Preface |
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xiii | |
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1 Gravitational waves, theory and experiment (an overview) |
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1 | (10) |
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9 | (2) |
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PART I Gravitational Waves, Sources and Detectors |
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11 | (78) |
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13 | (2) |
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2 Elements of gravitational waves |
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15 | (9) |
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2.1 Mathematics of linearized theory |
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16 | (1) |
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2.2 Using the TT gauge to understand gravitational waves |
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17 | (2) |
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2.3 Interaction of gravitational waves with detectors |
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19 | (2) |
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2.4 Analysis of beam detectors |
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21 | (1) |
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2.4.1 Ranging to spacecraft |
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21 | (1) |
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22 | (1) |
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22 | (1) |
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2.5 Exercises for chapter 2 |
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22 | (2) |
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3 Gravitational-wave detectors |
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24 | (19) |
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3.1 Gravitational-wave observables |
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26 | (2) |
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3.2 The physics of interferometers |
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28 | (6) |
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3.2.1 New interferometers and their capabilities |
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32 | (2) |
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3.3 The physics of resonant mass detectors |
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34 | (4) |
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3.3.1 New bar detectors and their capabilities |
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37 | (1) |
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38 | (3) |
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3.4.1 LISA's capabilities |
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39 | (2) |
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3.5 Gravitational and electromagnetic waves compared and contrasted |
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41 | (2) |
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4 Astrophysics of gravitational-wave sources |
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43 | (7) |
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4.1 Sources detectable from ground and from space |
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43 | (7) |
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4.1.1 Supernovae and gravitational collapse |
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43 | (1) |
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44 | (1) |
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4.1.3 Chirping binary systems |
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44 | (2) |
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4.1.4 Pulsars and other spinning neutron stars |
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46 | (2) |
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48 | (1) |
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49 | (1) |
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50 | (8) |
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5.1 Variational principle for general relativity |
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50 | (1) |
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5.2 Variational principles and the energy in gravitational waves |
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51 | (3) |
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5.2.1 Gauge transformation and invariance |
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52 | (1) |
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5.2.2 Gravitational-wave action |
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52 | (2) |
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5.3 Practical applications of the Isaacson energy |
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54 | (2) |
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5.3.1 Curvature produced by waves |
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55 | (1) |
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5.3.2 Cosmological background of radiation |
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55 | (1) |
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56 | (1) |
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5.4 Exercises for chapter 5 |
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56 | (2) |
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6 Mass- and current-quadrupole radiation |
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58 | (13) |
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6.1 Expansion for the far field of a slow-motion source |
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58 | (2) |
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6.2 Application of the TT gauge to the mass quadrupole field |
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60 | (4) |
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6.2.1 The TT gauge transformations |
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60 | (1) |
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6.2.2 Quadrupole field in the TT gauge |
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61 | (1) |
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6.2.3 Radiation patterns related to the motion of sources |
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62 | (2) |
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6.3 Application of the TT gauge to the current-quadrupole field |
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64 | (4) |
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6.3.1 The field at third order in slow-motion |
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64 | (1) |
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6.3.2 Separating the current quadrupole from the mass octupole |
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65 | (2) |
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6.3.3 A model system radiating current-quadrupole radiation |
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67 | (1) |
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6.4 Energy radiated in gravitational waves |
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68 | (2) |
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6.4.1 Mass-quadrupole radiation |
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69 | (1) |
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6.4.2 Current-quadrupole radiation |
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69 | (1) |
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6.5 Radiation in the Newtonian limit |
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70 | (1) |
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71 | (18) |
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7.1 Radiation from a binary system |
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71 | (2) |
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73 | (1) |
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73 | (7) |
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7.2.1 Linear growth of the r-modes |
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76 | (1) |
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7.2.2 Nonlinear evolution of the star |
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77 | (2) |
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7.2.3 Detection of r-mode radiation |
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79 | (1) |
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80 | (1) |
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81 | (3) |
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84 | (5) |
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PART 2 Gravitational-wave detectors |
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89 | (90) |
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8 Resonant detectors for gravitational waves and their bandwidth |
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91 | (12) |
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8.1 Sensitivity and bandwidth of resonant detectors |
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91 | (4) |
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8.2 Sensitivity for various GW signals |
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95 | (4) |
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8.3 Recent results obtained with the resonant detectors |
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99 | (2) |
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8.4 Discussion and conclusions |
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101 | (1) |
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102 | (1) |
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9 The Earth-based large interferometer Virgo and the Low Frequency Facility |
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103 | (12) |
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103 | (5) |
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9.1.1 Interferometer principles and Virgo parameters |
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104 | (4) |
