Correlation function in z and real space and consequences A MEASURE OF  = ( Ω m 0.6 / b) Via redshift distorsions.

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.
Early models of an expanding Universe Paramita Barai Astr 8900 : Astronomy Seminar 5th Nov, 2003.
Astro-2: History of the Universe Lecture 4; April
Non-linear matter power spectrum to 1% accuracy between dynamical dark energy models Matt Francis University of Sydney Geraint Lewis (University of Sydney)
Christian Wagner - September Potsdam Nonlinear Power Spectrum Emulator Christian Wagner in collaboration with Katrin Heitmann, Salman Habib,
Dark Matter-Baryon segregation in the non-linear evolution of coupled Dark Energy models Roberto Mainini Università di Milano Bicocca Mainini 2005, Phys.Rev.
PRESENTATION TOPIC  DARK MATTER &DARK ENERGY.  We know about only normal matter which is only 5% of the composition of universe and the rest is  DARK.
Physics 133: Extragalactic Astronomy and Cosmology Lecture 10; February
Final review: Milky Way Galaxies Active galaxies Cosmology: –The future of the universe –The beginning of the universe Test schedule (in LL203) –8 am class:
PRE-SUSY Karlsruhe July 2007 Rocky Kolb The University of Chicago Cosmology 101 Rocky I : The Universe Observed Rocky II :Dark Matter Rocky III :Dark Energy.
Measuring the local Universe with peculiar velocities of Type Ia Supernovae MPI, August 2006 Troels Haugbølle Institute for Physics.
Macroscopic Behaviours of Palatini Modified Gravity Theories [gr-qc] and [gr-qc] Baojiu Li, David F. Mota & Douglas J. Shaw Portsmouth,
Cosmological Models II Connecting Hubble’s law and the cosmological scale factor What determines the kind of Universe in which we live? The Friedman equation.
Lecture 22 Cosmological Models ASTR 340 Fall 2006 Dennis Papadopoulos Chapter 11.
A cosmic sling-shot mechanism Johan Samsing DARK, Niels Bohr Institute, University of Copenhagen.
GALAXY FORMATION AND EVOLUTION - 1. The Expansion of Galaxies In the 1920’s, Edwin Hubble demonstrated that all the `nebulae’ observed in the sky, which.
THE STRUCTURE OF COLD DARK MATTER HALOS J. Navarro, C. Frenk, S. White 2097 citations to NFW paper to date.
MODELING INTRACLUSTER MEDIUM AND DARK MATTER IN GALAXY CLUSTERS Elena Rasia Dipartimento di Astronomia Università di Padova Padova, April 9th, 2002.
Rotating Platform By Unknown.
Review for Exam 3.
Weak Lensing 3 Tom Kitching. Introduction Scope of the lecture Power Spectra of weak lensing Statistics.
Cosmological Tests using Redshift Space Clustering in BOSS DR11 (Y. -S. Song, C. G. Sabiu, T. Okumura, M. Oh, E. V. Linder) following Cosmological Constraints.
Impact of Early Dark Energy on non-linear structure formation Margherita Grossi MPA, Garching Volker Springel Advisor : Volker Springel 3rd Biennial Leopoldina.
Gene University, Finland. Local Group Estimation of Dark Energy & Gravitating Matter Gene Byrd 1, A.D. Chernin 2, B.P. Teerikorpi 3, C.M. Valtonen 4, V.
The formation of galactic disks An overview of Mo Mao & White 1998 MNRAS
Dark energy fluctuations and structure formation Rogério Rosenfeld Instituto de Física Teórica/UNESP I Workshop "Challenges of New Physics in Space" Campos.
Robust cosmological constraints from SDSS-III/BOSS galaxy clustering Chia-Hsun Chuang (Albert) IFT- CSIC/UAM, Spain.
Black Holes Escape velocity Event horizon Black hole parameters Falling into a black hole.
Gary Mamon, 2 July 2005, PNe as astronomical tools, Gdansk Do planetary nebulae indicate a lack of dark matter in elliptical galaxies? with Avishai DEKEL.
Clustering in the Sloan Digital Sky Survey Bob Nichol (ICG, Portsmouth) Many SDSS Colleagues.
Some Conceptual Problems in Cosmology Prof. J. V. Narlikar IUCAA, Pune.
Our Evolving Universe1 Vital Statistics of the Universe Today… l l Observational evidence for the Big Bang l l Vital statistics of the Universe   Hubble’s.
The Fate of the Universe
PHY306 1 Modern cosmology 4: The cosmic microwave background Expectations Experiments: from COBE to Planck  COBE  ground-based experiments  WMAP  Planck.
Dark Energy Wednesday, October 29 Midterm on Friday, October 31.
Masses of Galaxy Groups Brent Tully University of Hawaii.
Michael Doran Institute for Theoretical Physics Universität Heidelberg Time Evolution of Dark Energy (if any …)
Structural and scaling properties of galaxy clusters Probing the physics of structure formation M.Arnaud, G.Pratt, E.Pointecouteau (CEA-Sap Saclay) Dark.
General Relativity Physics Honours 2008 A/Prof. Geraint F. Lewis Rm 560, A29 Lecture Notes 10.
Superclusters as future “island universes” – the case of Shapley Andreas Reisenegger PUC / ESO Theory/simulations: Rolando Dünner (PUC) Andrés Meza (UChile/UNAB)
Cosmic Inhomogeneities and Accelerating Expansion Ho Le Tuan Anh National University of Singapore PAQFT Nov 2008.
Anisotropic Clustering of Galaxies in High-z Universe as a Probe of Dark Energy Taka Matsubara (Nagoya Univ.) “Decrypting the Universe: Large Surveys for.
23 Sep The Feasibility of Constraining Dark Energy Using LAMOST Redshift Survey L.Sun Peking Univ./ CPPM.
6dF Workshop April Sydney Cosmological Parameters from 6dF and 2MRS Anaïs Rassat (University College London) 6dF workshop, AAO/Sydney,
Observational Test of Halo Model: an empirical approach Mehri Torki Bob Nichol.
Zheng Dept. of Astronomy, Ohio State University David Weinberg (Advisor, Ohio State) Andreas Berlind (NYU) Josh Frieman (Chicago) Jeremy Tinker (Ohio State)
The Feasibility of Constraining Dark Energy Using LAMOST Redshift Survey L.Sun.
Hubble’s Law AST 112. Spectra If a light source is moving toward or away from an observer, its spectral lines shift We can use this to measure approaching.
Peculiar velocity decomposition, redshift distortion and velocity reconstruction in redshift surveys Zheng, Yi 郑逸 Shanghai Astronomical Observatory P.
The Boltzmann Distribution allows Calculation of Molecular Speeds Mathematically the Boltzmann Distribution says that the probability of being in a particular.
Cosmology and Dark Matter III: The Formation of Galaxies Jerry Sellwood.
How Different was the Universe at z=1? Centre de Physique Théorique, Marseille Université de Provence Christian Marinoni.
Taka Matsubara (Nagoya Univ.)
Cosmology 2002/20031 The Hubble expansion and the cosmic redshift Guido Chincarini Here we derive a few preliminary expression for the redshift. Try to.
Probing Dark Energy with Cosmological Observations Fan, Zuhui ( 范祖辉 ) Dept. of Astronomy Peking University.
Initial conditions for N-body simulations Hans A. Winther ITA, University of Oslo.
Derivative Examples 2 Example 3
Dark Energy vs. Dark Matter Towards a unification… Centre de Recherche Astronomique de Lyon Alexandre ARBEY March 5, 2006.
Mapping the Mass with Galaxy Redshift-Distance Surveys Martin Hendry, Dept of Physics and Astronomy University of Glasgow, UK “Mapping the Mass”: Birmingham,
MEASUREING BIAS FROM UNBIASED OBSERVABLE SEOKCHEON LEE (KIAS) The 50 th Workshop on Gravitation and Numerical INJE Univ.
Lecture 23: The Acceleration of the Universe Astronomy 1143 – Spring 2014.
Inh Jee University of Texas at Austin Eiichiro Komatsu & Karl Gebhardt
The universe: dark matter and dark energy. Cosmic Microwave Background was discovered in 1965 This really is a map of the sky, black zero emission, green.
Zong-Kuan Guo Department of Physics, Kinki University
Outline Part II. Structure Formation: Dark Matter
The influence of Dark Energy on the Large Scale Structure Formation
Lecture 41 – Cosmology- Final Remarks
Black Holes Escape velocity Event horizon Black hole parameters
Existence of Dark Matter
Presentation transcript:

Correlation function in z and real space and consequences A MEASURE OF  = ( Ω m 0.6 / b) Via redshift distorsions

 = ( Ω m 0.6 / b)

Redshift-space c. f. « distances » in the Z space not in real space

Leads to the true real space correlation function by deprojection

 = ( Ω m 0.6 / b)

Distorsion is a measure of  = ( Ω m 0.6 / b) and then to Ω m if b known

Dynamical effects of the cosmological constant Authors: Lahav, Ofer; Lilje, Per B.; Primack, Joel R.; Rees, Martin J. Affiliation: AA(Cambridge University Institute of Astronomy, England), AB(NORDITA, Copenhagen, Denmark), AC(California, University, Santa Cruz), AD(Cambridge University Institute of Astronomy, England) Journal: Royal Astronomical Society, Monthly Notices (ISSN ), vol. 251, July 1, 1991, p (MNRAS Homepage) Abstract Dynamical tests such as density and velocity profiles around clusters and virialization are employed to theoretically determine the cosmological constant and the density parameter. Limits on the cosmological constant and dynamical tests in linear theory are reviewed, and the tests do not provide a conclusive distinction for universes with cosmological constants. The practical limitations of observing clustering at different redshifts is discussed with respect to linear theory. The nonlinear spherical infall model is then examined for cold-dark- matter power spectra, and the limitations of this method and related observations are discussed. An expression is derived to describe the final radius of a virialized cluster, in which a repulsive cosmological constant lambda gives a smaller value. Two scenarios for the universe are suggested based on the results, one with a large amount of nonbaryonic matter and a zero cosmological constant and another in which all matter is baryonic and the cosmological constant is added to save inflation.