Gravitational Waves: Volume 1: Theory and Experiments |
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xvi | |
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Part I: Gravitational-wave theory |
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1 | (332) |
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1 The geometric approach to GWs |
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3 | (49) |
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1.1 Expansion around flat space |
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4 | (3) |
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1.2 The transverse-traceless gauge |
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7 | (6) |
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1.3 Interaction of GWs with test masses |
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13 | (13) |
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1.3.1 Geodesic equation and geodesic deviation |
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13 | (2) |
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1.3.2 Local inertial frames and freely falling frames |
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15 | (2) |
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1.3.3 TT frame and proper detector frame |
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17 | (9) |
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26 | (14) |
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1.4.1 Separation of GWs from the background |
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27 | (2) |
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1.4.2 How GWs curve the background |
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29 | (6) |
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1.4.3 The energy-momentum tensor of GWs |
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35 | (5) |
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1.5 Propagation in curved space-time |
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40 | (8) |
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1.5.1 Geometric optics in curved space |
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42 | (4) |
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1.5.2 Absorption and scattering of GWs |
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46 | (2) |
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48 | (3) |
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1.1 Linearization of the Riemann tensor in curved space |
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48 | (1) |
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1.2 Gauge transformation of hμupsilon and R(1)μupsilonρσ |
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49 | (2) |
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51 | (1) |
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2 The field-theoretical approach to GWs |
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52 | (49) |
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2.1 Linearized gravity as a classical field theory |
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53 | (13) |
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53 | (5) |
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2.1.2 The energy-momentum tensor of GWs |
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58 | (3) |
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2.1.3 The angular momentum of GWs |
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61 | (5) |
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66 | (15) |
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2.2.1 Why a spin-2 field? |
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66 | (4) |
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2.2.2 The Pauli-Fierz action |
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70 | (4) |
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2.2.3 From gravitons to gravity |
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74 | (5) |
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2.2.4 Effective field theories and the Planck scale |
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79 | (2) |
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81 | (14) |
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2.3.1 Phenomenological bounds |
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82 | (2) |
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2.3.2 Field theory of massive gravitons |
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84 | (11) |
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95 | (5) |
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2.1 The helicity of gravitons |
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95 | (3) |
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2.2 Angular momentum and parity of graviton states |
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98 | (2) |
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100 | (1) |
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3 Generation of GWs in linearized theory |
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101 | (66) |
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3.1 Weak-field sources with arbitrary velocity |
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102 | (3) |
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3.2 Low-velocity expansion |
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105 | (4) |
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3.3 Mass quadrupole radiation |
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109 | (16) |
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3.3.1 Amplitude and angular distribution |
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109 | (4) |
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113 | (1) |
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3.3.3 Radiated angular momentum |
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114 | (2) |
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3.3.4 Radiation reaction on non-relativistic sources |
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116 | (5) |
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3.3.5 Radiation from a closed system of point masses |
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121 | (4) |
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3.4 Mass octupole and current quadrupole |
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125 | (6) |
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3.5 Systematic multipole expansion |
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131 | (25) |
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3.5.1 Symmetric-trace-free (STF) form |
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134 | (5) |
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3.5.2 Spherical tensor form |
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139 | (17) |
