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1 | (4) |
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5 | (28) |
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2.1 The Optical Classification of Supernovae |
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8 | (5) |
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2.1.1 Spectroscopic Classification |
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8 | (2) |
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2.1.2 Supernova Light Curve Classification |
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10 | (2) |
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2.1.3 The Supernova Rates Per Type |
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12 | (1) |
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2.2 Core-Collapse Supernovae |
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13 | (5) |
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2.2.1 Pre-explosion Composition |
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13 | (1) |
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2.2.2 Neutron Star and Black Hole Formation |
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14 | (1) |
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2.2.3 The Explosion Mechanism |
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15 | (1) |
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2.2.4 Electron-Capture Supernovae of 8--10 M Stars |
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16 | (1) |
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2.2.5 Core-Collapse Supernova Ejecta Composition |
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17 | (1) |
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2.3 Thermonuclear (Type la) Supernovae |
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18 | (8) |
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2.3.1 The Single Degenerate Versus Double Generate Channel |
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19 | (2) |
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2.3.2 Thermonuclear Explosions: Deflagration Versus Detonation |
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21 | (2) |
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2.3.3 The Diversity Among Type la Supernova |
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23 | (3) |
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2.4 Detection of Radio-Active Elements from Supernovae |
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26 | (1) |
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27 | (6) |
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3 Classification and Population |
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33 | (22) |
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3.1 Morphological Classification of Supernova Remnants |
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33 | (3) |
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3.2 The Galactic Supernova Remnant Population |
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36 | (7) |
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3.2.1 Finding and Naming Supernova Remnants |
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37 | (1) |
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3.2.2 Measuring Distances to Supernova Remnants |
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38 | (2) |
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40 | (3) |
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3.3 The Spatial Distribution of Known Galactic Supernova Remnants |
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43 | (3) |
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3.4 The Supernova-Remnant Population in the Magellanic Clouds |
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46 | (4) |
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3.5 Supernova Remnant Populations in Other Galaxies |
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50 | (5) |
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4 Shocks and Post-shock Plasma Processes |
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55 | (32) |
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4.1 The Rankine-Hugoniot Jump Conditions |
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56 | (2) |
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4.2 Magnetohydrodynamical Shocks |
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58 | (4) |
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62 | (13) |
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4.3.1 Visocity and the Shock Transition Layer Thickness |
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62 | (2) |
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4.3.2 The Collisional Mean Free Path |
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64 | (1) |
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4.3.3 The Thermalisation Processes |
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65 | (2) |
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4.3.4 The Expected Post-shock Electron-Ion Temperature Ratio |
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67 | (2) |
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4.3.5 Post-shock Electron-Ion Temperature Equilibration |
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69 | (4) |
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73 | (2) |
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75 | (5) |
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78 | (1) |
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4.4.2 Magnetically Supported, Radiative Shocks |
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79 | (1) |
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4.5 Shock Waves Mediated by Magnetic Precursors |
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80 | (7) |
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5 Supernova Remnant Evolution |
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87 | (30) |
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5.1 Supernova Remnant Evolution: Four Phases |
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87 | (1) |
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5.2 The Expansion Parameter |
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88 | (1) |
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89 | (3) |
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5.3.1 The Reverse Shock Velocity in the Shock- and Observer-Frame |
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90 | (1) |
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5.3.2 The Condition for Forming a Reverse Shock |
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91 | (1) |
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5.3.3 The Turning Around of the Reverse Shock |
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92 | (1) |
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5.4 Self-similar Solutions |
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92 | (4) |
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5.4.1 The Self-similar Sedov-Taylor Solution |
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93 | (1) |
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5.4.2 An Alternative Derivation of the Sedov-Taylor Solution |
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94 | (1) |
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5.4.3 The Sedov-Taylor solution for a stellar-wind profile |
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95 | (1) |
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5.4.4 The Expected Size Distribution of Supernova Remnants |
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95 | (1) |
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5.5 The Internal Structure of Self-similar Explosions |
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96 | (1) |
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5.6 Self-similar Models for the Ejecta-Dominated Phase |
