Foreword to second edition |
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xiii | |
Foreword |
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xv | |
Acknowledgments |
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xvii | |
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1 | (10) |
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11 | (58) |
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11 | (1) |
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II.2 Dipole autocorrelation function |
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12 | (6) |
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12 | (4) |
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II.2.2 The Hamiltonian of the molecular system |
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16 | (2) |
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II.3 Toward "conventional" impact theories |
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18 | (7) |
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II.3.1 General properties of the correlation function |
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19 | (1) |
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II.3.2 The binary collision approximation |
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20 | (2) |
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II.3.3 Initial statistical correlations |
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22 | (1) |
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II.3.4 The impact approximation |
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22 | (3) |
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II.4 Beyond the impact approximation |
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25 | (2) |
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II.5 Effects of the radiator translational motion |
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27 | (4) |
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II.6 Collision-induced spectra |
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31 | (5) |
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36 | (1) |
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Appendix II.A Spectral and time domain profiles in various spectroscopies |
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36 | (11) |
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II.A1 Absorption, emission, and dispersion |
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36 | (2) |
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II.A2 Rayleigh and spontaneous Raman scatterings |
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38 | (3) |
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II.A3 Nonlinear Raman spectroscopies |
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41 | (4) |
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II.A4 Time-resolved Raman spectroscopies |
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45 | (2) |
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Appendix II.B Some criteria for the approximations |
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47 | (7) |
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II.B1 The large number of perturbers |
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47 | (1) |
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II.B2 The local thermodynamic equilibrium |
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48 | (3) |
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II.B3 The binary collisions |
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51 | (2) |
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II.B4 The (full) impact assumption |
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53 | (1) |
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Appendix II.C The impact relaxation matrix |
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54 | (6) |
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II.C1 Analysis through the time dependence |
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54 | (5) |
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II.C2 Analysis through the frequency dependence |
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59 | (1) |
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Appendix II.D The Liouville space |
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60 | (2) |
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Appendix II.E The resolvent approach |
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62 | (7) |
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II.E1 Spectral-shape expression |
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62 | (3) |
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II.E2 Rotational invariance |
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65 | (1) |
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66 | (3) |
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69 | (112) |
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69 | (12) |
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III.2 Doppler broadening and Dicke narrowing |
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81 | (3) |
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III.2.1 The Doppler broadening |
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81 | (1) |
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III.2.2 The Dicke narrowing |
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82 | (2) |
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III.3 Basic models for spectral line shapes |
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84 | (14) |
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III.3.1 The Lorentz profile |
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84 | (2) |
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III.3.2 The Dicke profile |
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86 | (1) |
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III.3.3 The Voigt profile |
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86 | (2) |
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III.3.4 The Galatry profile |
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88 | (1) |
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III.3.5 The Nelkin-Ghatak profile |
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89 | (1) |
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III.3.6 Correlated profiles |
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90 | (3) |
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III.3.7 Characteristics of the basic profiles |
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93 | (5) |
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III.4 Speed-dependent line-shape models |
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98 | (40) |
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III.4.1 Observation of speed-dependent inhomogeneous profiles |
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98 | (9) |
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III.4.2 Basic speed-dependent profiles |
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107 | (7) |
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III.4.3 The Rautian-Sobelman model |
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114 | (11) |
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III.4.4 The Keilson-Storer memory model |
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125 | (13) |
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III.5 Ab initio approaches of the line shape |
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138 | (14) |
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III.5.1 The Waldmann-Snider kinetic equation |
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139 | (2) |
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III.5.2 The generalized Hess method |
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141 | (2) |
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III.5.3 Collision kernel method |
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143 | (4) |
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III.5.4 Approaches from a simplified Waldmann-Snider equation |
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147 | (5) |
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III.6 New achievements since 2008 |
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152 | (21) |
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III.6.1 Direct prediction from molecular dynamics simulations |
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153 | (1) |
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III.6.2 Using a kinetic equation |
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154 | (4) |
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III.6.3 Relativistic and dispersion corrections to line-shape models |
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158 | (1) |
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III.6.4 Phenomenological line-shape models |
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159 | (4) |
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III.6.5 Pressure-broadening and-shifting coefficients |
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163 | (6) |
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169 | (4) |
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173 | (1) |
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Appendix III.A Computational aspects |