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156 | (1) |
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3.1 Quadrupole radiation from an oscillating mass |
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156 | (2) |
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3.2 Quadrupole radiation from a mass in circular orbit |
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158 | (3) |
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3.3 Mass octupole and current quadrupole radiation from a mass in circular orbit |
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161 | (2) |
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3.4 Decomposition of Skl,m into irreducible representations of SO(3) |
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163 | (2) |
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3.5 Computation of integral dΩ(TE2B2lm)*ijni1...niα |
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165 | (1) |
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166 | (1) |
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167 | (69) |
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4.1 Inspiral of compact binaries |
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167 | (33) |
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4.1.1 Circular orbits. The chirp amplitude |
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169 | (7) |
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4.1.2 Elliptic orbits. (I) Total power and frequency spectrum of the radiation emitted |
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176 | (8) |
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4.1.3 Elliptic orbits. (II) Evolution of the orbit under back-reaction |
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184 | (6) |
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4.1.4 Binaries at cosmological distances |
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190 | (10) |
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4.2 Radiation from rotating rigid bodies |
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200 | (15) |
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4.2.1 GWs from rotation around a principal axis |
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201 | (3) |
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4.2.2 GWs from freely precessing rigid bodies |
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204 | (11) |
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4.3 Radial infall into a black hole |
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215 | (9) |
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4.3.1 Radiation from an infalling point-like mass |
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215 | (4) |
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4.3.2 Tidal disruption of a real star falling into a black hole. Coherent and incoherent radiation |
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219 | (5) |
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4.4 Radiation from accelerated masses |
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224 | (6) |
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4.4.1 GWs produced in elastic collisions |
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224 | (3) |
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4.4.2 Lack of beaming of GWs from accelerated masses |
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227 | (3) |
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230 | (5) |
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4.1 Fourier transform of the chirp signal |
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230 | (3) |
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4.2 Fourier decomposition of elliptic Keplerian motion |
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233 | (2) |
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235 | (1) |
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5 GW generation by post-Newtonian sources |
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236 | (66) |
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5.1 The post-Newtonian expansion |
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237 | (13) |
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5.1.1 Slowly moving, weakly self-gravitating sources |
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237 | (2) |
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5.1.2 PN expansion of Einstein equations |
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239 | (1) |
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240 | (2) |
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242 | (3) |
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5.1.5 Motion of test particles in the PN metric |
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245 | (2) |
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5.1.6 Difficulties of the PN expansion |
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247 | (2) |
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5.1.7 The effect of back-reaction |
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249 | (1) |
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5.2 The relaxed Einstein equations |
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250 | (3) |
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5.3 The Blanchet-Damour approach |
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253 | (26) |
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5.3.1 Post-Minkowskian expansion outside the source |
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253 | (6) |
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5.3.2 PN expansion in the near region |
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259 | (4) |
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5.3.3 Matching of the solutions |
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263 | (3) |
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5.3.4 Radiative fields at infinity |
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266 | (9) |
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275 | (4) |
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279 | (3) |
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5.5 Strong-field sources and the effacement principle |
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282 | (7) |
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5.6 Radiation from inspiraling compact binaries |
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289 | (10) |
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5.6.1 The need for a very high-order computation |
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290 | (2) |
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5.6.2 The 3.5PN equations of motion |
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292 | (2) |
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5.6.3 Energy flux and orbital phase to 3.5PN order |
