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Vibrational and Electronic Excitation of Molecules by Short-Pulse Strong Laser Fields |
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1 | (22) |
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1 | (1) |
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2 | (7) |
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Vibrational Excitation Through Ionization |
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3 | (2) |
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Vibrational Excitation Through R-Dependent Depletion |
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5 | (2) |
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Vibrational Excitation Through Bond-Softening |
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7 | (2) |
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9 | (8) |
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Ionization of Charge-Asymmetric Dissociation Curves |
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9 | (1) |
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Resonant High-Order Multiphoton Excitation |
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9 | (6) |
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15 | (1) |
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Excitation Through Recollision |
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16 | (1) |
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17 | (3) |
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Strong Field Interactions |
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17 | (1) |
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17 | (1) |
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18 | (1) |
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19 | (1) |
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20 | (1) |
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21 | (2) |
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Coherent Lattice Oscillations in Solids and Their Optical Control Part I. Fundamentals and Optical Detection Techniques |
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23 | (24) |
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23 | (2) |
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Generation of Coherent Phonons |
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25 | (4) |
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Impulsive Stimulated Raman Scattering |
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25 | (2) |
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Photocarrier-Mediated Excitation of Coherent Phonons |
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27 | (2) |
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Optical Detection of Coherent Phonons |
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29 | (1) |
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Electron-Phonon Coupling in Group V Semimetals |
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30 | (3) |
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Coherent Phonons in Group IV Crystals and Graphitic Materials |
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33 | (5) |
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Coherent Phonons in Tetrahedrally Bonded Crystals |
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33 | (2) |
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Ultrafast Electron-Phonon Decoupling in Graphite |
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35 | (2) |
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Exciton-Phonon and Phonon-Phonon Couplings in Carbon Nanotubes |
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37 | (1) |
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Coherent Optical Phonons in Metals |
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38 | (3) |
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Coherent Phonons in Other Materials |
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41 | (1) |
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42 | (1) |
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43 | (4) |
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Coherent Lattice Oscillations in Solids and Their Optical Control Part II. New Detection Techniques and Optical Control |
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47 | (18) |
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Coherent Phonons Detected by Novel Techniques |
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47 | (8) |
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Time Resolved X-Ray Diffraction |
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47 | (3) |
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X-Ray Abrotption Spectroscopy |
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50 | (1) |
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Time-Resolved THz Spectroscopy |
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50 | (2) |
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Time-Resolved Photo-Spectroscopy |
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52 | (3) |
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Optical Control of Coherent Phonons |
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55 | (5) |
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Optical Control at Low Excitation Density |
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55 | (3) |
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Optical Control Near the Lindemann Limit |
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58 | (2) |
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Optical Control in Strongly Correlated Systems |
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60 | (1) |
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60 | (1) |
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61 | (4) |
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Heterodyne Interferometry Using High-Order Harmonic Generation in Mixed Gases |
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65 | (16) |
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65 | (2) |
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Theory of HHG in Mixed Gases and Heterodyne Interferometry for Detection of Ultrafast Molecular Dynamics |
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67 | (2) |
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Destructive Interference During HHG in Mixed Gases |
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69 | (1) |
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69 | (3) |
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Application of the Heterodyne Interferometry to Attosecond Physics |
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72 | (7) |
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73 | (2) |
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Physical Origin of the Interference Signal |
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75 | (4) |
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79 | (1) |
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79 | (2) |
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Propagation of Ultrashort Pulses in Condensed Media |
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81 | (28) |
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81 | (3) |
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Propagation Effects: Filamentation |
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84 | (10) |
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Visualization of Filamentation |
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85 | (1) |
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Control Over the Onset of Filamentation |
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86 | (3) |
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Focusing-Refocusing Events |
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89 | (2) |
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Other Control Issues: Multi-Filamentation |
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91 | (3) |
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Propagation Effects: Supercontinuum Generation |
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94 | (7) |
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94 | (1) |
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95 | (2) |
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Pulse Duration Dependence |
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97 | (1) |
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97 | (2) |
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99 | (1) |
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Incident Power Dependence |
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99 | (2) |
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Applications of White Light Generation and Filamentation |
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101 | (3) |
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Supercontinuum Generation in Bio-Media |
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102 | (1) |
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103 | (1) |
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104 | (5) |
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On Lightning Control Using Lasers |
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109 | (14) |
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109 | (1) |
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110 | (1) |
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Attempts to Trigger Lightning Using High-Energy Lasers |
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111 | (1) |
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Control of High-Voltage Discharges Using Ultrashort Lasers |
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112 | (2) |
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Field Experiments Using Femtosecond Laser Filamentation |
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114 | (1) |
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Optimization of the Filament Effect in Thunderstorms |
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115 | (4) |
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Optimization of the Plasma Density and Lifetime |
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115 | (1) |
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Mechanism of the Laser Filament Action in Thunderclouds |
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115 | (2) |
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Influence of the Geometric Configuration |
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117 | (2) |
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119 | (1) |
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120 | (3) |
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Advances in X-Ray Studies of Ultraintense Laser-Plasma Interactions |
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123 | (16) |
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123 | (2) |
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Basic Spectroscopy Techniques |
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125 | (2) |
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The Single Photon Detection Technique |
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127 | (2) |
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129 | (7) |
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X-Ray Imaging of Interactions With Ti Foil Targets |
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130 | (1) |
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Fast Electron Transport in Multilayer Targets |
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131 | (5) |
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136 | (1) |
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137 | (2) |
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High Field Photonics in Laser Plasmas: Propagation Studies, Electron Acceleration, and Nuclear Activation With Ultrashort Intense Laser Pulses |
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139 | (26) |
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139 | (2) |
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Studies on Laser Pulse Propagation |
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141 | (8) |
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Propagation in Overdense Plasmas |
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141 | (2) |
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Propagation in Underdense Plasmas and Pre-pulse Action |
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143 | (3) |
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Preformed Pulse-Guiding Channels in Plasmas |
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146 | (3) |
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Electron Acceleration: Experiments and Simulations |
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149 | (6) |
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Laser Wakefield Acceleration and Associated Regimes |
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149 | (2) |
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Advanced Techniques and Record Results |
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151 | (2) |
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An Efficient Source of Relativistic Electrons for Medical Applications |
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153 | (2) |
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Nuclear Activation Using Electron Bunches from Laser Plasmas |
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155 | (6) |
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Basics of Nuclear Photo-Activation |
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156 | (1) |
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Activation Induced by Laser-Plasma Electrons |
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157 | (2) |
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An Example of High-Efficiency Photonuclear Activation in a Gas-Jet Experiment |
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159 | (1) |
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Perspectives of Possible Applications |
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160 | (1) |
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161 | (4) |
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161 | |
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Laser Plasma Acceleration and Related Electromagnetic Sources |
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165 | (22) |
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165 | (4) |
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Relativistic Electrons Sources |
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169 | (4) |
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173 | (3) |
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Laser Plasma Based e. m. Sources |
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176 | (4) |
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180 | (1) |
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181 | (6) |
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Laser-Driven Ion Generation with Short, Intense, and High Contrast Pulses |
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187 | (22) |
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187 | (1) |
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The TNSA Acceleration Mechanism: The Role of a Plasma Gradient |
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188 | (6) |
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Ultra High Contrast Pulses with a Double Plasma Mirror |
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194 | (3) |
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197 | (5) |
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197 | (4) |
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201 | (1) |
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An Analytical Model for Ion and Proton Emission at UHC |
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202 | (3) |
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205 | (4) |
Index |
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209 | |