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97 | (6) |
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5.6.1 The Chevalier Self-similar Model for Young Remnants |
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99 | (2) |
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5.6.2 The Transition from Ejecta-Dominated to Adiabatic Phase |
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101 | (2) |
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5.7 The Late Time Evolution of Supernova Remnants |
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103 | (1) |
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5.8 Supernova Remnant Evolution Inside Wind Bubbles |
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104 | (8) |
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5.8.1 The Evolution of Main Sequence Wind Bubbles |
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108 | (2) |
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5.8.2 Supernova Remnant Evolution of Inside Wind Bubbles |
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110 | (2) |
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5.9 Rayleigh-Taylor Instabilities |
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112 | (5) |
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6 Neutron Stars, Pulsars, and Pulsar Wind Nebulae |
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117 | (54) |
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6.1 The Internal Constitution of Neutron Stars |
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118 | (1) |
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119 | (9) |
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6.2.1 The Magnetic Dipole Model for Neutron Stars |
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119 | (4) |
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6.2.2 The Pulsar Braking Index |
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123 | (2) |
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125 | (3) |
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6.3 The Inner Regions of Pulsar Wind Nebulae |
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128 | (11) |
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129 | (2) |
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6.3.2 The Kennel and Coroniti Model |
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131 | (3) |
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6.3.3 Wisps, Jets, and Tori |
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134 | (1) |
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135 | (4) |
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6.4 The Evolution and Radiation of Pulsar Wind Nebulae |
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139 | (17) |
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6.4.1 A Self-similar Solution for the Expansion into the Ejecta |
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140 | (2) |
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6.4.2 The Appearance and Dynamics of the Crab Nebula |
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142 | (1) |
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6.4.3 Pulsar Wind Nebulae Interacting with the Reverse Shock |
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143 | (2) |
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6.4.4 The Radiation from Pulsar Wind Nebulae |
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145 | (3) |
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6.4.5 The Electron/Positron Populations in Pulsar Wind Nebulae |
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148 | (2) |
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6.4.6 The Frequency Dependent Sizes of Pulsar Wind Nebulae |
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150 | (1) |
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6.4.7 The Large Extent of Some Pulsar Wind Nebulae in γ-Rays |
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151 | (3) |
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6.4.8 Pulsars Moving Through Hot Supernova Remnant Shells |
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154 | (2) |
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6.5 Magnetars and Central Compact Objects |
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156 | (13) |
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158 | (8) |
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6.5.2 Compact Central Objects (CCOs) |
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166 | (3) |
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169 | (2) |
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7 Dust Grains and Infrared Emission |
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171 | (28) |
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7.1 Introduction: Interstellar Dust |
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171 | (2) |
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7.2 The Supernova Connection |
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173 | (1) |
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7.3 Dust Heating and Radiation |
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174 | (9) |
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174 | (2) |
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7.3.2 Collisional Dust Heating |
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176 | (4) |
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7.3.3 Stochastic Dust Heating |
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180 | (2) |
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7.3.4 Determining Dust Masses |
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182 | (1) |
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7.4 Dust Formation in Supernova Ejecta |
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183 | (4) |
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7.5 Dust Destruction in Supernova Remnants |
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187 | (3) |
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7.6 Infrared Observations of Supernova Remnants |
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190 | (9) |
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7.6.1 Infrared Emission from Young Supernova Remnants |
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191 | (5) |
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7.6.2 Observational Evidence for Dust Destruction |
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196 | (3) |
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8 Optical Emission from Supernova Remnants |
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199 | (22) |
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8.1 Line Emission from Radiative Shocks Regions |
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200 | (7) |
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8.1.1 On the Prominence of Forbidden Line Emission |
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201 | (5) |
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8.1.2 Optical Emission from Young Supernova Remnants: Optical Emission from High-Density Clumps |
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206 | (1) |
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8.2 Balmer-Dominated Shocks |
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207 | (14) |
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8.2.1 The Formation of the Narrow- and Broad-Line Components |
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209 | (3) |
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8.2.2 The Broad- to Narrow-Line Ratio as a Diagnostic Tool |
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212 | (3) |
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8.2.3 Measuring Distances to Balmer-Dominated Shocks |
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215 | (1) |
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8.2.4 The Shock Structure in the Presence of Neutrals |