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294 | (2) |
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296 | (3) |
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299 | (3) |
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6 Experimental observation of GW emission in compact binaries |
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302 | (31) |
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6.1 The Hulse-Taylor binary pulsar |
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302 | (3) |
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6.2 The pulsar timing formula |
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305 | (21) |
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6.2.1 Pulsars as stable clocks |
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305 | (1) |
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6.2.2 Roemer, Shapiro and Einstein time delays |
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306 | (8) |
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6.2.3 Relativistic corrections for binary pulsars |
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314 | (12) |
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6.3 The double pulsar, and more compact binaries |
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326 | (5) |
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331 | (2) |
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Part II: Gravitational-wave experiments |
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333 | (204) |
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7 Data analysis techniques |
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335 | (80) |
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7.1 The noise spectral density |
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335 | (4) |
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7.2 Pattern functions and angular sensitivity |
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339 | (4) |
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343 | (3) |
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7.4 Probability and statistics |
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346 | (15) |
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7.4.1 Frequentist and Bayesian approaches |
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346 | (4) |
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7.4.2 Parameters estimation |
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350 | (6) |
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7.4.3 Matched filtering statistics |
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356 | (5) |
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361 | (10) |
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7.5.1 Optimal signal-to-noise ratio |
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361 | (4) |
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7.5.2 Time-frequency analysis |
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365 | (4) |
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369 | (2) |
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371 | (16) |
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7.6.1 Amplitude modulation |
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373 | (2) |
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7.6.2 Doppler shift and phase modulation |
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375 | (6) |
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7.6.3 Efficient search algorithms |
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381 | (6) |
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7.7 Coalescence of compact binaries |
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387 | (5) |
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7.7.1 Elimination of extrinsic variables |
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388 | (2) |
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7.7.2 The sight distance to coalescing binaries |
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390 | (2) |
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7.8 Stochastic backgrounds |
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392 | (21) |
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7.8.1 Characterization of stochastic backgrounds |
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393 | (4) |
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7.8.2 SNR for single detectors |
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397 | (3) |
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7.8.3 Two-detector correlation |
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400 | (13) |
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413 | (2) |
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8 Resonant-mass detectors |
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415 | (55) |
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8.1 The interaction of GWs with an elastic body |
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415 | (12) |
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8.1.1 The response to bursts |
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415 | (5) |
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8.1.2 The response to periodic signals |
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420 | (1) |
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8.1.3 The absorption cross-section |
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421 | (6) |
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8.2 The read-out system: how to measure extremely small displacements |
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427 | (9) |
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8.2.1 The double oscillator |
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428 | (4) |
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8.2.2 Resonant transducers |
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432 | (4) |
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436 | (23) |
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437 | (6) |
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8.3.2 Read-out noise and effective temperature |
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443 | (3) |
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8.3.3 Back-action noise and the quantum limit |
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446 | (3) |
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8.3.4 Quantum non-demolition measurements |
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449 | (4) |
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8.3.5 Experimental sensitivities |
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453 | (6) |
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459 | (10) |
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8.4.1 The interaction of a sphere with GWs |
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459 | (7) |
