Y.K.Lau Institute of Appl. Maths, CAS. Bondi Sachs Formulation of the Kerr Metric Gravitational Wave Physics of a Kerr Black Hole.

Slides:



Advertisements
Similar presentations
Regularization of the the second-order gravitational perturbations produced by a compact object Eran Rosenthal University of Guelph - Canada Amos Ori Technion.
Advertisements

Reissner–Nordström Expansion Emil M. Prodanov Dublin Institute of Technology.
Spacetime Approach to Force-Free Magnetospheres Sam Gralla University of Maryland Collaborators: Daniel Brennan (UMD undergrad) Ted Jacobson (UMD prof)
Numerical Relativity & Gravitational waves I.Introduction II.Status III.Latest results IV.Summary M. Shibata (U. Tokyo)
The Calculus of Black Holes James Wang Elizabeth Lee Alina Leung Elizabeth Klinger.
Gravitational and electromagnetic solitons Monodromy transform approach Solution of the characteristic initial value problem; Colliding gravitational and.
Introduction to Black Hole Thermodynamics Satoshi Iso (KEK)
Pennsylvania State University Joint work at Southampton University Ulrich Sperhake Ray d’Inverno Robert Sjödin James Vickers Cauchy characteristic matching.
ASYMPTOTIC STRUCTURE IN HIGHER DIMENSIONS AND ITS CLASSIFICATION KENTARO TANABE (UNIVERSITY OF BARCELONA) based on KT, Kinoshita and Shiromizu PRD
Scott Johnson, John Rossman, Charles Harnden, Rob Schweitzer, Scott Schlef Department of Physics, Bridgewater State College // Bridgewater MA, Mentor:
Non-Localizability of Electric Coupling and Gravitational Binding of Charged Objects Matthew Corne Eastern Gravity Meeting 11 May 12-13, 2008.
Rotating BHs at future colliders: Greybody factors for brane fields Kin-ya Oda Kin-ya Oda, Tech. Univ. Munich Why Study BHs at Collider? BH at Collider.
Gerard ’t Hooft Spinoza Institute Utrecht University CMI, Chennai, 20 November 2009 arXiv:
General Relativity Physics Honours 2006 A/Prof. Geraint F. Lewis Rm 557, A29 Lecture Notes 6.
ANALYSIS OF PDE & GENERAL RELATIVITY Sergiu Klainerman June, 2000.
Black Holes Written for Summer Honors Black Holes Massive stars greater than 10 M  upon collapse compress their cores so much that no pressure.
Simulation of relativistic jets near a spinning black hole V.S. Semenov* and S.A. Dyadechkin** It is generally believed that the magnetic field plays a.
Gravitational Radiation Energy From Radial In-fall Into Schwarzschild and Kerr Geometries Project for Physics 879, Professor A. Buonanno, University of.
Announcements Exam 4 is Monday May 4. Tentatively will cover Chapters 9, 10, 11 & 12 Sample questions will be posted soon Observing Night tomorrow night.
2008 May 315th Italian-Sino Workshop Yu-Huei Wu and Chih-Hung Wang Accept by Classical and Quantum Gravity without correction Provisionally scheduled to.
2次ゲージ不変摂動論定式化の進行状況 Kouji Nakamura (Grad. Univ. Adv. Stud. (NAOJ)) References : K.N. Prog. Theor. Phys., vol.110 (2003), 723. (gr-qc/ ). K.N. Prog.
1 Yasushi Mino Theoretical AstroPhysics Including Relativity (TAPIR), CalTech Index 1: Introduction: LISA project 2: MiSaTaQuWa.
Gravitational Radiation from a particle in bound orbit around black hole Presentation for 11 th Amaldi Conference on Gravitational Waves By ASHOK TIWARI.
Plasma Modes Along Open Field Lines of Neutron Star with Gravitomagnetic NUT Charge JD02-21 B. Ahmedov and V. Kagramanova UBAI/INP, Tashkent, UBAI/INP,
Elcio Abdalla Perturbations around Black Hole solutions.
A Periodic Table for Black Hole Orbits Janna Levin Dynamical Systems approach Gabe Perez-Giz NSF Fellow
Objective of numerical relativity is to develop simulation code and relating computing tools to solve problems of general relativity and relativistic astrophysics.
Chapter 13 Black Holes. What do you think? Are black holes just holes in space? What is at the surface of a black hole? What power or force enables black.
Einstein’s elusive waves
Yi-Zen Chu BCCS Case Western Reserve University 9 December 2008 The n-body problem in General Relativity from perturbative field theory arXiv:
International Workshop on Astronomical X-Ray Optics Fingerprints of Superspinars in Astrophysical Phenomena Zdeněk Stuchlík and Jan Schee Institute of.
Prof. dr. A. Achterberg, Astronomical Dept., IMAPP, Radboud Universiteit.
Pavel Bakala Martin Blaschke, Martin Urbanec, Gabriel Török and Eva Šrámková Institute of Physics, Faculty of Philosophy and Science, Silesian University.
Self-Force and the m-mode regularization scheme Sam Dolan (with Leor Barack) University of Southampton BriXGrav, Dublin 2010.
1 Steklov Mathematical Institute RAS G. Alekseev G. Alekseev Cosmological solutions Dynamics of waves Fields of accelerated sources Stationary axisymmetric.
Black Holes Chapter Twenty-Four. Guiding Questions 1.What are the two central ideas behind Einstein’s special theory of relativity? 2.How do astronomers.
Hawking radiation for a Proca field Mengjie Wang (王梦杰 ) In collaboration with Carlos Herdeiro & Marco Sampaio Mengjie Wang 王梦杰 Based on: PRD85(2012)
Multipole moments as a tool to infer from gravitational waves the geometry around an axisymmetric body. Thomas P. Sotiriou SISSA, International School.
Computational Relativity The largest field of enquiry historically has been the field of exact solutions of Einstein's field equations. The Einstein field.
On finding fields and self force in a gauge appropriate to separable wave equations (gr-qc/ ) 2006 Midwest Relativity Meeting Tobias Keidl University.
Gravitational and electromagnetic solitons Stationary axisymmetric solitons; soliton waves Monodromy transform approach Solutions for black holes in the.
1 Building Bridges: CGWA Inauguration 15 December 2003 Lazarus Approach to Binary Black Hole Modeling John Baker Laboratory for High Energy Astrophysics.
Conserved Quantities in General Relativity A story about asymptotic flatness.
Department of Physics, National University of Singapore
Intermediate mass black hole and numerical relativity Zhoujian Cao Institute of Applied Mathematics, AMSS
Gravitational collapse of massless scalar field Bin Wang Shanghai Jiao Tong University.
Motions of Self-Gravitating bodies to the Second Post- Newtonian Order of General Relativity.
Black Hole Universe -BH in an expanding box- Yoo, Chulmoon ( YITP) Hiroyuki Abe (Osaka City Univ.) Ken-ichi Nakao (Osaka City Univ.) Yohsuke Takamori (Osaka.
The Meaning of Einstein’s Equation*
Relativistic Stars with Magnetic Fields
Gravitational Self-force on a Particle in the Schwarzschild background Hiroyuki Nakano (Osaka City) Norichika Sago (Osaka) Wataru Hikida (Kyoto, YITP)
Universe Tenth Edition
ON EXISTENCE OF HALO ORBITS IN COMPACT OBJECTS SPACETIMES Jiří Kovář Zdeněk Stuchlík & Vladimír Karas Institute of Physics Silesian University in Opava.
1 Yasushi Mino ( 蓑 泰 志 ) WUGRAV, Washington University at St. Louis Index 1: Introduction 2: Self-force in a Linear Perturbation.
Wednesday, Apr. 6, 2005PHYS 3446, Spring 2005 Jae Yu 1 PHYS 3446 – Lecture #17 Wednesday, Apr. 6, 2005 Dr. Jae Yu Symmetries Local gauge symmetry Gauge.
Brief summaries on general relativity (II) Gungwon Kang (KISTI) July 26, 2015 at Int’l Summer School on NR & GW, KAIST in Korea.
Center of Mass and Spin in GR Newman-Kozameh Bariloche January 2009 TexPoint fonts used in EMF. Read the TexPoint manual before you delete this box.: AAAAAA.
Geometrically motivated, hyperbolic gauge conditions for Numerical Relativity Carlos Palenzuela Luque 15 December
BLACK HOLES SIMULATION and visualization
The Rotating Black Hole
A rotating hairy BH in AdS_3
Detection of gravitational waves from binary black hole mergers
Black Holes.
Honors Physics 1 Class 12 Fall 2013
From Einstein to Hawking : A journey through spacetime
A New Approach to Equation of Motion for a fast-moving particle
Thermodynamics of Kerr-AdS Black Holes
History of Black Hole Research
Santiago de Compostela, June 27, 2016 Aron Jansen
Spin and Quadrupole corrections to IMRIs
Presentation transcript:

Y.K.Lau Institute of Appl. Maths, CAS

Bondi Sachs Formulation of the Kerr Metric Gravitational Wave Physics of a Kerr Black Hole

Joint work with Shan Bai, Zhoujian Cao, Xuefei Gong, Xiaoning Wu IAM, AMSS Yuguang Shi Peking University

Numerical Relativity Numerical Simulation Using Large Scale Computation Compute Gravitational Waveform Data Mining Of Experimental Database Relativistic Two body Einstein field equations

Angular momentum carries away gravitational radiation Rotating star Gravitational radiation emitted

Wavefront Tracking

Distortion of wavefront by angular momentum of the source ?

Constant time slice Wavefront Two sphere as snapshot of wave front

Describes the distortion of the two sphere Eigenvectors Two states of polarization of GW

Why Angular Momentum is Tough?

Dilemma In need of a pragmatic description at the level of application Lack of good theoretic foundation

Kerr Metric of a Prototype of Rotating Source

Motivations for Studying Kerr Waveform generated by Rotating Star Extreme Mass Ratio Inspiral Problem (LISA Template) Stability of Black Hole ………..

Kerr black hole in Boyer- Lindquist coordinate Dragging effect of star’s angular momentum

Construction of Wavefronts Solution of Eikonal Equation

Eikonal Equation

Asymptotic Solution as r tends to infinity

Moving frame adapted to the null hypersurface

Conserved Quantity for Gravitational Radiation Field Maxwell Theory: Total Charge Conserved General Relativity: Mass, Momentum, Angular Momentum are not conserved!

Newman Penrose Constants Newman-Penrose Constants Absolutely Conserved at Null Infinity

NP const defined NP constant---independent on the wavefront that intersects infinity # of NP constants=10

NP constants constructed from the multipole expansion of the ingoing radiation field

# of NP constants=10 Definition of NP constants reads: u -- time measured at null infinity

Newman Penrose Constants …..Another problem is to understand the significance (either mathematical or physical) of a certain curious set of ten exactly conserved asymptotically defined quantities ….. Roger Penrose “Unsolved Problems in General Relativity” in “Seminars in Differential Geometry” edited by S.T.Yau, Princeton Univ. Press, 1982

Mathematical Physical Constraint of NP constants to initial data? What role will the NP constants play in the evolution of field eqs? Are there deeper physical meaning for these absolute conserved quantities?

NP constant of Kerr spacetime NP constants of Kerr spacetime all vanish!

Evolution of Binary Stars No hair theorem means Kerr end state NP constant vanishes for generic initial data set ?

NP constants for binary system (Dain and Kroon) What happens from binary to Kerr? Possible ways out of this dilemma?

Journey to the Promised Land Numerical Simulation of the angular momentum of gravitational waves generated by tidal distortion of Kerr Understand better the Newman Penrose Constant in Binary Black Hole Spacetime