Analysis of a New Gravitational Lens FLS 1718+59 Yoon Chan Taak Feb 14 2013 Survey Science Group Workshop 2013 1.

Slides:



Advertisements
Similar presentations
ANITA workshop. Jan 2003 Gravitational lensing and the VO Randall Wayth.
Advertisements

The Large Scale Structure of the Universe Clusters of galaxies X-rays from clusters of galaxies Sheets and voids.
Astrophysical applications of gravitational microlensing By Shude Mao Ziang Yan Department of Physics,Tsinghua.
Gravitational Lensing Boot Camp Robert Nemiroff Michigan Tech.
Chapter 16 Dark Matter And The Fate Of The Universe.
H.-W. Rix, Vatican 2003 Gravitational Lensing as a Tool in Cosmology A Brief History of Lensing 1704 Newton (in Optics): „Do not bodies act upon light.
Optical Scalar Approach to Weak Gravitational Lensing by Thick Lenses Louis Bianchini Mentor: Dr. Thomas Kling Department of Physics, Bridgewater State.
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.
How do we transform between accelerated frames? Consider Newton’s first and second laws: m i is the measure of the inertia of an object – its resistance.
July 7, 2008SLAC Annual Program ReviewPage 1 Weak Lensing of The Faint Source Correlation Function Eric Morganson KIPAC.
General Relativity Physics Honours 2006 A/Prof. Geraint F. Lewis Rm 557, A29 Lecture Notes 6.
The Consequences of a Dynamical Dark Energy Density on the Evolution of the Universe By Christopher Limbach, Alexander Luce, and Amanda Stiteler Background.
Gradient Refractive Index Gradient Refractive Index The refractive index of a particular point of a lens with a gradient refractive index The refractive.
Physics 133: Extragalactic Astronomy and Cosmology Lecture 12; February
Dark matter and black holes over cosmic time TOMMASO TREU.
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.
Measuring the local Universe with peculiar velocities of Type Ia Supernovae MPI, August 2006 Troels Haugbølle Institute for Physics.
Chapter 16: Hubble’s Law and Dark Matter 3C295 in X-rays 5 billion light years away and 2 million light years across.
Einstein’s Lens Presented by: Kevin McLin, SSU NASA E/PO 2008 EA Training, SSU Einstein’s Lens.
The Hidden Lives of Galaxies Jim Lochner, USRA & NASA/GSFC.
Hubble Finds Ring of Dark Matter The Astrophysical Journal, 661: , 2007 June 1.
Probing Small-Scale Structure in Galaxies with Strong Gravitational Lensing Arthur Congdon Rutgers University.
Lens Galaxy Environments Neal Dalal (IAS), Casey R. Watson (Ohio State) astro-ph/ Who cares? 2.What to do 3.Results 4.Problems! 5.The future.
Type Ia Supernovae on a glass: The bread and butter of peculiar velocities Lunch meeting Aarhus, March 2007 Troels Haugbølle Institute.
Progress on Cosmology Sarah Bridle University College London.
Galaxies Chapter 13:. Galaxies Contain a few thousand to tens of billions of stars, Large variety of shapes and sizes Star systems like our Milky Way.
1 Gravitational lensing and neutrinos Why not look where natural lenses exist? Proposal of an additional candidate list in point source search: 1. Motivation.
Dark Matter begin. Definition Dark Matter is matter that we cannot see. It neither emits nor reflects any light. If we can’t see it, how do we know it.
Weak Lensing 3 Tom Kitching. Introduction Scope of the lecture Power Spectra of weak lensing Statistics.
Application of Gravitational Lensing Models to the Brightest Strongly Lensed Lyman Break Galaxy – the 8 o’clock arc E. Buckley-Geer 1, S. Allam 1,2, H.
Eric V. Linder (arXiv: v1). Contents I. Introduction II. Measuring time delay distances III. Optimizing Spectroscopic followup IV. Influence.
1 Galaxies at Cosmic Dawn Revealed in the First Year of the Hubble Frontier Fields Initiative Dr. Gabriel Brammer (ESA/AURA, STScI) Hubble Science Briefing.
Galaxy Mass Star Number/Density Counting stars in a given volume
1 Galaxies The Andromeda Galaxy - nearest galaxy similar to our own. Only 2 million light years away! Galaxies are clouds of millions to hundreds of billions.
GRAVITATIONAL LENSING
A Short Talk on… Gravitational Lensing Presented by: Anthony L, James J, and Vince V.
Constraining Dark Energy with Cluster Strong Lensing Priyamvada Natarajan Yale University Collaborators: Eric Jullo (JPL), Jean-Paul Kneib (OAMP), Anson.
PREDRAG JOVANOVIĆ AND LUKA Č. POPOVIĆ ASTRONOMICAL OBSERVATORY BELGRADE, SERBIA Gravitational Lensing Statistics and Cosmology.
Origins Lecture 10; May Previously… on Origins: Is Earth a special/unique place? What does the question mean? How do we find planets? What are.
1 Gravitational lensing with neutrinos Results, paper and public plots J.P. Gómez-González, S.Mangano,
Gravitational Lensing
Exploring Dark Matter through Gravitational Lensing Exploring the Dark Universe Indiana University June 2007.
Introduction to the modern observational cosmology Introduction/Overview.
General Relativity Physics Honours 2005 Dr Geraint F. Lewis Rm 557, A29
Constraining Cosmology with Peculiar Velocities of Type Ia Supernovae Cosmo 2007 Troels Haugbølle Institute for Physics & Astronomy,
PHY306 1 Modern cosmology 3: The Growth of Structure Growth of structure in an expanding universe The Jeans length Dark matter Large scale structure simulations.
Space Warps. Light is believed to travel the shortest distance between two points But…… the path of light is curved in the presence of a gravitational.
Astronomy 102/112: Introduction to Stars, Galaxies, and the Universe Professor R. Somerville Fall 2001.
Constraining Cosmography with Cluster Lenses Jean-Paul Kneib Laboratoire d’Astrophysique de Marseille.
Gravity I’m attracted to you.
Influence of dark energy on gravitational lensing Kabita Sarkar 1, Arunava Bhadra 2 1 Salesian College, Siliguri Campus, India High Energy Cosmic.
10/5/2004New Windows on the Universe Jan Kuijpers Part 1: Gravitation & relativityPart 1: Gravitation & relativity J.A. Peacock, Cosmological Physics,
Announcements The final exam will be at Noon on Monday, December 13 in Van Allen Hall LR1. Practice questions for unit #5 are available on the class web.
Conformal Gravity in the X-ray Cluster Abell 2029 Keith Horne SUPA St Andrews 10 8 K gas galaxies monster galaxy.
Galaxies with Active Nuclei Chapter 14:. Active Galaxies Galaxies with extremely violent energy release in their nuclei (pl. of nucleus).  “active galactic.
The Universe. Galaxies are believed to have formed from mergers of smaller galaxies and star clusters. Galaxy Formation and Evolution.
Quiz #10 What would really happen to you if you were to fall all the way into the Event Horizon of a black hole? We know the gravity is unbelievably strong.
Physics 55 Monday, December 5, Course evaluations. 2.General relativity with applications to black holes, dark matter, and cosmology. 3.Hubble’s.
Gravitational Lensing
General Relativity and Grade-9 Astronomy. 0) Gravity causes time to slow down. Everyday Einstein: The GPS and Relativity OAPT Conference May 12 – 14 McMaster.
Probing Dark Energy with Cosmological Observations Fan, Zuhui ( 范祖辉 ) Dept. of Astronomy Peking University.
March 7, 2016March 7, 2016March 7, 2016Yerevan, Armenia1 GRAVITATIONAL LENSING GRAVITATIONAL LENSING History, Discovery and Future Measuring Mass of Dark.
VISIBLE PROPERTIES OF COSMIC ANTI-STRING Kotvytskiy A.T., Shulga V.M. Institute of Radio Astronomy of Nat. Ac. Sci. of Ukraine Karazin Kharkov National.
MEASUREING BIAS FROM UNBIASED OBSERVABLE SEOKCHEON LEE (KIAS) The 50 th Workshop on Gravitation and Numerical INJE Univ.
The Nature of Dark Energy David Weinberg Ohio State University Based in part on Kujat, Linn, Scherrer, & Weinberg 2002, ApJ, 572, 1.
Seeing the Invisible: Observing the Dark Side of the Universe Sarah Bridle University College London.
1 Gravitational lensing and neutrinos Why not look where natural lenses exist? Proposal of an additional candidate list in point source search: 1. Motivation.
Chapter 16 Active Galaxy.
Announcements Final exam is Monday, May 9, at 7:30 am.
Presentation transcript:

Analysis of a New Gravitational Lens FLS Yoon Chan Taak Feb Survey Science Group Workshop

What is Gravitational Lensing? Deflection of light by body of mass ◦ Deflection angle greater for GR (factor of 2)  vs (r: source-lens distance) ◦ e.g. Solar eclipse of May 1919 Causes distortion of images 2

Images of GL 3 Abell 1689 cluster

Images of GL 4 Einstein Ring – SDSS J Einstein Cross – QSO

Images of GL 5

Types of GL Strong GL ◦ Big distortions, e.g. rings, arcs, multiple img ◦ Lens is galaxy or cluster Weak GL ◦ Shear distortion ◦ Lens is galaxy or cluster, but further away from source Microlensing ◦ Brightness variations ◦ Lens has stellar masses (e.g. planets) 6

Why GL? Requires only mass  Allows detection of dark matter Acts as “cosmic telescope”  Lets us see more distant objects Determines cosmological parameters ◦ Deflection depends on redshift-distance formula ◦ Time delay related to Hubble constant  Constrains geometry of universe 7

Gravitational Lensing Theory Point-mass lens Finite lens 8

Point Mass (Schwarzschild) Lens Lens (Ray-trace) equation ◦ 11 ◦ 1 9 θ S : lens-source angular distance α : deflection angle of light ray θ 1,2 : lens-img angular distances b : lens-deflection pt angular dist. α 0 : Einstein rad. [(4GM/c 2 ) (D LS /D L D S )] 1/2 α D LS θSDSθSDS (D S /D L )b

Finite Lens Ray-trace eqn is for 2-D plane ◦ Change scalars to vectors for 3-D Integrate deflection angle for all infinitesimal masses ◦ I Calculate numerical solution 10

gravlens: Software for G-Lensing Developed by C. Keeton (Rutgers) Useful for various g-lens images ◦ Able to find best set of lens parameters for multiple images (lensmodel) Contains 20+ lens models ◦ Can be superposed, diverse potentials possible 11

FLS G-lensing image in Spitzer First Look Survey Field z lens = 0.08 z source = ◦ Closest source so far(?) RA = 17 h 18 m 17.6 s Dec = 59 d 31 m 46 s

FLS

Procedures Simulated lensing images with several sets of input variables ◦ Mass scale of lens ◦ X coord. of source ◦ Ellipticity (angle) of source ◦ Ellipticity (angle) of lens* Assumed no external shear * Obtained from original HST image

Softened Power Law Ellipsoid

Results

Discussion Many sets of variables may yield similar images A more careful approach is necessary for constraining errors  requires analysis with more sets of variables  M gal ~ M ʘ, σ ~ 150km/s  Possibly an edge-on spiral