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9.2 The SA suspension and requirements on the control |
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108 | (3) |
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9.3 A few words about the Low Frequency Facility |
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111 | (1) |
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112 | (2) |
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114 | (1) |
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10 LISA: A proposed joint ESA--NASA gravitational-wave mission |
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115 | (37) |
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10.1 Description of the LISA mission |
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115 | (17) |
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115 | (1) |
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10.1.2 Overall antenna and spacecraft design |
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116 | (5) |
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10.1.3 Optics and interferometry system |
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121 | (4) |
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125 | (4) |
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10.1.5 Micronewton thrusters |
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129 | (2) |
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131 | (1) |
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10.2 Expected gravitational-wave results from LISA |
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132 | (16) |
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10.2.1 LISA sensitivity and galactic sources |
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132 | (4) |
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10.2.2 Origin of massive black holes |
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136 | (2) |
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10.2.3 Massive black holes in normal galaxies |
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138 | (3) |
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10.2.4 Structure formation and massive black hole coalescence |
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141 | (2) |
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10.2.5 Fundamental physics tests with LISA |
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143 | (3) |
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146 | (2) |
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148 | (1) |
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148 | (4) |
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11 Detection of scalar gravitational waves |
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152 | (27) |
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152 | (2) |
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11.2 Testing theories of gravity |
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154 | (5) |
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11.2.1 Free vibrations of an elastic sphere |
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154 | (1) |
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11.2.2 Interaction of a metric GW with the sphere vibrational modes |
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155 | (2) |
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11.2.3 Measurements of the sphere vibrations and wave polarization states |
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157 | (2) |
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11.3 Gravitational wave radiation in the JBD theory |
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159 | (9) |
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11.3.1 Scalar and Tensor GWs in the JBD Theory |
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160 | (1) |
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11.3.2 Power emitted in GWs |
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161 | (1) |
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11.3.3 Power emitted in scalar GWs |
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162 | (2) |
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164 | (1) |
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11.3.5 Detectability of the scalar GWs |
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165 | (3) |
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168 | (2) |
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11.5 Scalar--tensor cross sections |
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170 | (6) |
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176 | (1) |
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176 | (3) |
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PART 3 The Stochastic Gravitational-Wave Background |
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179 | (64) |
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12 Generalities on the stochastic GW background |
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181 | (30) |
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181 | (3) |
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184 | (7) |
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12.2.1 Ωgw(ƒ) and the optimal SNR |
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184 | (3) |
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12.2.2 The characteristic amplitude |
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187 | (2) |
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12.2.3 The characteristic noise level |
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189 | (2) |
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12.3 The overlap reduction function |
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191 | (6) |
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12.3.1 Two interferometers |
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193 | (3) |
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12.3.2 Interferometer---bar |
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196 | (1) |
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12.3.3 Interferometer---sphere |
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196 | (1) |
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12.4 Achievable sensitivities to the SGWB |
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197 | (10) |
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197 | (2) |
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199 | (5) |
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12.4.3 More than two detectors |
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204 | (3) |
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12.5 Observational bounds |
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207 | (4) |
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211 | (32) |
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211 | (12) |
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214 | (7) |
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221 | (2) |
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223 | (6) |
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224 | (1) |
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13.2.2 Calculation of the spectrum |
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225 | (4) |
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229 | (6) |
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230 | (4) |
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13.3.2 Observational bounds to the spectrum |
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234 | (1) |
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13.4 First-order phase transitions |
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235 | (2) |
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13.5 Astrophysical sources |
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237 | (2) |
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239 | (4) |
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PART 4 Theoretical developments |
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243 | (116) |
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14 Infinite-dimensional symmetries in gravity |
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245 | (23) |
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245 | (7) |
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245 | (1) |
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14.1.2 Mathematical conventions |
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245 | (2) |
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14.1.3 The Einstein--Hilbert action |
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247 | (1) |
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14.1.4 Dimensional reduction D = 4 → D = 3 |
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247 | (1) |
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14.1.5 Dimensional reduction D = 3 → D = 2 |
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248 | (4) |
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252 | (5) |
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14.2.1 Ehlers Lagrangian as a nonlinear σ-model |
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254 | (1) |
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14.2.2 The Ernst equation |
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255 | (1) |
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14.2.3 The Matzner--Misner Lagrangian as a nonlinear a-model |
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255 | (2) |
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14.3 Symmetries of nonlinear σ-models |
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257 | (2) |
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14.3.1 Nonlinear realization of SL(2, R)E |
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257 | (1) |
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14.3.2 Nonlinear realization of SL(2, ***R)MM |
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258 | (1) |
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259 | (2) |
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14.4.1 Action of SL(2, R)E on λ, B2 |
