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quantum optics pdf

(Further reading) 76 0 obj 32 0 obj (Heisenberg-Langevin equations) 81 0 obj (Jaynes Cummings model) endobj (Single mode quantum model) 173 0 obj 248 0 obj << /S /GoTo /D (section.1.2) >> sources of coherent electromagnetic radiation. 164 0 obj << /S /GoTo /D (section.8.3) >> endobj /Resources 2 0 R endobj endobj endobj 180 0 obj << /S /GoTo /D (section.4.2) >> endobj (Quantisation of electromagnetism) endobj endobj endobj endobj /Length 522 (Dynamic superradiance) 100 0 obj 224 0 obj << /S /GoTo /D (section.9.2) >> 165 0 obj 260 0 obj (Spontaneous emission, noise, and \040parameter) (Further Reading) << /S /GoTo /D (chapter.3) >> (Fluctuation dissipation theorem) (Further reading) >> endobj endobj 168 0 obj endobj (Dephasing in addition to relaxation) 21 0 obj 92 0 obj 89 0 obj 156 0 obj << /S /GoTo /D (section*.77) >> 217 0 obj (Lasers and micromasers) endobj /Filter /FlateDecode (Density matrix equation) (Contents) 96 0 obj << /S /GoTo /D (section.11.2) >> (The Dicke model) endobj endobj 84 0 obj 208 0 obj endobj 108 0 obj << /S /GoTo /D (section.5.3) >> (Bibliography) (Further reading) endobj 148 0 obj endobj endobj 68 0 obj << /S /GoTo /D (section.1.5) >> << /S /GoTo /D (section.2.5) >> >> 233 0 obj endobj (Quantum jump formalism) endobj Fundamentals of Quantum Optics Marco Ornigotti Lukas Maczewsky Alexander Szameit Summer Semester 2016 Friedrich-Schiller Universität - Jena June 19, 2016 97 0 obj >> 56 0 obj << /S /GoTo /D (chapter.7) >> endobj 80 0 obj 93 0 obj << /S /GoTo /D (section.7.1) >> << /S /GoTo /D (section.4.4) >> endobj 25 0 obj 117 0 obj endobj 184 0 obj endobj 200 0 obj << /S /GoTo /D (section.8.1) >> 161 0 obj (Further reading) (Further reading) (No-go theorem: no vacuum instability) 205 0 obj endobj 141 0 obj endobj endobj endobj endobj (Resonance Fluorescence) 136 0 obj endobj 85 0 obj endobj (More on lasers) 153 0 obj (Power broadening of absorption) (Semiclassical introduction) endobj 144 0 obj endobj endobj �6�o�sC�6 ���E����f�%�]�'��gf��{^L�o��jr�Yl�6��!s53�Z8�9Q�v{o�͔�5^�8��ڛ�9�����^��� �faendstream 269 0 obj << << /S /GoTo /D (section.10.2) >> 265 0 obj << /S /GoTo /D (section.6.1) >> endobj << /S /GoTo /D (section.2.4) >> 172 0 obj endobj 216 0 obj << /S /GoTo /D (chapter*.2) >> Quantum Optics and The Renaissance of Atomic Physics Quantum Optics is an area of atomic, molecular and optical (AMO) physics, which is not easy to define very precisely. 149 0 obj (Laser Linewidth) endobj (Quantum stochastic methods) >> endobj endobj 152 0 obj 188 0 obj 37 0 obj endobj << /S /GoTo /D (section.3.3) >> 52 0 obj endobj (Electric dipole gauge for semiclassical problems) 41 0 obj 113 0 obj %���� endobj 133 0 obj endobj (Further properties of collapse and revival) (Canonical quantisation; photon modes) endobj (Semiclassical limit) 193 0 obj endobj endobj << /S /GoTo /D (section.5.1) >> endobj << /S /GoTo /D (section.9.3) >> 14 0 obj << /Type /Page endobj << /S /GoTo /D (chapter.8) >> endobj 45 0 obj 221 0 obj endobj %PDF-1.4 101 0 obj << /S /GoTo /D (section.4.1) >> 157 0 obj endobj << /S /GoTo /D (section.5.4) >> 145 0 obj endobj << /S /GoTo /D (section.4.3) >> (Eliminating redundant variables) 196 0 obj << /S /GoTo /D (section.12.4) >> stream 261 0 obj endobj endobj endobj endobj /ProcSet [ /PDF /Text ] << /S /GoTo /D (section.11.1) >> (Further reading) << /S /GoTo /D (section*.1) >> endobj (Density matrix equations for a micromaser and a laser) (Three levels, and coherent control) endobj endobj 232 0 obj << /S /GoTo /D (section.6.2) >> 105 0 obj endobj << /S /GoTo /D (section.11.3) >> 40 0 obj endobj endobj endobj 229 0 obj 88 0 obj endobj 116 0 obj endobj (Simple density matrix equation for collective emission) 17 0 obj (Superradiance) endobj /Parent 11 0 R 109 0 obj 128 0 obj (Further reading) 249 0 obj 16 0 obj endobj endobj Its main characteristics, however, is that it deals with lasers, i.e. /Length 849 112 0 obj (Weak to strong coupling via density matrices ) endobj 237 0 obj 236 0 obj endobj << /S /GoTo /D (section.3.2) >> endobj endobj 204 0 obj endobj endobj endobj endobj << /S /GoTo /D (section.7.3) >> x��TMo�0��W��H�x�5�$(�@P5���eS�M�fK���Φ]��Q#{���=��*������vSH��r'�#�@�ől�� ����s؟