Note continued:9.14.Super-Excited States of Molecules Inside a Filament --9.15.Looking Ahead and Conclusion --References --10.Diagnosing Intense and Ultra-intense Laser-Matter Interactions: Status and Future Requirements /Leonida A. Gizzi --10.1.Introduction on Ultra-Intense Laser-Matter Interactions --10.2.Optical Interferometry and Propagation Issues --10.3.Time-Resolved X-Ray Spectroscopy and Imaging --10.4.Fast Electron Production and Characterization --10.5.Summary and Future Instrumentation Requirements --References.
متن يادداشت
Note continued:6.Nonlinear Interaction of Strong XUV Fields with Atoms and Molecules /Katsumi Midorikawa --6.1.Introduction --6.2.Generation of High-Power High-Order Harmonics --6.3.Spatial Properties of High-Order Harmonics --6.4.Characterization of Attosecond Pulses by PANTHER --6.5.Autocorrelation Measurement of Attosecond Pulses by Molecular Coulomb Explosion --6.6.Summary --References --7.Ultrafast X-Ray Absorption Spectroscopy Using Femtosecond Laser-Driven X-Rays /Hidetoshi Nakano --7.1.Introduction --7.2.Soft X-Ray Emission from Femtosecond Laser-Produced Plasma --7.3.Time-Resolved XAFS Measurement of Optically Excited Silicon --7.4.Spatiotemporally Resolved XAS --7.5.Summary --References --8.Quantum Emission and Its Application to Materials Dynamics /Kazutaka G. Nakamura --8.1.Introduction --8.2.Quantum Emission --8.3.Time-Resolved Imaging with Quantum Emission --8.4.Time-Resolved X-Ray Diffraction --8.5.Summary --References --9.Filamentation Nonlinear Optics /See Leang Chin --9.1.Introduction --9.2.Self-Focusing and Filamentation Physics --9.3.Theoretical Model and Simulation --9.4.Background or Energy Reservoir --9.5.Extraordinary Properties of Filaments --9.6.Long-Distance Propagation in Air --9.7.Clean Fluorescence --9.8.Self-Pulse Compression --9.9.Self-Spatial Filtering --9.10.Self-Group Phase Locking --9.11.Nonlinear Optics Inside the Filament Core --9.12.Four-Wave Mixing Inside the Filament Core --9.13.Detection of Chemical and Biological Agents in Air Based on Clean Fluorescence --9.13.1.Halocarbons --9.13.2.CH4 --9.13.3.Ethanol Vapor --9.13.4.CH4 in air --9.13.5.Bio-agents: Egg White and Yeast Powders --9.13.6.Summary of Remote Sensing Feasibility Using Only One Laser --
متن يادداشت
Note continued:3.3.4.Wavelength Scaling of the Photoelectron Spectra --3.3.5.Wavelength Scaling of the Ionization Rate: TDSE vs. Tunneling Theory --3.3.6.Intensity Scaling of the Rescattering Plateau --3.3.7.Wavelength Scaling of the Rescattering Plateau --3.3.8.Ionization of Scaled Systems --3.3.9.Low Energy Structure in the Photoelectron Energy Spectra --3.4.MIR High Harmonics and Attophysics --3.4.1.Scaling of the Harmonic Cutoff --3.4.2.Scaling of the Group Delay Dispersion --3.4.3.Scaling of the Harmonic Yield --3.5.Tomographic Reconstruction of Molecular Orbitals --References --4.How Do Molecules Behave in Intense Laser Fields? Theoretical Aspects /Hirohiko Kono --4.1.Introduction --4.2.Electronic and Vibrational Dynamics of H+2 in a Near-IR Field --4.3.Time-Dependent Adiabatic State Approach and Its Application to Large Amplitude Vibrational Motion of C60 Induced by Near-IR Fields --4.4.Bond Dissociation Dynamics of Ethanol: Branching Ratio of C-C and C-O Dissociation --References --5.Pulse Shaping of Femtosecond Laser Pulses and Its Application of Molecule Control /Fumihiko Kannari --5.1.Introduction --5.2.Femtosecond Laser Pulse Shaping with a 4f Pulse Shaper --5.3.Spatiotemporal Coupling at 4f Pulse Shapers --5.4.Replica Pulse Formation with a Pixelated SLM Pulse Shaper --5.5.Femtosecond Laser Pulse Shaping with an AOPDF --5.6.How to Generate the Desired Ultrashort Laser Pulse in an Actual Laser System: Case 1: We Know the Desired Pulse Shape --5.7.How to Generate the Desired Ultrashort Laser Pulse in an Actual Laser System: Case 2: We Do Not Know What the Desired Pulse Shape Is --5.8.Adaptive Pulse Shaping for Dissociative Ionization of Ethanol Molecules --5.9.Adaptive Pulse Shaping of Two-Photon Excited Fluorescence Efficiency --References --