Femtosecond Laser SpectroscopyPeter Hannaford Springer Science & Business Media, 27.12.2005 - 334 Seiten The embryonic development of femtoscience stems from advances made in the generation of ultrashort laser pulses. Beginning with mode-locking of glass lasers in the 1960s, the development of dye lasers brought the pulse width down from picoseconds to femtoseconds. The breakthrough in solid state laser pulse generation provided the current reliable table-top laser systems capable of average power of about 1 watt, and peak power density of easily watts per square centimeter, with pulse widths in the range of four to eight femtoseconds. Pulses with peak power density reaching watts per square centimeter have been achieved in laboratory settings and, more recently, pulses of sub-femtosecond duration have been successfully generated. As concepts and methodologies have evolved over the past two decades, the realm of ultrafast science has become vast and exciting and has impacted many areas of chemistry, biology and physics, and other fields such as materials science, electrical engineering, and optical communication. In molecular science the explosive growth of this research is for fundamental reasons. In femtochemistry and femtobiology chemical bonds form and break on the femtosecond time scale, and on this scale of time we can freeze the transition states at configurations never before seen. Even for n- reactive physical changes one is observing the most elementary of molecular processes. On a time scale shorter than the vibrational and rotational periods the ensemble behaves coherently as a single-molecule trajectory. |
Inhalt
| 1 | |
I2 hyperfine interactions optical frequency standards | 14 |
Femtosecond lasers and external optical cavities | 21 |
Extreme | 29 |
Phase preservation in the supercontinuum generation | 39 |
Phase preservation in chirpedpulse amplification | 54 |
The Measurement of Ultrashort Light Simple Devices | 61 |
OPA XFROG for measuring ultraweak fluorescence | 68 |
A New Probe | 166 |
Spectrally Resolved TwoColour Femtosecond Photon Echoes | 197 |
Molecular systems | 217 |
Optimal Control of Atomic Molecular and Electron | 225 |
Manyparameter control in the gas phase | 243 |
Manyparameter control in the liquid phase | 252 |
102 | 256 |
Concusions | 262 |
Extremely simple FROG device | 75 |
Femtosecond Combs for Precision Metrology | 87 |
B CHATEL 267 Laboratoire de Collisions Agrégats et Réactivité CNRS | 107 |
Infrared Precision Spectroscopy using FemtosecondLaser | 109 |
RealTime Spectroscopy of Molecular Vibrations with | 133 |
B GIRARD 267 Laboratoire de Collisions Agrégats et Réactivité CNRS | 267 |
Ultrafast Processes of Highly Excited WideGap Dielectric | 305 |
| 331 | |
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3-pulse photon echo absorption spectrum amplitude atomic attosecond axis band bandwidth beam calculated cavity Chem chirp component correlation spectra corresponding crystal decay delay detected dispersion dynamical linewidth electric field electron evolution excited excited-state exciton experimental experiments femtosecond pulses FFCF fiber Figure frequency comb function GRENOUILLE harmonic hydrogen bond hydroxyl hydroxyl stretch interaction interference ionization J-aggregates laser intensity Lett measured MeOD mode-locked modulation molecules nonlinear nonlinear optical observed oligomers optical clock optical coherences optical frequency optical parametric amplifier optimization oscillation parameters phase-matching photo-electron photon echo signals photon echo spectra photoproduct peak Phys population porphyrin pulse shape pump pulse pump-probe Q-band quantum control region resonance shift shown in Fig simulations soliton spatial spectral broadening spectral diffusion spectrally resolved spectroscopy structure supercontinuum tapered fibres temporal Ti:Sapphire laser transition dipole transition dipole moment two-photon ultrashort ultrashort pulses vibronic coupling wave-packet motion wavelength width