p��1DYY�7�F�ۺx��y��@���k�$ << /S /GoTo /D (section.12.3) >> 65 0 obj 169 0 obj endobj 177 0 obj 36 0 obj << /S /GoTo /D (section.9.4) >> 33 0 obj << /S /GoTo /D (chapter.5) >> << /S /GoTo /D (chapter.10) >> (Coherent evolution alone; why does EIT occur) 24 0 obj /Filter /FlateDecode r2��޴�� �Mև��.�c�� 3`�X> �ې��mh���d��4�Ο6L,�FSU+�%�2�H. 12 0 obj endobj << /S /GoTo /D (section.5.2) >> 57 0 obj << /S /GoTo /D (chapter.2) >> 9 0 obj << /S /GoTo /D [266 0 R /Fit ] >> 120 0 obj (Dark state polaritons) endobj (Single atom lasers) << /S /GoTo /D (section.2.1) >> (Laser rate equations) (Introduction) x�M�=o�0��_q#�l�ѱR*5mUUb�:X $���u�o���|��9�w_'��@�V�#0&QHUY�������Ԇ��fR�!4_YΕN},mF��� ��}�{�� (Resonance fluorescence spectrum) 125 0 obj 28 0 obj endobj 256 0 obj 185 0 obj The title quantum optics covers a large range of possible courses, and so this introduction intends to explain what this course does and does not aim to provide. (Spectrum of emission into a reservoir) endobj 209 0 obj endobj << /S /GoTo /D (section.2.2) >> endobj 72 0 obj 160 0 obj << /S /GoTo /D (section.6.4) >> endobj endobj endobj 64 0 obj << /S /GoTo /D (section.7.4) >> /MediaBox [0 0 595.2757 841.8898] endobj endobj << /S /GoTo /D (section.12.1) >> << /S /GoTo /D (chapter.11) >> 245 0 obj endobj 61 0 obj 176 0 obj 129 0 obj (Pitfalls of perturbation) 140 0 obj /Font << /F68 7 0 R /F71 10 0 R >> 201 0 obj endobj (Beyond the simple model) (Transformation to the electric dipole gauge) 189 0 obj endobj endobj 228 0 obj endobj endobj << /S /GoTo /D (chapter.9) >> 181 0 obj endobj 220 0 obj endobj (Radiation in a box; restoring the phase transition) endobj << /S /GoTo /D (section.3.1) >> (Density matrix equation for relaxation of two-level system) 3 0 obj << endobj endobj (Many mode quantum model --- irreversible decay) (Further reading) 13 0 obj xڭVMs�0��+|�gbE�寞J3Iڴ�ЁL�c���E���j%Y12�L����v��[����G. endobj endobj endobj << /S /GoTo /D (section.10.4) >> << /S /GoTo /D (chapter.1) >> << /S /GoTo /D (section.12.2) >> endobj endobj 241 0 obj (Examples of Cavity QED systems) 69 0 obj endobj 20 0 obj 257 0 obj endobj << /S /GoTo /D (section.6.3) >> (Density matrices for 2 level systems) Regarding the negatives, there are several things this course deliberately avoids: It is not a course on quantum information theory. /Contents 4 0 R 60 0 obj endobj 197 0 obj << /S /GoTo /D (chapter.12) >> 137 0 obj (Revision: Lagrangian for electromagnetism) endobj << /S /GoTo /D (section.1.3) >> 48 0 obj endobj << /S /GoTo /D (section.8.2) >> endobj if�t� endobj %PDF-1.4 endobj 225 0 obj << /S /GoTo /D (section.7.2) >> << /S /GoTo /D (section.9.1) >> endobj /Length 242 This course will provide a wide-ranging introduction to the field of quantum optics, developing in detail the semiclassical and quantum approaches to light-matter interactions. << /S /GoTo /D (section.1.4) >> 104 0 obj 124 0 obj (Quantum electrodynamics in other gauges) (The Purcell effect in a 1D model cavity) endobj endobj 4 0 obj << << /S /GoTo /D (section.9.5) >> endobj endobj endobj << /S /GoTo /D (section.11.4) >> << /S /GoTo /D (chapter.4) >> endobj 29 0 obj (Phase transitions, spontaneous superradiance) endobj 49 0 obj endobj 253 0 obj 2 0 obj << stream endobj stream 212 0 obj 8 0 obj endobj /Filter /FlateDecode 192 0 obj 77 0 obj 244 0 obj 121 0 obj >> endobj (Quantum regression ``theorem'') (Freedom of choice of gauge and classical equations) endobj (Further reading) 264 0 obj endobj endobj endobj << /S /GoTo /D (chapter.6) >>

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