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174 | (7) |
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III.A1 Algorithms for the Voigt and Galatry profiles |
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175 | (2) |
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III.A2 Computation of speed-dependent profiles |
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177 | (4) |
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IV Collisional line mixing (within clusters of lines) |
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181 | (110) |
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181 | (8) |
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189 | (21) |
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IV.2.1 Approximations and general expressions |
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189 | (5) |
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IV.2.2 Asymptotic expansions |
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194 | (11) |
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IV.2.3 Computational aspects and recommendations |
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205 | (5) |
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IV.3 Constructing the impact relaxation matrix |
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210 | (50) |
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IV.3.1 Simple empirical (classical) approaches |
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211 | (7) |
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IV.3.2 Statistically based energy gap fitting laws |
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218 | (8) |
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IV.3.3 Dynamically based scaling laws |
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226 | (13) |
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IV.3.4 Semiclassical models |
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239 | (12) |
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251 | (9) |
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IV.4 Determining line-mixing parameters from experiments |
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260 | (9) |
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260 | (4) |
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IV.4.2 Relaxation matrix elements |
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264 | (2) |
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IV.4.3 First-order line-coupling coefficients |
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266 | (3) |
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IV.4.4 Mixed theoretical model and measured spectra fitting approaches |
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269 | (1) |
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269 | (4) |
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IV.5.1 Available line-mixing data |
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270 | (1) |
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IV.5.2 Comparisons between predictions and laboratory measurements |
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271 | (2) |
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IV.5.3 Comparisons between predictions and atmospheric measurements |
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273 | (1) |
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IV.6 New achievements since 2008 |
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273 | (8) |
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IV.6.1 Requantized classical molecular dynamics simulations |
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274 | (1) |
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IV.6.2 Quantal approaches |
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274 | (1) |
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IV.6.3 Refined semiclassical Robert-Bonamy formalism |
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275 | (1) |
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IV.6.4 Fully classical formalism |
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276 | (2) |
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IV.6.5 Dynamically based scaling laws |
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278 | (1) |
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IV.6.6 Energy-gap fitting laws and state-to-state cross sections |
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279 | (1) |
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IV.6.7 The ovaloid sphere and hard collision models |
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279 | (1) |
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IV.6.8 Kochanov's approach |
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279 | (1) |
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280 | (1) |
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281 | (1) |
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Appendix IV.A Vibrational dephasing |
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282 | (4) |
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Appendix IV.B Perturbed wave functions |
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286 | (1) |
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Appendix IV.C Resonance broadening |
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287 | (4) |
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V The far wings (beyond the impact approximation) |
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291 | (46) |
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291 | (2) |
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293 | (6) |
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V.2.1 The x factor approach |
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293 | (4) |
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V.2.2 The tabulated continua |
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297 | (1) |
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298 | (1) |
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V.3 Far wings calculations: the quasistatic approach |
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299 | (9) |
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V.3.1 General expressions |
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299 | (3) |
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V.3.2 Practical implementation and typical results |
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302 | (3) |
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V.3.3 The band average line shape: back to the % factors |
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305 | (3) |
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V.4 From resonance to the far wing: a perturbative treatment |
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308 | (3) |
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V.4.1 General expressions |
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308 | (2) |
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V.4.2 Illustrative results |
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310 | (1) |
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V.5 From resonance to the far wing: a nonperturbative treatment |
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311 | (6) |
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V.5.1 General expressions |
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312 | (2) |
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V.5.2 Illustrative results |
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314 | (3) |
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V.6 New achievements since 2008 |
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317 | (10) |
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V.6.1 Direct predictions from classical molecular dynamics simulations |
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317 | (2) |
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V.6.2 Non Markovian energy-corrected sudden approach |
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319 | (1) |
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V.6.3 Asymptotic line shape and x_factor empirical models |
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319 | (1) |
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V.6.4 The MT_CKD water vapor continuum |
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320 | (2) |
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322 | (5) |
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327 | (1) |
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Appendix V.A The water vapor continuum |
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328 | (9) |
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V.A1 Definition, properties, and semiempirical modeling of the H2O continuum |
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330 | (2) |
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V.A2 On the origin of the water vapor continua |
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332 | (1) |
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V.A3 The self- and N2-broadened continua within the v2 band |
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333 | (2) |
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335 | (2) |
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VI Collision-induced absorption and light scattering |
