Null infinity waveforms from extreme-mass-ratio inspirals in Kerr spacetime
暂无分享,去创建一个
[1] S. Bernuzzi,et al. Binary black hole coalescence in the extreme-mass-ratio limit: testing and improving the effective-one-body multipolar waveform , 2010, 1012.2456.
[2] W. Press,et al. Radiation fields in the Schwarzschild background , 1973 .
[3] Richard H. Price,et al. Nonspherical perturbations of relativistic gravitational collapse , 1971 .
[4] Anil Zenginoglu,et al. Gravitational perturbations of Schwarzschild spacetime at null infinity and the hyperboloidal initial value problem , 2008, 0810.1929.
[5] Gaurav Khanna,et al. Towards adiabatic waveforms for inspiral into Kerr black holes: A new model of the source for the time domain perturbation equation , 2007 .
[6] J. Stewart,et al. Linearized perturbations of the Kerr spacetime and outer boundary conditions in numerical relativity , 2011 .
[7] F. Zerilli,et al. Effective potential for even parity Regge-Wheeler gravitational perturbation equations , 1970 .
[8] Thibault Damour,et al. Transition from inspiral to plunge in binary black hole coalescences , 2000 .
[9] Y. Zlochower,et al. Binary black hole waveform extraction at null infinity , 2011, 1106.4841.
[10] F. D. Ryan. Accuracy of estimating the multipole moments of a massive body from the gravitational waves of a binary inspiral , 1997 .
[11] Constant crunch coordinates for black hole simulations , 2000, gr-qc/0005113.
[12] H. Pfeiffer,et al. Black hole initial data on hyperboloidal slices , 2009, 0907.3163.
[13] T. Damour,et al. Faithful effective-one-body waveforms of small-mass-ratio coalescing black-hole binaries , 2007, 0705.2519.
[14] Numerical Relativity with the Conformal Field Equations , 2002, gr-qc/0204057.
[15] S. Bernuzzi,et al. Binary black hole merger in the extreme-mass-ratio limit: a multipolar analysis , 2010, 1003.0597.
[16] Michael Jasiulek. Hyperboloidal slices for the wave equation of Kerr–Schild metrics and numerical applications , 2011, 1109.2513.
[17] Gaurav Khanna,et al. Towards adiabatic waveforms for inspiral into Kerr black holes. II. Dynamical sources and generic orbits , 2008, 0803.0317.
[18] F. D. Lora-Clavijo,et al. Evolution of a massless test scalar field on boson star space-times , 2010, 1007.1162.
[19] Gabor Zsolt Toth,et al. Numerical investigation of the late-time Kerr tails , 2011, 1104.4199.
[20] O. Rinne,et al. Regularity of the Einstein equations at future null infinity , 2008, 0811.4109.
[21] Anil Zenginoglu,et al. Hyperboloidal layers for hyperbolic equations on unbounded domains , 2010, J. Comput. Phys..
[22] Pasadena,et al. Gravitational waves from a compact star in a circular, inspiral orbit, in the equatorial plane of a massive, spinning black hole, as observed by LISA , 2000, gr-qc/0007074.
[23] Luciano Rezzolla,et al. Gauge-invariant non-spherical metric perturbations of Schwarzschild black-hole spacetimes , 2005 .
[24] S. Bernuzzi,et al. Binary black hole coalescence in the large-mass-ratio limit: The hyperboloidal layer method and waveforms at null infinity , 2011, 1107.5402.
[25] Subrahmanyan Chandrasekhar,et al. The Mathematical Theory of Black Holes , 1983 .
[26] A. Buonanno,et al. Modeling extreme mass ratio inspirals within the effective-one-body approach. , 2009, Physical review letters.
[27] A. Zimmerman,et al. New generic ringdown frequencies at the birth of a Kerr black hole , 2011, 1106.0782.
[28] Numerical integration of the Teukolsky equation in the time domain , 2004, gr-qc/0409065.
[29] J. Gair,et al. Improved approximate inspirals of test bodies into Kerr black holes , 2005, gr-qc/0510129.
[30] Anil Zenginoglu,et al. Asymptotics of Schwarzschild black hole perturbations , 2009, 0911.2450.
