Forward |
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xvii | |
Preface |
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xix | |
About the Author |
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xxi | |
Introduction |
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1 | (6) |
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1 | (1) |
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2 | (1) |
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3 | (1) |
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3 | (4) |
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Chapter 1 Our First Encounter with the Quantum World: Light |
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7 | (16) |
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1.1 Some Opening Thoughts |
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7 | (1) |
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1.2 A little Light Reading |
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7 | (2) |
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1.3 Lasers and Video Cameras |
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9 | (1) |
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10 | (1) |
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1.5 An Interference Experiment |
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11 | (9) |
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1.5.1 Interference as a Wave Effect |
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12 | (4) |
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1.5.2 Mach-Zehnder with Photons |
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16 | (2) |
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18 | (2) |
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20 | (3) |
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20 | (3) |
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23 | (12) |
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23 | (1) |
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2.1.1 Electrons and Electron Guns |
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23 | (1) |
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2.2 The Stern-Gerlach Experiment |
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24 | (10) |
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2.2.1 Turning Things Around |
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27 | (1) |
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2.2.2 Things Get More Puzzling |
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28 | (1) |
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2.2.3 So, Where Did It Go? |
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29 | (2) |
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2.2.4 What Does It All Mean? |
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31 | (3) |
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34 | (1) |
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34 | (1) |
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35 | (20) |
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35 | (1) |
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3.2 Describing Classical Systems |
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35 | (3) |
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37 | (1) |
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3.3 Describing Quantum Systems |
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38 | (13) |
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3.3.1 Specific Example: Mach-Zehnder Again |
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40 | (4) |
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3.3.2 Probability Amplitudes |
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44 | (1) |
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3.3.3 Relating Amplitudes to Probabilities |
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44 | (1) |
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3.3.4 Amplitudes, Complex Numbers and Phase |
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45 | (3) |
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3.3.5 States in Stern-Gerlach Experiment |
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48 | (1) |
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3.3.6 General Stern-Gerlach States |
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49 | (1) |
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3.3.7 Some Further Thoughts |
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50 | (1) |
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3.4 What Are Quantum States? |
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51 | (4) |
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52 | (3) |
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55 | (10) |
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55 | (4) |
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58 | (1) |
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59 | (6) |
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60 | (1) |
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61 | (2) |
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4.2.3 Going the Other Way |
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63 | (1) |
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63 | (2) |
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65 | (12) |
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65 | (1) |
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65 | (1) |
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65 | (1) |
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66 | (1) |
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66 | (1) |
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67 | (3) |
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5.4.1 Operators and Physical Quantities |
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69 | (1) |
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5.4.2 Classical and Quantum |
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69 | (1) |
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70 | (7) |
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5.5.1 Why Is State Collapse Necessary? |
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73 | (1) |
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74 | (1) |
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5.5.3 Determinism and Free Will |
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74 | (1) |
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75 | (2) |
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77 | (14) |
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77 | (1) |
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6.2 The Double-Slit Experiment |
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77 | (6) |
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6.2.1 The Double Slit with Electrons |
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79 | (3) |
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6.2.2 Wave/Particle Duality |
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82 | (1) |
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6.2.3 Wave Nature of Electrons |
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82 | (1) |
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6.3 Double-Slit Amplitudes |
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83 | (5) |
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84 | (2) |
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6.3.2 An Experiment with Phase |
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86 | (1) |
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6.3.3 The Interference Term |
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87 | (1) |
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6.3.4 Amplitudes and Electron Strikes |
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87 | (1) |
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88 | (3) |
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89 | (2) |
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91 | (8) |
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91 | (1) |
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7.2 The Amplitude for a Free Particle |
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91 | (7) |
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92 | (2) |
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7.2.2 The Complex Wave of the Amplitude |
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94 | (1) |
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95 | (1) |
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7.2.4 What Does the Amplitude Tell Us about the Motion of a Free Particle? |
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96 | (1) |
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7.2.5 Amplitudes, Energy, and Momentum |
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97 | (1) |
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98 | (1) |
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98 | (1) |
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Chapter 8 Identical Particles |
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99 | (16) |
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8.1 Some Opening Thoughts |