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8.4.2 Spheres as multi-mode detectors |
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466 | (3) |
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469 | (1) |
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470 | |
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9.1 A simple Michelson interferometer |
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470 | (10) |
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9.1.1 The interaction with GWs in the TT gauge |
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471 | (5) |
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9.1.2 The interaction in the proper detector frame |
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476 | (4) |
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9.2 Interferometers with Fabry-Perot cavities |
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480 | (17) |
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9.2.1 Electromagnetic fields in a FP cavity |
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480 | (9) |
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9.2.2 Interaction of a FP cavity with GWs |
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489 | (5) |
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9.2.3 Angular sensitivity and pattern functions |
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494 | (3) |
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9.3 Toward a real GW interferometer |
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497 | (18) |
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9.3.1 Diffraction and Gaussian beams |
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497 | (7) |
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9.3.2 Detection at the dark fringe |
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504 | (6) |
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9.3.3 Basic optical layout |
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510 | (1) |
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9.3.4 Controls and locking |
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511 | (4) |
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515 | (13) |
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516 | (3) |
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519 | (3) |
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9.4.3 The standard quantum limit |
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522 | (2) |
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524 | (4) |
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9.5 Existing and planned detectors |
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528 | (7) |
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9.5.1 Initial interferometers |
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528 | (4) |
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9.5.2 Advanced interferometers |
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532 | (3) |
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535 | (2) |
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537 | (12) |
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549 | |
Gravitational Waves: Volume 2: Astrophysics and Cosmology |
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Part III: Astrophysical sources of gravitational waves |
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1 | (366) |
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3 | (71) |
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10.1 Historical Supernovae |
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4 | (6) |
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10.2 Properties of Supernovae |
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10 | (11) |
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11 | (4) |
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15 | (3) |
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18 | (3) |
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10.3 The dynamics of core collapse |
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21 | (14) |
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21 | (4) |
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10.3.2 Core collapse and neutrino-driven delayed shock |
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25 | (5) |
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10.3.3 The remnant of the collapse |
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30 | (5) |
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10.4 GW production by self-gravitating fluids |
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35 | (11) |
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10.4.1 Energy-momentum tensor of a perfect fluid |
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35 | (3) |
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10.4.2 GW production from gravitating Newtonian fluids |
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38 | (4) |
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10.4.3 Quadrupole radiation from axisymmetric sources |
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42 | (4) |
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10.5 GWs from stellar collapse |
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46 | (20) |
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10.5.1 GWs from collapse and bounce of rotating cores |
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47 | (4) |
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10.5.2 GWs from bar-mode instabilities |
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51 | (4) |
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10.5.3 GWs from post-bounce convective instabilities |
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55 | (2) |
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10.5.4 GWs from anisotropic neutrino emission |
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57 | (5) |
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10.5.5 GWs from magneto-rotational core collapse |
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62 | (3) |
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10.5.6 GWs from fragmentation during collapse |
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65 | (1) |
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10.6 Complements: luminosity, color and metallicity of stars |
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66 | (5) |
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71 | (3) |
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74 | (41) |
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11.1 Observations of neutron stars |
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74 | (15) |
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11.1.1 The discovery of pulsars |
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74 | (1) |