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337 | (38) |
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337 | (1) |
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VI.2 Collision-induced dipoles and polarizabilities for diatomic molecules |
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337 | (2) |
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VI.3 Collision-induced spectra in the isotropic approximation |
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339 | (8) |
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VI.3.1 Two illustrative examples: H2 and N2 |
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339 | (4) |
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VI.3.2 Modeling of the line shape |
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343 | (4) |
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VI.4 Effects of the anisotropy of the interaction potential |
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347 | (7) |
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VI.4.1 Interaction potential |
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349 | (1) |
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VI.4.2 Radiative coupling |
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349 | (5) |
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VI.5 The importance of bound and quasibound states in CIA spectra |
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354 | (3) |
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VI.6 Interference between permanent and induced dipoles (CIA) or polarizabilities (CILS) |
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357 | (9) |
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VI.6.1 Depolarized light scattering spectra of H2 and N2 |
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358 | (3) |
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361 | (4) |
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VI.6.3 Intercollisional dips |
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365 | (1) |
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VI.7 New achievements since 2008 |
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366 | (5) |
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VI.7.1 Quantum scattering advances |
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366 | (1) |
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VI.7.2 Intracollisional interference effects |
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367 | (1) |
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VI.7.3 Standard binary collision treatments |
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368 | (1) |
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Vl.7.4 Direct predictions from classical molecular dynamics simulations |
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368 | (1) |
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VI.7.5 Integrated collision-induced absorption intensities |
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369 | (1) |
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370 | (1) |
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371 | (4) |
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VII Consequences for applications |
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375 | (56) |
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375 | (2) |
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377 | (7) |
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VII.2.1 Radiative heat transfer |
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377 | (3) |
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380 | (4) |
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384 | (8) |
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VII.3.1 The basic Lorentz and Voigt profiles |
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384 | (4) |
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VII.3.2 More refined isolated line profiles |
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388 | (4) |
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VII.4 Line mixing within clusters of lines |
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392 | (8) |
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VII.4.1 Radiative heat transfer |
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392 | (1) |
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392 | (8) |
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VII.5 Allowed band wings and collision-induced absorption |
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400 | (10) |
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VII.5.1 Allowed band wings |
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400 | (7) |
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VII.5.2 Collision-induced absorption |
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407 | (3) |
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VII.6 New achievements since 2008 |
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410 | (18) |
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410 | (9) |
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419 | (5) |
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VII.6.3 Radiative heat transfer and climate modeling |
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424 | (4) |
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428 | (3) |
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VIII Laboratory experimental techniques |
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431 | (18) |
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431 | (4) |
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VIII.2 Cavity-enhanced absorption spectroscopy |
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435 | (2) |
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VIII.3 Cavity ring-down spectroscopy |
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437 | (1) |
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VIII.4 Frequency comb-assisted methods |
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438 | (1) |
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VIII.5 Cavity mode-width and mode-dispersion spectroscopies |
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439 | (3) |
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VIII.6 Direct frequency comb spectroscopy |
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442 | (2) |
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VIII.6.1 Dual comb with two femtosecond lasers |
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442 | (1) |
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VIII.6.2 Dual comb with minicombs |
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443 | (1) |
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VIII.6.3 Comb-based Fourier-transform spectroscopy with subnominal resolution |
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443 | (1) |
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VIII.7 Cavity-enhanced direct frequency comb spectroscopy |
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444 | (1) |
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VIII.8 Dual-laser absorption spectroscopy |
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445 | (1) |
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VIII.9 Fourier-transform spectroscopy methods |
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446 | (1) |
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VIII.10 Advances in coherent terahertz spectroscopy |
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447 | (2) |
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IX Toward future researches |
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449 | (24) |
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449 | (1) |
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IX.2 Dicke narrowing in speed-dependent line-mixing profiles |
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449 | (11) |
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IX.2.1 Models of profiles in the hard collision frame |
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450 | (4) |
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IX.2.2 Experimental tests in multiplet spectra |
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454 | (6) |
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IX.3 From resonances to the far wings |
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460 | (6) |
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IX.3.1 Semiclassical approach |
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461 | (4) |
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IX.3.2 Generalized scaling approach |
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465 | (1) |
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IX.4 Tomorrow's spectroscopic databases |
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466 | (4) |
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470 | (3) |
Abbreviations and acronyms |
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473 | (6) |
Symbols |
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479 | (4) |
Units and conversions |
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483 | (2) |
References |
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485 | (68) |
Index |
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553 | |