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99 | (1) |
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99 | (5) |
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8.2.1 Scattering Amplitudes |
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101 | (2) |
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8.2.2 The Moral of the Story |
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103 | (1) |
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8.3 States of More Than One Particle |
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104 | (9) |
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8.3.1 Identical Particles |
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106 | (3) |
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8.3.2 States in Real World |
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109 | (2) |
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111 | (1) |
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8.3.4 More Than Two Particles |
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111 | (1) |
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8.3.5 More General States |
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112 | (1) |
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8.3.6 A More Elegant Approach |
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112 | (1) |
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113 | (2) |
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113 | (2) |
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Chapter 9 Scattering Identical Bosons |
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115 | (12) |
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115 | (2) |
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9.2 The Same, but Different: Identical Particles |
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117 | (3) |
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9.2.1 Using the Whole Detector |
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118 | (1) |
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119 | (1) |
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9.3 Transitions Away from States |
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120 | (3) |
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9.3.1 Spontaneous vs Stimulated |
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122 | (1) |
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122 | (1) |
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9.4 Bose-Einstein Condensates |
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123 | (4) |
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9.4.1 Einstein's Argument |
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125 | (1) |
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126 | (1) |
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127 | (16) |
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10.1 Fermions, Bosons, and Stern-Gerlach Magnets |
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127 | (1) |
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127 | (7) |
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10.2.1 Angular Momentum in Quantum Theory |
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129 | (1) |
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10.2.2 Eigenstates of Angular Momentum |
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129 | (2) |
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131 | (1) |
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10.2.4 The Magnetic Moment of an Electron |
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132 | (1) |
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10.2.5 Intrinsic Angular Momentum |
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133 | (1) |
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134 | (6) |
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135 | (4) |
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10.3.2 Fermions and Bosons |
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139 | (1) |
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10.4 Quantum Scale, Spin, Spinors and Twistors |
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140 | (3) |
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140 | (3) |
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Chapter 11 Fermion States |
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143 | (20) |
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11.1 States, Normalization, and Phase |
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143 | (1) |
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11.2 Exchange and Rotation |
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144 | (1) |
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11.3 Rotational Symmetry of States |
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145 | (6) |
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11.3.1 Reversing the Polarity of the Neutron Flow |
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146 | (3) |
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11.3.2 Coffee Mugs and Quantum States |
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149 | (1) |
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11.3.3 Spin, Symmetry, and Exchanges |
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150 | (1) |
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151 | (6) |
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11.4.1 Spinning Things Round |
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153 | (2) |
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11.4.2 Rotation for More Fun and Profit |
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155 | (1) |
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156 | (1) |
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157 | (3) |
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11.5.1 More on Time Reversal |
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158 | (1) |
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11.5.2 Time-Reversed Boson States |
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159 | (1) |
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160 | (3) |
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160 | (3) |
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Chapter 12 Continuous Bases |
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163 | (648) |
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163 | (2) |
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165 | (6) |
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12.2.1 Probability Density |
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165 | (2) |
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12.2.2 Infinite State Expansions |
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167 | (1) |
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12.2.3 The Identity Operator |
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168 | (1) |
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12.2.4 A Short Aside: Projection Operators |
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169 | (2) |
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12.3 State Functions and Wave Functions |
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171 | (1) |
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172 | (639) |
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12.4.1 The Problem of Momentum |
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172 | (1) |
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12.4.2 Momentum in Quantum Theory |
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173 | (3) |
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12.4.3 Operators and Representations |
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176 | (1) |
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12.4.4 Expectation Values Again |
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177 | (1) |
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12.4.5 Operators and Variables |
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178 | (1) |
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179 | (2) |
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181 | (1) |
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13.1 Expectation Is Not Enough |
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181 | (5) |
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13.1.1 Developing Uncertainty |
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183 | (3) |
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13.2 Heisenberg's Principle |
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186 | (2) |
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186 | (1) |
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13.2.2 I'm Not Sure What You Mean by Uncertainty |
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187 | (1) |
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13.3 Yet More Uncertainty |
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188 | (3) |
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13.3.1 The Generalized Uncertainty Principle |
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189 | (1) |
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190 | (1) |
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Chapter 14 The Equations of Quantum Theory |