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11.1.2 Pulsar spindown and the P-P plane |
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75 | (5) |
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11.1.3 Millisecond pulsars |
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80 | (1) |
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81 | (2) |
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11.1.5 SGRs and magnetars |
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83 | (6) |
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11.2 GW emission from neutron stars |
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89 | (22) |
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89 | (10) |
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11.2.2 The CFS instability |
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99 | (7) |
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11.2.3 GWs from post-merger NS remnants |
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106 | (2) |
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11.2.4 GWs from deformed rotating NS |
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108 | (3) |
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111 | (4) |
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12 Black-hole perturbation theory |
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115 | (74) |
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12.1 Scalar perturbations |
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115 | (2) |
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12.2 Gravitational perturbations |
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117 | (23) |
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12.2.1 Zerilli tensor harmonics |
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118 | (5) |
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12.2.2 The Regge-Wheeler gauge |
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123 | (4) |
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12.2.3 Axial perturbations: Regge-Wheeler equation |
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127 | (3) |
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12.2.4 Polar perturbations: Zerilli equation |
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130 | (1) |
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12.2.5 Boundary conditions |
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131 | (2) |
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12.2.6 The radiation field in the far zone |
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133 | (5) |
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138 | (2) |
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12.3 Black-hole quasi-normal modes |
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140 | (24) |
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12.3.1 General discussion |
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140 | (4) |
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12.3.2 QNMs from Laplace transform |
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144 | (7) |
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151 | (6) |
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12.3.4 Frequency spectrum of QNMs |
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157 | (5) |
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12.3.5 The physical interpretation of the QNM spectrum |
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162 | (2) |
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12.4 Radial infall into a black hole |
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164 | (4) |
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165 | (1) |
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12.4.2 Numerical integration of the Zerilli equation |
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166 | (1) |
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12.4.3 Waveform and energy spectrum |
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167 | (1) |
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12.5 Perturbations of rotating black holes |
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168 | (12) |
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169 | (4) |
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12.5.2 Null tetrads and the Newman-Penrose formalism |
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173 | (4) |
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12.5.3 Teukolsky equation and QNMs of rotating BHs |
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177 | (3) |
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180 | (6) |
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12.1 Derivation of the Zerilli equation |
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180 | (4) |
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12.2 The source term for radial infall |
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184 | (2) |
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186 | (3) |
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13 Properties of dynamical space-times |
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189 | (21) |
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13.1 The 3+1 decomposition of space-time |
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189 | (3) |
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13.2 Boundary terms in the gravitational action |
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192 | (3) |
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13.3 Hamiltonian formulation of GR |
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195 | (2) |
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13.4 Conserved quantities for isolated systems |
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197 | (10) |
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13.5 GWs and Newman-Penrose scalar |
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207 | (2) |
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209 | (1) |
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14 GWs from compact binaries. Theory |
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210 | (67) |
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14.1 Non-perturbative resummations. A simple example |
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212 | (5) |
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14.2 Effective one-body action |
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217 | (24) |
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14.2.1 Equivalence to a one-body problem |
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217 | (10) |
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14.2.2 Conservative dynamics |
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227 | (3) |
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14.2.3 Inclusion of radiation reaction |
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230 | (1) |