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215 | (1) |
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8.2.5 Complications: Pickup Ions and Non-thermal Distributions |
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215 | (2) |
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8.2.6 The Effects of Cosmic-Ray Acceleration |
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217 | (4) |
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9 Young Supernova Remnants: Probing the Ejecta and the Circumstellar Medium |
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221 | (36) |
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9.1 Core-Collapse Versus Type Ia Supernova Remnants |
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221 | (3) |
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9.2 Type la Supernova Remnants |
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224 | (14) |
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9.2.1 Hydrodynamical Plus Radiation Modelling |
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227 | (1) |
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9.2.2 X-ray Cr and Mn Line Diagnostics |
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228 | (2) |
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9.2.3 The Ambient Medium of Type Ia Supernova Remnants |
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230 | (6) |
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9.2.4 The Case of the Missing Donor Stars |
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236 | (1) |
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9.2.5 The Confusing Evidence Concerning Type Ia Progenitors |
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237 | (1) |
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9.3 Core-Collapse Supernova Remnants |
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238 | (19) |
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9.3.1 Cas A and Other Oxygen-Rich Supernova Remnants |
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239 | (4) |
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9.3.2 Asymmetric Ejecta: Donuts, Jets, Rings and Bubbles |
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243 | (6) |
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9.3.3 SN 1987A: the making of a supernova remnant |
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249 | (8) |
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10 Middle-Aged and Old Supernova Remnants |
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257 | (20) |
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10.1 The Presence of Metal-Rich Ejecta in Middle-Aged Supernova Remnants |
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260 | (2) |
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10.2 Interaction with Molecular Clouds |
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262 | (6) |
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10.2.1 Radiation from Molecules |
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263 | (1) |
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10.2.2 The Interaction of Shocks with Molecular Clouds |
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264 | (3) |
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10.2.3 Maser Emission from Supernova Remnants |
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267 | (1) |
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10.3 Mixed-Morphology Supernova Remnants |
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268 | (9) |
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11 Cosmic-Ray Acceleration by Supernova Remnants: Introduction and Theory |
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277 | (46) |
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11.1 Introduction: Galactic Cosmic Rays |
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277 | (17) |
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11.1.1 The Cosmic-Ray Spectrum |
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278 | (2) |
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11.1.2 Cosmic-Ray Composition |
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280 | (4) |
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11.1.3 Cosmic-Ray Transport in the Galaxy |
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284 | (5) |
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11.1.4 SNRs as the dominant sources for Galactic cosmic rays |
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289 | (1) |
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11.1.5 Other Potential Sources of Galactic Cosmic Rays |
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290 | (4) |
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11.2 The Theory of Diffusive Shock Acceleration |
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294 | (14) |
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11.2.1 Diffusive-Shock Acceleration |
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294 | (3) |
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11.2.2 The Convection-Diffusion Equation |
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297 | (3) |
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11.2.3 The Acceleration Time Scale |
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300 | (2) |
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11.2.4 The Maximum Size of the Cosmic-Ray Shock Precursor |
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302 | (1) |
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11.2.5 The Effect of Adiabatic Losses on the Maximum Energy |
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303 | (1) |
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11.2.6 Particle Acceleration by Evolving Shocks |
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303 | (2) |
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11.2.7 The Escape of Cosmic Rays |
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305 | (1) |
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11.2.8 Radiative Losses: The Maximum Electron Energy |
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305 | (3) |
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11.3 Non-linear Shock Acceleration |
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308 | (5) |
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11.4 Particle Acceleration and Magnetic Fields |
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313 | (10) |
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11.4.1 Resonant Particle-Wave Interaction |
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314 | (3) |
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11.4.2 Streaming Instabilities and Non-resonant Processes |
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317 | (1) |
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11.4.3 The non-resonant Bell instability |
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318 | (5) |
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12 Supernova Remnants and Cosmic Rays: Non-thermal Radiation |
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323 | (56) |
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323 | (15) |
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12.1.1 The Radio Spectral Index Distribution |
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324 | (3) |
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12.1.2 The Minimum Energy Requirement and the Van der Laan Mechanism |
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327 | (3) |
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12.1.3 The Radio Evolution of Supernova Remnants |
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330 | (5) |
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12.1.4 Radio Polarisation Measurements |
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335 | (3) |
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12.2 X-ray Synchrotron Radiation |