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191 | (14) |
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14.1 The Schrodinger Equations |
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191 | (3) |
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193 | (1) |
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193 | (1) |
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194 | (3) |
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14.2.1 The Classical Limit |
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196 | (1) |
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14.2.2 Constants of Motion |
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197 | (1) |
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14.3 The Energy-Time Inequality |
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197 | (4) |
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14.3.1 I Really Don't Have the Time |
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200 | (1) |
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14.3.2 Energy/Time Uncertainty |
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201 | (1) |
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201 | (1) |
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202 | (3) |
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203 | (2) |
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Chapter 15 Constrained Particles |
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205 | (1) |
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205 | (11) |
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15.1.1 Another Brick in the Wall |
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206 | (2) |
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208 | (1) |
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15.1.3 Energy within the Box |
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209 | (1) |
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15.1.4 Momentum in the Box |
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210 | (1) |
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15.1.5 Spatial Distribution |
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211 | (1) |
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212 | (4) |
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15.1.7 Two-Dimensional and Three-Dimensional Boxes |
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216 | (1) |
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216 | (8) |
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15.2.1 Quantum Numbers for Hydrogen |
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220 | (1) |
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15.2.2 Visualising Hydrogen State Functions |
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221 | (3) |
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15.3 A Box Containing More Than One Electron |
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224 | (1) |
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15.3.1 Temperature and the Fermi Gas |
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225 | (1) |
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226 | (3) |
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229 | (4) |
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233 | (1) |
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16.1 The Scientific Community |
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233 | (1) |
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16.2 "It Was the Best of Times, It Was the Worst of Times" |
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234 | (3) |
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235 | (2) |
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Chapter 17 Planck and Einstein |
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237 | (10) |
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237 | (1) |
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237 | (1) |
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17.3 Planck Enters Research |
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237 | (3) |
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17.3.1 Planck's Formula for Black Body Spectra |
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239 | (1) |
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240 | (3) |
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17.4.1 Quantization of Light |
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241 | (1) |
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17.4.2 The Photoelectric Effect |
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242 | (1) |
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242 | (1) |
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243 | (1) |
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243 | (4) |
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244 | (3) |
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247 | (12) |
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247 | (1) |
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247 | (1) |
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248 | (7) |
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248 | (1) |
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249 | (3) |
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252 | (3) |
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255 | (2) |
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256 | (1) |
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257 | (2) |
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258 | (1) |
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259 | (8) |
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259 | (1) |
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19.2 The Development of Quantum Theory |
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259 | (5) |
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19.2.1 Cloud Chamber Tracks |
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261 | (1) |
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19.2.2 The Uncertainty Principle |
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261 | (2) |
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263 | (1) |
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264 | (3) |
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265 | (2) |
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Chapter 20 De Broglie & Schrodinger |
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267 | (8) |
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267 | (2) |
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20.1.1 Electron Diffraction |
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268 | (1) |
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20.2 Enter the Wave Equation |
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269 | (3) |
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270 | (1) |
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271 | (1) |
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272 | (1) |
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20.3 Schrodinger's Philosophy |
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272 | (3) |
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273 | (2) |
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275 | (8) |
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21.1 Dirac's Influence on Quantum Physics |
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275 | (2) |
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277 | (1) |
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21.3 Dirac's Views on the Meaning of Quantum Theory |
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278 | (5) |
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281 | (2) |
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283 | (1) |
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284 | (3) |
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Chapter 23 Quantum Correlations |
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287 | (1) |
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287 | (1) |
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23.2 Is Quantum Theory Complete? |
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287 | (8) |
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288 | (3) |
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23.2.2 Follow-Up by David Bohm |
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291 | (2) |
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23.2.3 Bohr's Reply to the EPR Argument |
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293 | (1) |
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294 | (1) |
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23.3 Schrodinger Introduces Entanglement |
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295 | (4) |
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23.3.1 Entanglement and Measurement |
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295 | (2) |
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23.3.2 The Sorry Tail of Schrodinger's Cat |
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297 | (2) |
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23.4 John Bell and Bohm's EPR |