[31] Self force via a Green's function decomposition , 2002, gr-qc/0202086.
[32] F. Ohme,et al. Stationary hyperboloidal slicings with evolved gauge conditions , 2009, 0905.0450.
[33] J. Isenberg,et al. K‐surfaces in the Schwarzschild space‐time and the construction of lattice cosmologies , 1980 .
[34] S. Dolan,et al. Self-force via m-mode regularization and 2+1D evolution. II. Scalar-field implementation on Kerr spacetime , 2011, 1107.0012.
[35] Anil Zenginoglu,et al. Spacelike matching to null infinity , 2009, 0906.3342.
[36] Roger Penrose,et al. Zero rest-mass fields including gravitation: asymptotic behaviour , 1965, Proceedings of the Royal Society of London. Series A. Mathematical and Physical Sciences.
[37] J. Gair,et al. "Kludge"gravitational waveforms for a test-body orbiting a Kerr black hole , 2006, gr-qc/0607007.
[38] Luth,et al. Pseudospectral collocation methods for the computation of the self-force on a charged particle: Generic orbits around a Schwarzschild black hole , 2010, 1006.3201.
[39] Quasi-spherical light cones of the Kerr geometry , 1998, gr-qc/9803080.
[40] Roger Penrose,et al. Asymptotic properties of fields and space-times , 1963 .
[41] Thibault Damour,et al. Determination of the last stable orbit for circular general relativistic binaries at the third post-Newtonian approximation , 2000 .
[42] Marcus J. Grote,et al. Nonreflecting Boundary Conditions for Time-Dependent Scattering , 1996 .
[43] T. Damour,et al. Binary black hole merger in the extreme-mass-ratio limit , 2006, gr-qc/0612096.
[44] O. Sarbach,et al. Improved outer boundary conditions for Einstein's field equations , 2007, gr-qc/0703129.
[45] Thomas Hagstrom,et al. RADIATION BOUNDARY CONDITIONS FOR MAXWELL'S EQUATIONS: A REVIEW OF ACCURATE TIME-DOMAIN , 2007 .
[46] V. Cardoso,et al. Test bodies and naked singularities: is the self-force the cosmic censor? , 2010, Physical review letters.
[47] T. Damour,et al. Effective one-body approach to general relativistic two-body dynamics , 1999 .
[48] Michael Boyle,et al. Testing gravitational-wave searches with numerical relativity waveforms: results from the first Numerical INJection Analysis (NINJA) project , 2009, 0901.4399.
[49] Saul A. Teukolsky,et al. Perturbations of a rotating black hole. I. Fundamental equations for gravitational, electromagnetic, and neutrino-field perturbations , 1973 .
[50] Anil Zenginoglu,et al. Hyperboloidal evolution with the Einstein equations , 2008, Classical and Quantum Gravity.
[51] Larry Smarr,et al. Kinematical conditions in the construction of spacetime , 1978 .
[52] S. Orszag,et al. Numerical solution of problems in unbounded regions: Coordinate transforms , 1977 .
[53] Gaurav Khanna,et al. Binary black hole merger gravitational waves and recoil in the large mass ratio limit , 2010, 1003.0485.
[54] Anil Zenginoglu,et al. A hyperboloidal study of tail decay rates for scalar and Yang–Mills fields , 2008 .
[55] Anil Zenginoglu,et al. Saddle-point dynamics of a Yang–Mills field on the exterior Schwarzschild spacetime , 2010, 1005.1708.
[56] Anil Zenginoglu,et al. A geometric framework for black hole perturbations , 2011 .
[57] C. Misner,et al. Excising das All: Evolving Maxwell waves beyond Scri , 2006, gr-qc/0603034.
[58] Towards absorbing outer boundaries in general relativity , 2006, gr-qc/0608051.
[59] Anil Zenginoglu,et al. Hyperboloidal foliations and scri-fixing , 2007, Classical and Quantum Gravity.
[60] T. Tanaka,et al. Gravitational waves from extreme mass-ratio inspirals , 2008 .
[61] Anil Zenginoglu,et al. Hyperboloidal evolution of test fields in three spatial dimensions , 2010, 1004.0760.
