David Bacon (Cambridge) Richard.
Galaxy-Galaxy Lensing What did we learn? What can we learn? Henk Hoekstra.
Astro 101 Slide Set: Multiple Views of an Extremely Distant Galaxy 0 Topic: Distant galaxies Concepts: Galaxy development, Gravitational lensing Missions:
 CDM Subhalos P.Nurmi, P.Heinämäki, E. Saar, M. Einasto, J. Holopainen, V.J. Martinez, J. Einasto Subhalos in LCDM cosmological simulations: Masses and.
Cosmic shear results from CFHTLS Henk Hoekstra Ludo van Waerbeke Catherine Heymans Mike Hudson Laura Parker Yannick Mellier Liping Fu Elisabetta Semboloni.
Impact of Early Dark Energy on non-linear structure formation Margherita Grossi MPA, Garching Volker Springel Advisor : Volker Springel 3rd Biennial Leopoldina.
Structure formation in dark energy cosmology La Magia, April 2005.
, Tuorla Observatory 1 Galaxy groups in ΛCDM simulations and SDSS DR5 P. Nurmi, P. Heinämäki, S. Niemi, J. Holopainen Tuorla Observatory E. Saar,
GRAVITATIONAL LENSING
Complementarity of weak lensing with other probes Lindsay King, Institute of Astronomy, Cambridge University UK.
Intrinsic ellipticity correlation of luminous red galaxies and misalignment with their host dark matter halos The 8 th Sino – German workshop Teppei O.
Cluster Strong Lensing Neal Dalal IAS. Cluster Strong Lensing Images of background galaxies strongly distorted by potential of foreground massive cluster.
Cosmological studies with Weak Lensing Peak statistics Zuhui Fan Dept. of Astronomy, Peking University.
Formation and structure of dark matter halos in N-body and SPH simulations Wei-Peng Lin The Partner Group of MPI for Astrophysics, Shanghai Astronomical.
PREDRAG JOVANOVIĆ AND LUKA Č. POPOVIĆ ASTRONOMICAL OBSERVATORY BELGRADE, SERBIA Gravitational Lensing Statistics and Cosmology.
Understanding formation of galaxies from their environments Yipeng Jing Shanghai Astronomical Observatory.
Exploring Dark Matter through Gravitational Lensing Exploring the Dark Universe Indiana University June 2007.
Large-scale structure at high z: the SHADES survey Eelco van Kampen, University of Edinburgh with Jim Dunlop, John Peacock, Will Percival, Chris Rimes,
SUNYAEV-ZELDOVICH EFFECT. OUTLINE  What is SZE  What Can we learn from SZE  SZE Cluster Surveys  Experimental Issues  SZ Surveys are coming: What.
The masses and shapes of dark matter halos from galaxy- galaxy lensing in the CFHTLS Henk Hoekstra Mike Hudson Ludo van Waerbeke Yannick Mellier Laura.
The Structure Formation Cookbook 1. Initial Conditions: A Theory for the Origin of Density Perturbations in the Early Universe Primordial Inflation: initial.
Cosmology with Gravitaional Lensing
Theoretical Predictions about the Cold- Warm Gas Size around Cluster Galaxies using MgII systems Iván Lacerna VII Reunión Anual, SOCHIAS 2009 January 14.
The effects of the complex mass distribution of clusters on weak lensing cluster surveys Zuhui Fan Dept. of Astronomy, Peking University.
Racah Institute of physics, Hebrew University (Jerusalem, Israel)
Applications of Cosmological N-body/ SPH simulations Baryonic Effects on the Properties of Dark Matter Halos Weipeng Lin (Shanghai Astronomical Observatory,
A wide field multi-wavelength survey of two clusters at z~0.5 Tommaso Treu (UCSB)
Simulating the SZ Sky Predictions for Upcoming Sunyaev-Zel’dovich Effect Galaxy Cluster Surveys Eric J. Hallman CASA, University of Colorado 16 February,
Cosmic shear and intrinsic alignments Rachel Mandelbaum April 2, 2007 Collaborators: Christopher Hirata (IAS), Mustapha Ishak (UT Dallas), Uros Seljak.
Probing cosmic structure formation in the wavelet representation Li-Zhi Fang University of Arizona IPAM, November 10, 2004.
April 3, 2005 The lens redshift distribution – Constraints on galaxy mass evolution Eran Ofek, Hans-Walter Rix, Dan Maoz (2003)
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.
Strong Lensing Surveys and Statistics Dan Maoz. zqzq Survey strategies: Search among source population for lensed cases or Search behind potential lenses.
Elinor Medezinski Johns Hopkins University Galaxy Galaxy Lensing in CLASH clusters.
Merger time scale of galaxies Yipeng Jing Shanghai Astronomical Observatory Collaborators: Chunyan Jiang, A. Faltenbacher, W.P. Lin, C. Li (astroph/ ;
Evolution of galaxies and dark matter halos Yipeng Jing Shanghai Astronomical Observatory Main Collaborators: Chunyan Jiang ( 姜春艳), Cheng Li (李成), Donghai.
The influence of baryons on the matter distribution and shape of dark matter halos Weipeng Lin , Yipeng Jing ( Shanghai Astronomical Observatory , CAS.
Investigating dark matter halos of galaxies from the COMBO-17 survey Martina Kleinheinrich (Max-Planck-Institut für Astronomie, Heidelberg) & Hans-Walter.
Semi-analytical model of galaxy formation Xi Kang Purple Mountain Observatory, CAS.
Gravitational Lensing
Finding and Characterizing the Giant Arcs Bingxiao Xu Johns Hopkins University.
Feasibility of detecting dark energy using bispectrum Yipeng Jing Shanghai Astronomical Observatory Hong Guo and YPJ, in preparation.
Study of Proto-clusters by Cosmological Simulation Tamon SUWA, Asao HABE (Hokkaido Univ.) Kohji YOSHIKAWA (Tokyo Univ.)
Mass Profiles of Galaxy Clusters Drew Newman Newman et al. 2009, “The Distribution of Dark Matter Over Three Decades in Radius in the Lensing Cluster Abell.
N-body Simulations and Gravitational Lensing with Dark Energy Beyond Einstein Meeting, May 13, 2004.
Thomas Collett Institute of Astronomy, Cambridge
The Dark Energy Survey Probe origin of Cosmic Acceleration:
Clustering and environments of dark matter halos
Advisors: Tom Broadhurst, Yoel Rephaeli
Some issues in cluster cosmology
The Role of Baryons in Strong Lensing properties of Simulated Clusters
Intrinsic Alignment of Galaxies and Weak Lensing Cluster Surveys Zuhui Fan Dept. of Astronomy, Peking University.
Chengliang Wei Purple Mountain Observatory, CAS
Presentation transcript:

Guoliang Li Shanghai Astronomic Observatory November 1st, 2006 November 1st, 2006 The giant arc statistic in the three-year WMAP cosmological model COLLABORATORS: Shude mao (JBO) Yipeng Jing, Xi Kang, Weipeng Lin (SHAO) Matthias Bartelmann, Massimo Menegentti (Heidelberg) Liang Gao (Durham)

Giant arcs are background galaxies distorted into long arcs by foreground clusters A2218 Z=0.175

Z=0.18 A1689 Observations can determine, arc L/W ratio, width, source redshift & arc frequency

Why do we study giant arcs? Giant arcs probe the largest bound structures in the universe Their numbers and positions are a sensitive probe of cluster properties including their abundance and mass profiles Their numbers are also sensitive to the cosmogony, particularly the power-spectrum normalisation σ 8 Clusters are nature telescope, allow us to study high-z background objects

Observational samples of giant arcs Luppino et al. found strong lensing in eight out of 38 X-ray selected clusters (Bartelmann(1998) predicted the frequency is 7x10 -3 deg -2 but the observation is 3.7~5.6x10 -2 deg -2 ) Zaritsky & Gozalez (2003) using LCRS and Gladders et al. (2003) using RCS also found high fractions Sand, Ellis, Treu, & Smith (2005) found 104 candidate tangential arcs in 128 clusters with HST Giant arcs appear common in massive clusters and the discrepancy with Bartelmann is kept.

How do we model giant arcs? Earlier studies used analytical spherical models (e.g. Wu & Hammer 1993; Wu & Mao 1996). But clusters are complex (ellipticities, substructures, mergers). More realistic studies use numerical simulated clusters –Bartelmann and associates (1998-) –Dalal et al. (2004) –Li, Mao, Jing, Bartelmann, Kang, Meneghetti (2005) –Wambsganss, Ostriker, Bode (2004): 3D ray-tracing

High resolution simulations Numerical simulations performed by Jing (2000) –Dark matter only, particles –Box size: 300/h Mpc, 30/h kpc (comoving) resolution 200 massive clusters are selected using the friends- of-friends algorithm, from redshift 0.1, 0.2, …, 2.5 Background source population –At redshift 0.6, 1.0, 1.4, …., 7 –Sources have 0.5, 1, 1.5 arcsecond effective diameter –Ellipticity: 1-b/a, from 0.5 to 1 Integrate the cross-sections of all clusters to get the total lensing cross sections.

Optical depth as a function of source redshift Optical depth ~ for z s =1, but for z s =4 –Several previous values are too high due to incorrect assumptions of sigma_8 and L/W definition –Consistent with Dalal et al. (2004) Strong zs dependence Weaker dependence on ellipticity and source size

Optical depth as a function of lens redshift For sources at high z, probe clusters at high redshift Gladders et al. who found all of their lensing clusters were at z>0.62; understood if source z is high.

Comparing with Bartelmann (1998), Dalal et al. (2004) pointed that the numbers of lens and should be increased by a factor of 2. The giant arcs number which they predicted is in good agreement with almost all of the observations. What will happen in the three-year WMAP universe?

Giant arcs in the WMAP3 cosmology The WMAP three-year model has lower  m and  8 compared with the WMAP one-year model. The lower  m (0.238) and  8 (0.74) both reduce the number of giants We compared the arc predictions in the usual LCDM and WMAP three-year model: –Using two 300/h Mpc N-body simulations –The predicted number is reduced by a factor of about six in the WMAP three year model –Easily understood due to the abundance of clusters

Predicted number of giant arcs Effect of star formation? Likely a factor of 2 Source redshift distribution, size, ellipticity(modest)

The way to increase the lensing efficiency The asysmetric of lens ok The merger effect ok The substructure ok The redshift distribution of source ---ok The size and shape of source ---modest The mass around the line of sight----<7% The baryon effect ---not very clear(~2)

Summary Optical depth may be too low in the WMAP three-year model (with  8 =0.74) We need many larger giant arc unbiased samples -- they will come as by-products of weak lensing surveys.

Thanks !