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231 | (5) |
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236 | (5) |
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14.3 Numerical relativity |
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241 | (24) |
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14.3.1 Numerical integration of Einstein equations |
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241 | (3) |
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14.3.2 Equal-mass non-spinning BH binaries |
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244 | (4) |
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14.3.3 Unequal-mass non-spinning BH binaries |
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248 | (2) |
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250 | (3) |
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14.3.5 Spinning BHs and superkicks |
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253 | (7) |
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14.3.6 Astrophysical consequences of BH recoil |
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260 | (5) |
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14.4 GWs from NS-NS binaries |
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265 | (8) |
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14.4.1 Inspiral phase and tidal effects |
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265 | (5) |
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14.4.2 Merger phase and numerical relativity |
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270 | (3) |
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273 | (4) |
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15 GWs from compact binaries. Observations |
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277 | (50) |
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15.1 GW150914. The first direct detection |
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278 | (12) |
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15.1.1 Evaluation of the statistical significance |
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279 | (6) |
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15.1.2 Properties of GW150914 |
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285 | (5) |
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15.2 Further BH-BH detections |
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290 | (9) |
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290 | (3) |
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293 | (1) |
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294 | (1) |
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15.2.4 GW170814: the first three-detector observation |
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295 | (2) |
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15.2.5 The population of BH-BH binaries |
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297 | (2) |
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15.3 GW170817: the first NS-NS binary |
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299 | (15) |
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299 | (2) |
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15.3.2 The prompt-γ-ray burst |
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301 | (5) |
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15.3.3 The electromagnetic counterpart |
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306 | (3) |
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15.3.4 Kilonovae and r-process nucleosynthesis |
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309 | (2) |
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15.3.5 The cocoon scenario |
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311 | (3) |
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15.4 Tests of fundamental physics |
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314 | (8) |
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15.4.1 BH quasi-normal modes |
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314 | (2) |
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15.4.2 Tests of post-Newtonian gravity |
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316 | (1) |
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15.4.3 Propagation and degrees of freedom of GWs |
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317 | (5) |
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322 | (5) |
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16 Supermassive black holes |
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327 | (40) |
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16.1 The central supermassive black hole in our Galaxy |
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327 | (3) |
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16.2 Supermassive black-hole binaries |
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330 | (9) |
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16.2.1 Formation and evolution of SMBH binaries |
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330 | (4) |
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16.2.2 SMBH binaries at LISA |
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334 | (5) |
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16.3 Extreme mass ratio inspirals |
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339 | (10) |
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16.3.1 Formation mechanisms |
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339 | (2) |
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341 | (2) |
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16.3.3 Waveforms and the self-force approach |
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343 | (6) |
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16.4 Stochastic GWs from SMBH binaries |
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349 | (14) |
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16.4.1 Regime dominated by GW back-reaction |
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351 | (1) |
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16.4.2 Regime dominated by three-body interactions |
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352 | (3) |
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16.4.3 High-frequency regime and source discreteness |
|
|
355 | (2) |
|
16.4.4 Estimates of the SMBH merger rate |
|
|
357 | (2) |
|
16.4.5 Effect of the eccentricity |
|
|
359 | (4) |
|
|
363 | (4) |
|
Part IV: Cosmology and gravitational waves |
|
|
367 | (377) |
|
17 Basics of FRW cosmology |
|
|
369 | (43) |
|
|
369 | (5) |
|
17.1.1 Comoving and physical coordinates |
|
|
370 | (1) |
|
17.1.2 Comoving and physical momenta |
|
|
371 | (3) |
|
17.2 Cosmological background equations for a single fluid |
|
|
374 | (3) |
|
17.3 Multi-component fluids |
|
|
377 | (4) |
|
17.4 RD-MD equilibrium, recombination and decoupling |