[62] Stephen R. Lau. Rapid evaluation of radiation boundary kernels for time-domain wave propagation on blackholes: theory and numerical methods , 2004 .
[63] Leslie Greengard,et al. Rapid Evaluation of Nonreflecting Boundary Kernels for Time-Domain Wave Propagation , 2000, SIAM J. Numer. Anal..
[64] P. Diener,et al. Effective source approach to self-force calculations , 2011, 1101.2925.
[65] Stephen R. Lau,et al. Rapid evaluation of radiation boundary kernels for time-domain wave propagation on black holes: implementation and numerical tests , 2004 .
[66] Axiomatic approach to electromagnetic and gravitational radiation reaction of particles in curved spacetime , 1996, gr-qc/9610053.
[67] O. Rinne. An axisymmetric evolution code for the Einstein equations on hyperboloidal slices , 2009, 0910.0139.
[68] J. Bardeen,et al. Tetrad formalism for numerical relativity on conformally compactified constant mean curvature hypersurfaces , 2011, 1101.5479.
[69] Construction of Hyperboloidal Initial Data , 2002, gr-qc/0205083.
[70] Christian Reisswig,et al. Notes on the integration of numerical relativity waveforms , 2010, 1006.1632.
[71] B. Szilágyi,et al. Unambiguous determination of gravitational waveforms from binary black hole mergers. , 2009, Physical review letters.
[72] T. Hinderer,et al. Transient resonances in the inspirals of point particles into black holes. , 2010, Physical review letters.
[73] Numerical investigation of highly excited magnetic monopoles in SU(2) Yang-Mills-Higgs theory , 2006, hep-th/0609110.
[74] Kostas D. Kokkotas,et al. Quasi-Normal Modes of Stars and Black Holes , 1999, Living reviews in relativity.
[75] O. Sarbach,et al. Instability of charged wormholes supported by a ghost scalar field , 2009, 0906.0420.
[76] S. Teukolsky. ROTATING BLACK HOLES: SEPARABLE WAVE EQUATIONS FOR GRAVITATIONAL AND ELECTROMAGNETIC PERTURBATIONS. , 1972 .
[77] C. Gundlach,et al. Asymptotically null slices in numerical relativity: mathematical analysis and spherical wave equation tests , 2005, gr-qc/0512149.
[78] J. Gair,et al. 'Kludge' gravitational waveforms for a test-body orbiting a Kerr black hole , 2007 .
[79] Light cone structure near null infinity of the Kerr metric , 2007, gr-qc/0701171.
[80] Y. Mino,et al. Gravitational radiation from plunging orbits: Perturbative study , 2008, 0809.2814.
[81] A. Lun,et al. The Kerr spacetime in generalized Bondi?Sachs coordinates , 2003 .
[82] P. Laguna,et al. Dynamics of perturbations of rotating black holes , 1997 .
[83] H. Friedrich. On the existence ofn-geodesically complete or future complete solutions of Einstein's field equations with smooth asymptotic structure , 1986 .
[84] Helmut Friedrich,et al. Cauchy problems for the conformal vacuum field equations in general relativity , 1983 .
[85] Larry Smarr,et al. Time functions in numerical relativity: Marginally bound dust collapse , 1979 .
[86] W. Marsden. I and J , 2012 .
[87] R. Price,et al. Nonspherical Perturbations of Relativistic Gravitational Collapse. I. Scalar and Gravitational Perturbations , 1972 .
[88] A. Buonanno,et al. Extreme Mass-Ratio Inspirals in the Effective-One-Body Approach: Quasi-Circular, Equatorial Orbits around a Spinning Black Hole , 2010, 1009.6013.
[89] John Archibald Wheeler,et al. Stability of a Schwarzschild singularity , 1957 .
[90] L. Price,et al. Gravitational self-force for a particle in circular orbit around the Schwarzschild black hole , 2010 .
[91] Saul A. Teukolsky,et al. Perturbations of a rotating black hole , 1974 .
[92] Ernst Nils Dorband,et al. Gravitational-wave detectability of equal-mass black-hole binaries with aligned spins , 2009, 0907.0462.