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299 | (9) |
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300 | (1) |
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301 | (1) |
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302 | (1) |
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Experimental Correlations, Se |
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302 | (1) |
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Local Hidden Variable Correlations, S1 |
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303 | (2) |
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Quantum Mechanical Correlations, Sq |
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305 | (1) |
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23.4.4 Aspect's Experiment |
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306 | (2) |
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308 | (3) |
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308 | (3) |
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Chapter 24 Quantum Computing |
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311 | (14) |
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24.1 Historical Perspective |
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311 | (1) |
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24.2 The Fundamentals of Digital Computing |
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311 | (2) |
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24.2.1 A Bit More Information |
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312 | (1) |
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312 | (1) |
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313 | (6) |
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313 | (2) |
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315 | (2) |
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24.3.3 The No-Cloning Theorem |
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317 | (1) |
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24.3.4 What Makes a Quantum Computer Quantum? |
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318 | (1) |
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24.4 Quantum Teleportation |
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319 | (3) |
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24.4.1 Experimental Implementation |
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322 | (1) |
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24.5 Practical Quantum Computers |
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322 | (3) |
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323 | (2) |
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Chapter 25 Density Operators |
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325 | (10) |
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325 | (2) |
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327 | (2) |
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25.3 The Density Operator and EPR/Bohm-Type Experiments |
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329 | (3) |
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25.3.1 Representing a State |
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330 | (1) |
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25.3.2 The Density Operator and Entangled States |
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331 | (1) |
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25.4 The Density Matrix and the Measurement Problem |
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332 | (3) |
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334 | (1) |
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Chapter 26 Interpretations |
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335 | (18) |
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26.1 What is An Interpretation? |
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335 | (1) |
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26.2 A Collection of Problems |
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336 | (7) |
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26.2.1 The Nature of Probability |
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336 | (4) |
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26.2.2 Reduction of the State Vector |
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340 | (2) |
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342 | (1) |
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343 | (1) |
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343 | (9) |
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343 | (1) |
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26.3.2 The Kochen-Specker Theorem |
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344 | (1) |
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26.3.3 Proving the Kochen-Specker Theorem |
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344 | (1) |
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344 | (2) |
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346 | (2) |
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348 | (4) |
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352 | (1) |
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352 | (1) |
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352 | (1) |
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Chapter 27 The Copenhagen Interpretation |
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353 | (20) |
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353 | (1) |
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27.2 Bohr's View of Quantum Theory |
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354 | (7) |
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27.2.1 Classical Concepts Must Be Used to Describe the Results of Any Experiment |
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354 | (1) |
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27.2.2 During a Measurement It Is Impossible to Separate a Quantum Object from the Apparatus |
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355 | (3) |
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27.2.3 The Results of One Experimental Arrangement Cannot Necessarily Be Related to Another |
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358 | (1) |
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27.2.4 Classical Explanations |
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359 | (1) |
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27.2.5 Drawing the Threads Together |
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360 | (1) |
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27.3 Heisenberg and Potentia |
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361 | (2) |
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27.4 Von Neumann and Measurement |
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363 | (2) |
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27.4.1 The Mind of an Observer |
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364 | (1) |
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365 | (2) |
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27.6 Criticisms of the Copenhagen View |
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367 | (6) |
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27.6.1 The Problem of the Cut |
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367 | (3) |
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27.6.2 Problem of Collapse |
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370 | (1) |
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370 | (3) |
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Chapter 28 The Many Worlds Interpretation |
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373 | (20) |
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28.1 Everett, Wheeler, Bohr & DeWitt |
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373 | (1) |
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28.2 The Relative State Formulation 4 |
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374 | (2) |
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376 | (3) |
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378 | (1) |
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28.4 The Ontological Step |
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379 | (1) |
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380 | (1) |
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381 | (7) |
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28.6.1 The Nature of Probability |
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381 | (1) |
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382 | (1) |
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383 | (1) |
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Decision Theory Enters the Argument |
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383 | (4) |
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387 | (1) |
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387 | (1) |
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387 | (1) |
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28.6.5 Bell's Inequality and the K-S Theorem |
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387 | (1) |