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338 | (18) |
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12.2.1 The Implication of X-ray Synchrotron Radiation |
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340 | (1) |
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12.2.2 The Narrow Widths of the X-ray Synchrotron Regions |
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341 | (4) |
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12.2.3 The Case for Magnetic-Field Amplification |
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345 | (4) |
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12.2.4 Magnetic-Field Amplification Near the Reverse Shock |
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349 | (1) |
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12.2.5 X-ray Synchrotron Flickering and Flux Decline |
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350 | (3) |
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12.2.6 X-ray Synchrotron Peculiarities and (Possible) Consequences |
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353 | (3) |
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12.3 Gamma-Rays Observations: A Window on the Hadronic Cosmic-Ray Content of Supernova Remnants |
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356 | (23) |
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12.3.1 A Brief Historical Overview of γ-Ray Astronomy |
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357 | (2) |
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12.3.2 Hadronic Versus Leptonic Emission |
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359 | (5) |
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12.3.3 A Few Words on Modelling Inverse Compton Scattering |
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364 | (3) |
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12.3.4 Gamma-Ray Evidence for Escaping Cosmic Rays |
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367 | (3) |
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12.3.5 The Population of γ-Ray Emitting Supernova Remnants |
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370 | (4) |
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12.3.6 Where Are the PeVatrons? |
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374 | (5) |
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379 | (80) |
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379 | (1) |
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13.2 Radiation from Moving Charged Particles |
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380 | (9) |
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13.2.1 Thomson Scattering |
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380 | (3) |
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13.2.2 Inverse Compton Scattering |
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383 | (6) |
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13.3 Synchrotron Radiation |
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389 | (10) |
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13.3.1 The Synchrotron Power and Spectrum |
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390 | (4) |
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13.3.2 Radiation from a Power-Law Electron Distribution |
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394 | (1) |
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13.3.3 The Effects of Synchrotron Radiation Energy Losses |
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395 | (2) |
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397 | (2) |
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13.4 Bremsstrahlung (Free-Free Emission) |
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399 | (12) |
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13.4.1 Bremsstrahlung from a Single Electron-Ion Encounter |
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401 | (2) |
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13.4.2 The Collisional Cross-Section and Total Radiation Spectrum |
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403 | (2) |
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13.4.3 Relativistic Bremsstrahlung |
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405 | (1) |
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13.4.4 Thermal Bremsstrahlung |
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406 | (2) |
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13.4.5 Non-thermal Bremsstrahlung |
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408 | (2) |
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13.4.6 Free-Free Absorption |
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410 | (1) |
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13.5 Line Emission, Ionisation and Recombination Processes |
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411 | (38) |
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13.5.1 The Einstein Coefficients and Oscillator Strength |
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413 | (2) |
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13.5.2 Some Basic Atomic Physics |
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415 | (6) |
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13.5.3 The Atomic Shell Model and Electron Configurations |
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421 | (5) |
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13.5.4 Electron Transition Probabilities and the Einstein Coefficients |
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426 | (4) |
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13.5.5 Collisional Processes that Shape Emission Line Spectra |
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430 | (7) |
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13.5.6 Radiative Recombination Continuum (Free-Bound Emission) |
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437 | (2) |
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13.5.7 Non-equilibrium Ionisation |
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439 | (3) |
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13.5.8 X-ray Line Emission Diagnostics |
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442 | (5) |
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13.5.9 Resonant Absorption and Line Scattering |
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447 | (2) |
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13.6 Pion Production and Decay |
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449 | (10) |
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13.6.1 Meson Production in Supernova Remnants |
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451 | (1) |
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13.6.2 The Energy Threshold for Pion Production |
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452 | (1) |
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13.6.3 The Formation of the γ-Ray Spectrum |
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453 | (6) |
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459 | (16) |
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14.1 Knowledge Gained and Outstanding Questions |
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459 | (3) |
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14.2 Future Observing Facilities |
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462 | (8) |
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14.3 The Emergence of Multimessenger Astronomy |
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470 | (1) |
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14.4 The Extragalactic Transients Connection |
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471 | (4) |
Bibliography |
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475 | (38) |
Index |
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513 | (6) |
Astrophysical objects |
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519 | |