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259 | (1) |
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14.4.2 Action of SL(2, R)MM on λ, B |
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260 | (1) |
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14.4.3 The affine Kac--Moody SL(2, R) algebra |
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260 | (1) |
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261 | (6) |
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14.5.1 Solving Einstein's equations |
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261 | (2) |
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263 | (2) |
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14.5.3 Derivation of the colliding plane metric by factorization |
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265 | (2) |
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267 | (1) |
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267 | (1) |
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15 Gyroscopes and gravitational waves |
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268 | (12) |
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268 | (1) |
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15.2 Splitting formalism and test particle motion: a short review |
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269 | (3) |
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15.3 The spacetime metric |
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272 | (2) |
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15.4 Searching for an operational frame |
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274 | (2) |
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15.5 Precession of a gyroscope in geodesic motion |
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276 | (2) |
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278 | (1) |
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278 | (2) |
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16 Elementary introduction to pre-big bang cosmology and to the relic graviton background |
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280 | (58) |
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280 | (3) |
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16.2 Motivations: duality symmetry |
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283 | (6) |
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16.3 Kinematics: shrinking horizons |
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289 | (5) |
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16.4 Open problems and phenomenological consequences |
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294 | (3) |
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16.5 Cosmological perturbation theory |
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297 | (12) |
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16.5.1 Choice of the frame |
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297 | (2) |
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16.5.2 Choice of the gauge |
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299 | (3) |
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16.5.3 Normalization of the amplitude |
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302 | (2) |
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16.5.4 Computation of the spectrum |
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304 | (5) |
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16.6 The relic graviton background |
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309 | (7) |
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316 | (1) |
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316 | (1) |
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Appendix A The string effective action |
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317 | (5) |
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Appendix B Duality symmetry |
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322 | (6) |
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Appendix C The string cosmology equations |
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328 | (5) |
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333 | (5) |
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17 Post-Newtonian computation of binary inspiral waveforms |
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338 | (21) |
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338 | (2) |
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17.2 Summary of optimal signal filtering |
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340 | (3) |
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17.3 Newtonian binary polarization waveforms |
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343 | (3) |
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17.4 Newtonian orbital phase evolution |
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346 | (3) |
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17.5 Post-Newtonian wave generation |
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349 | (5) |
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349 | (1) |
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350 | (2) |
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352 | (2) |
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17.6 Inspiral binary waveform |
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354 | (2) |
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356 | (3) |
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PART 5 Numerical relativity |
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359 | (50) |
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361 | (48) |
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361 | (2) |
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18.2 Einstein equations for relativity |
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363 | (6) |
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18.2.1 Constraint equations |
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365 | (2) |
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18.2.2 Evolution equations |
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367 | (2) |
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18.3 Still newer formulations: towards a stable evolution system |
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369 | (13) |
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18.3.1 General relativistic hydrodynamics |
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376 | (2) |
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18.3.2 Boundary conditions |
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378 | (1) |
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18.3.3 Special difficulties with black holes |
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379 | (3) |
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18.4 Tools for analysing the numerical spacetimes |
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382 | (6) |
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382 | (1) |
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18.4.2 Locating the apparent horizons |
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383 | (2) |
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18.4.3 Locating the event horizons |
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385 | (1) |
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386 | (2) |
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18.5 Computational science, numerical relativity, and the `Cactus' code |
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388 | (1) |
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18.5.1 The computational challenges of numerical relativity |
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388 | (1) |
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18.6 Cactus computational toolkit |
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389 | (3) |
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18.6.1 Adaptive mesh refinement |
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391 | (1) |
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18.7 Recent applications and progress |
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392 | (7) |
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18.7.1 Evolving pure gravitational waves |
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392 | (2) |
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394 | (5) |
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399 | (1) |
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400 | (1) |
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400 | (3) |
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18.9.1 Overviews/formalisms of numerical relativity |
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400 | (1) |
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18.9.2 Numerical techniques |
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401 | (1) |
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401 | (1) |
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18.9.4 Black hole initial data |
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401 | (1) |
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18.9.5 Black hole evolution |
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401 | (1) |
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18.9.6 Black hole excision |
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402 | (1) |
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18.9.7 Perturbation theory and waveform extraction |
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402 | (1) |
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18.9.8 Event and apparent horizons |
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402 | (1) |
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18.9.9 Pure gravitational waves |
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403 | (1) |
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403 | (1) |
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403 | (6) |
Index |
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