|
|
381 | (2) |
|
17.5 Effective number of relativistic species |
|
|
383 | (5) |
|
17.6 Conformal time and particle horizon |
|
|
388 | (9) |
|
17.6.1 Radiation dominance |
|
|
389 | (2) |
|
|
391 | (1) |
|
17.6.3 Analytic formulas in RD-EMD |
|
|
392 | (1) |
|
|
393 | (1) |
|
17.6.5 Conformal time at significant epochs |
|
|
393 | (2) |
|
17.6.6 Comoving distance, angular diameter distance and luminosity distance |
|
|
395 | (2) |
|
17.7 Newtonian cosmology inside the horizon |
|
|
397 | (14) |
|
17.7.1 Newtonian dynamics in expanding backgrounds |
|
|
398 | (4) |
|
17.7.2 Newtonian fluid dynamics in an expanding Universe |
|
|
402 | (9) |
|
|
411 | (1) |
|
18 Helicity decomposition of metric perturbations |
|
|
412 | (25) |
|
18.1 Perturbations around flat space |
|
|
413 | (8) |
|
18.1.1 Helicity decomposition |
|
|
413 | (5) |
|
18.1.2 Radiative and non-radiative degrees of freedom |
|
|
418 | (3) |
|
18.2 Gauge invariance and helicity decomposition in FRW |
|
|
421 | (4) |
|
18.2.1 Linearized diffeomorphisms and gauge invariance in a curved background |
|
|
421 | (1) |
|
|
422 | (3) |
|
18.3 Perturbed energy-momentum tensor |
|
|
425 | (11) |
|
18.3.1 General decomposition of Tμν |
|
|
426 | (2) |
|
18.3.2 Perturbations of perfect fluids |
|
|
428 | (3) |
|
18.3.3 Linearized energy-momentum conservation |
|
|
431 | (3) |
|
18.3.4 Gauge-invariant combinations |
|
|
434 | (2) |
|
|
436 | (1) |
|
19 Evolution of cosmological perturbations |
|
|
437 | (70) |
|
19.1 Evolution equations in the scalar sector |
|
|
437 | (10) |
|
19.1.1 Single-component fluid |
|
|
439 | (2) |
|
19.1.2 Multi-component fluid |
|
|
441 | (2) |
|
19.1.3 Super-horizon and sub-horizon regimes |
|
|
443 | (4) |
|
|
447 | (7) |
|
19.2.1 Adiabatic and isocurvature perturbations |
|
|
449 | (2) |
|
19.2.2 The variables ζ and R |
|
|
451 | (3) |
|
19.3 Solutions of the equations for scalar perturbations |
|
|
454 | (10) |
|
19.3.1 Numerical integration |
|
|
454 | (4) |
|
19.3.2 Analytic solutions in RD |
|
|
458 | (3) |
|
19.3.3 Analytic solutions in MD |
|
|
461 | (2) |
|
19.3.4 Analytic solutions during dark-energy dominance |
|
|
463 | (1) |
|
19.4 Power spectra for scalar perturbations |
|
|
464 | (10) |
|
19.4.1 Definitions and conventions |
|
|
464 | (2) |
|
19.4.2 The primordial power spectrum |
|
|
466 | (3) |
|
19.4.3 Transfer function and growth rate |
|
|
469 | (3) |
|
19.4.4 The linearly processed power spectrum |
|
|
472 | (2) |
|
19.5 Tensor perturbations |
|
|
474 | (18) |
|
19.5.1 Cosmological evolution |
|
|
474 | (8) |
|
19.5.2 Transfer function for tensor modes |
|
|
482 | (4) |
|
19.5.3 GW damping from neutrino free-streaming |
|
|
486 | (2) |
|
19.5.4 The tensor power spectrum, &Qmega;gw(f) and hc(f) |
|
|
488 | (4) |
|
19.6 Standard sirens, dark energy and modified gravity |
|
|
492 | (13) |
|
19.6.1 Testing cosmological models against observations |
|
|
494 | (2) |
|
19.6.2 Cosmology with standard sirens |
|
|
496 | (4) |
|
19.6.3 Tensor perturbations in modified gravity |
|
|
500 | (2) |
|
19.6.4 An explicit example: non-local gravity |
|
|
502 | (3) |
|
|
505 | (2) |
|
20 The imprint of GWs on the CMB |
|
|
507 | (67) |
|
|
507 | (5) |
|
|
512 | (5) |
|
20.3 Temperature anisotropies at large angles |
|
|
517 | (28) |
|
20.3.1 Photon geodesics in a perturbed FRW metric |
|
|
517 | (2) |
|
20.3.2 Sachs-Wolfe, ISW and Doppler contributions |
|
|
519 | (4) |
|
20.3.3 Expression of the Cl in terms of the Θl(k) |
|
|
523 | (3) |
|
20.3.4 Scalar contribution to the Cl |
|
|
526 | (4) |
|
20.3.5 Tensor contribution to the Cl |
|
|
530 | (8) |
|
20.3.6 Finite thickness of the LSS |
|
|
538 | (2) |
|
20.3.7 The Boltzmann equation for photons |
|
|
540 | (5) |
|
|
545 | (26) |
|
|
545 | (3) |
|
20.4.2 Polarization maps. E and B modes |
|
|
548 | (3) |
|
20.4.3 Polarization and tensor spherical harmonics |
|
|
551 | (7) |
|
20.4.4 Generation of CMB polarization |
|
|
558 | (11) |
|
20.4.5 Experimental situation |
|
|
569 | (2) |
|
|
571 | (3) |
|
21 Inflation and primordial perturbations |
|
|
574 | (70) |
|
21.1 Inflationary cosmology |
|
|
574 | (21) |
|
21.1.1 The flatness problem |
|
|
574 | (4) |
|
21.1.2 The horizon problem |
|
|
578 | (2) |
|
21.1.3 Single-field slow-roll inflation |
|
|
580 | (4) |
|
21.1.4 Large-field and small-field inflation |
|
|
584 | (6) |
|
|
590 | (5) |
|
21.2 Quantum fields in curved space |
|
|
595 | (15) |
|
21.2.1 Field quantization in curved space |
|
|
595 | (6) |
|
21.2.2 Quantum fields in a FRW background |
|
|
601 | (2) |
|
21.2.3 Vacuum fluctuations in de Sitter inflation |
|
|
603 | (7) |
|
21.3 Primordial perturbations in single-field slow-roll inflation |
|
|
610 | (31) |
|
21.3.1 Mukhanov-Sasaki equation |
|
|
611 | (2) |
|
21.3.2 Scalar perturbations to lowest order in slowroll |
|
|
613 | (1) |
|
21.3.3 Scalar perturbations to first order. Spectral tilt |
|
|
614 | (6) |
|
21.3.4 Tensor perturbations |
|
|
620 | (4) |
|
21.3.5 Predictions from a sample of inflationary models |
|
|
624 | (5) |
|
21.3.6 The relic inflationary GW background today |
|
|
629 | (7) |
|
21.3.7 A full quantum computation of Ωgw(f) |
|
|
636 | (5) |
|
|
641 | (3) |
|
22 Stochastic backgrounds of cosmological origin |
|
|
644 | (79) |
|
22.1 Characteristic frequency of relic GWs |
|
|
644 | (3) |
|
22.2 GW production by classical fields |
|
|
647 | (6) |
|
|
647 | (4) |
|
22.2.2 GW generation by a stochastic scalar field |
|
|
651 | (2) |
|
22.3 GWs from preheating after inflation |
|
|
653 | (4) |
|
22.3.1 Parametric resonance in single-field inflation |
|
|
653 | (3) |
|
22.3.2 Tachyonic preheating in hybrid inflation |
|
|
656 | (1) |
|
22.4 GWs from first-order phase transitions |
|
|
657 | (27) |
|
22.4.1 Crossovers and phase transitions |
|
|
657 | (4) |
|
22.4.2 First-order phase transitions in cosmology |
|
|
661 | (2) |
|
22.4.3 Thermal tunneling theory |
|
|
663 | (12) |
|
22.4.4 Bubble dynamics and GW production |
|
|
675 | (9) |
|
|
684 | (21) |
|
22.5.1 Global and local strings |
|
|
684 | (4) |
|
22.5.2 Effective description and Nambu-Goto action |
|
|
688 | (4) |
|
22.5.3 String dynamics. Cusps and kinks |
|
|
692 | (5) |
|
22.5.4 Gravitational radiation from cosmic strings |
|
|
697 | (8) |
|
22.6 Alternatives to inflation |
|
|
705 | (5) |
|
22.7 Bounds on primordial GW backgrounds |
|
|
710 | (10) |
|
22.7.1 The nucleosynthesis bound |
|
|
710 | (7) |
|
22.7.2 Bounds on extra radiation from the CMB |
|
|
717 | (1) |
|
22.7.3 Bounds from the CMB at large angles |
|
|
718 | (1) |
|
22.7.4 Limits on stochastic backgrounds from interferometers |
|
|
719 | (1) |
|
|
720 | (3) |
|
23 Stochastic backgrounds and pulsar timing arrays |
|
|
723 | (21) |
|
23.1 GW effect on the timing of a single pulsar |
|
|
724 | (5) |
|
23.2 Response to a continuous signal |
|
|
729 | (1) |
|
23.3 Response to a stochastic GW background |
|
|
730 | (4) |
|
23.4 Extracting the GW signal from noise |
|
|
734 | (7) |
|
23.5 Searches for stochastic backgrounds with PTAs |
|
|
741 | (1) |
|
|
742 | (2) |
|
|
744 | (71) |
|
|
815 | |