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28.7 Criticisms of the Many Worlds View |
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388 | (2) |
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390 | (3) |
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390 | (3) |
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Chapter 29 Assorted Alternatives |
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393 | (8) |
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29.1 Being in Two Minds about Something |
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393 | (3) |
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394 | (1) |
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29.1.2 The Advantages of Having More Than One Mind |
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395 | (1) |
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396 | (5) |
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29.2.1 The Penrose Interpretation |
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396 | (3) |
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399 | (2) |
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Chapter 30 Consistent Histories |
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401 | (24) |
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401 | (4) |
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405 | (2) |
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30.2.1 Moggies and Sample Spaces |
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405 | (1) |
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30.2.2 Meaningless Statements |
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405 | (2) |
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407 | (1) |
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407 | (1) |
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407 | (13) |
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30.3.1 Combining Histories |
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408 | (1) |
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409 | (2) |
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30.3.3 Consistent Histories |
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411 | (1) |
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30.3.4 Histories and Mach-Zehnder |
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412 | (3) |
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415 | (2) |
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30.3.6 Decoherence and the Classical World |
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417 | (2) |
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30.3.7 Histories in Cosmology |
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419 | (1) |
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420 | (5) |
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421 | (1) |
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421 | (1) |
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30.4.3 Probability (Again) |
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422 | (1) |
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422 | (1) |
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423 | (2) |
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Chapter 31 The Ontological Interpretation |
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425 | (18) |
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31.1 Physics and Philosophy |
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425 | (1) |
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426 | (6) |
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31.2.1 Bohm's Version of the Schrodinger Equation |
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426 | (3) |
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31.2.2 The Quantum Potential Energy |
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429 | (3) |
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432 | (1) |
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31.4 Quantum Potential Energy in Action |
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433 | (3) |
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31.4.1 Quantum Potential Energy and the Double Slit Experiment |
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433 | (1) |
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31.4.2 Quantum Potential Energy and the Particle in a Box |
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434 | (1) |
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435 | (1) |
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436 | (1) |
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31.5 Information and Wave Function Collapse |
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436 | (3) |
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439 | (1) |
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31.7 Reactions to Bohm's Theory |
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440 | (3) |
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441 | (2) |
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Chapter 32 Quantum Field Theory |
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443 | (26) |
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32.1 Why Are We Doing This? |
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443 | (1) |
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32.2 Taking Identical Particles Seriously |
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443 | (2) |
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444 | (1) |
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445 | (1) |
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32.3 States in Quantum Field Theory |
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445 | (9) |
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446 | (1) |
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447 | (1) |
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447 | (1) |
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447 | (1) |
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448 | (1) |
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32.3.6 Fermions and Bosons |
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449 | (1) |
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450 | (1) |
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451 | (1) |
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32.3.9 Round and Round We Go |
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452 | (1) |
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32.3.10 Multiparticle Operators Representing Observables |
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453 | (1) |
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454 | (4) |
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32.4.1 So Why Is It Called Quantum Field Theory? |
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455 | (2) |
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32.4.2 Wave-Particle Duality |
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457 | (1) |
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32.5 Interactions in Quantum Field Theory |
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458 | (5) |
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32.5.1 Interaction Operators |
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459 | (2) |
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32.5.2 Interaction Potentials |
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461 | (2) |
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463 | (2) |
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32.6.1 Fields and Numbers |
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464 | (1) |
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465 | (4) |
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32.7.1 Loop Quantum Gravity (LQG) |
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466 | (1) |
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466 | (1) |
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466 | (1) |
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467 | (2) |
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Chapter 33 Personal Conclusions |
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469 | (5) |
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469 | (1) |
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469 | (4) |
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470 | (1) |
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33.2.2 Copenhagenism & Consistent Histories |
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471 | (1) |
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33.2.3 Many Worlds and Many Minds |
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472 | (1) |
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33.2.4 The Ontological Interpretation |
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473 | (1) |
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33.2.5 Objective Collapse |
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473 | (1) |
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473 | (1) |
Notes |
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474 | (1) |
Appendix List of Important Rules |
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475 | (2) |
Index |
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477 | |