| 762 | 217 |
|---|
| Introduction and motivation | 762 |
| Femtosecond thin disk laser | 762 |
| Photoelectron imaging spectroscopy (PEIS) | 763 |
| Summary and conclusions | 764 |
| Ultra-high intensity-High Contrast 300-TW laserat 0.1 Hz repetition rate. | 765 |
| 1. Introduction | 765 |
| 2. Laser design | 765 |
| 3. Experimental results | 766 |
| 4. Conclusion | 767 |
| Highly Efficient, Low-Cost Diode-PumpedFemtosecond Cr3+:LiCAF Lasers | 768 |
| Introduction | 768 |
| Experimental Setup | 769 |
| Results and Discussion | 769 |
| Conclusions | 770 |
| Environmentally stable 200-fs Yb-doped fiberlaser with dispersion compensation by photoniccrystal fiber | 771 |
| 1. Introduction | 771 |
| 2. Photonic crystal fiber | 771 |
| 3. Environmentally stable mode-locked laser | 772 |
| 4. Conclusions | 773 |
| Noncollinear Optical Parametric AmplificationPumped by the Third Harmonics ofa Ti:sapphire Laser | 774 |
| Introduction | 774 |
| Experiments | 774 |
| Results and Discussion | 775 |
| Conclusion | 776 |
| Sub-10 fs Pulse Generation in Vacuum UltravioletUsing Chirped Four Wave Mixing in HollowFibers | 777 |
| Introduction | 777 |
| Results and Discussion | 778 |
| Conclusions | 779 |
| Generation of High Energy Pulses from a FiberbasedFemtosecond Oscillator | 780 |
| Introduction | 780 |
| Experimental Methods | 780 |
| Results and Discussion | 781 |
| Conclusions | 782 |
| Femtosecond passively mode-locked fiber lasersusing saturable Bragg reflectors | 783 |
| Introduction | 783 |
| Experimental Results | 783 |
| Linear soliton laser | 783 |
| Stretched-pulse laser | 784 |
| Discussion and conclusion | 785 |
| Noncollinear optical parametric amplification ofcw light, continua and vacuum fluctuations | 786 |
| Influence of the seed light on the output of parametric amplifiers | 786 |
| Amplification of cw light in femtosecond and picosecond pumped NOPAs | 786 |
| Comparison of cw-, continuum- and OPG-seeded NOPAs in the fs-regime | 787 |
| Modeling of Octave-Spanning Sub-Two-CycleTitanium:Sapphire Lasers: Simulation andExperiment | 789 |
| Introduction | 789 |
| Laser Model | 789 |
| Experimental Setup | 790 |
| Pulse Dynamics in the Laser | 790 |
| Conclusions | 791 |
| Ultra-Broadband Infrared Pulses from aPotassium-Titanyl Phosphate Optical ParametricAmplifier for VIS-IR-SFG Spectroscopy | 792 |
| Chirped-pulse Raman amplification fortwo-color high-intensity laser experiments | 795 |
| Introduction | 795 |
| Results and Discussion | 796 |
| Generation of Broadband mid-infrared Pulsesfrom an Optical Parametric Amplifier | 798 |
| References | 800 |
| Optimized 2-micron Optical Parametric ChirpedPulse Amplifier for High Harmonic Generation | 801 |
| Generation of sub-20-fs, two-colordeep-ultraviolet pulses by four-wave mixingthrough filamentation in gases | 804 |
| Efficient ultrafast four-wave opticalparametric amplification in condensed bulkmedia | 807 |
| Introduction | 807 |
| Experimental Methodology | 807 |
| Results and Discussion | 808 |
| Conclusions | 809 |
| Cascaded four-wave mixing technique for highpowerfew-cycle pulse generation | 810 |
| Introduction | 810 |
| Experimental setup and results | 811 |
| Conclusions | 812 |
| 2 MHz repetition rate - 15 fs fiber amplifierpumped optical parametric amplifier | 813 |
| Introduction | 813 |
| Experiment and Results | 813 |
| Scaling Considerations | 815 |
| Conclusions | 815 |
| Octave-wide tunable NOPA pulses at up to 2 MHzrepetition rate | 816 |
| Complete spectral coverage for ultrafast spectroscopy | 816 |
| Octave-wide tunability with femtosecond UV pumping | 817 |
| Investigation of phase dependencies in optical parametric amplification | 817 |
| Asymptotic pulse shapes and pulseself-compression in femtosecond filaments | 819 |
| Efficient and Highly Coherent Extreme-Ultraviolet High-Harmonic Source | 822 |
| Introduction | 822 |
| Experimental Methods | 822 |
| Results and Discussion | 823 |
| Conclusions | 824 |
| References | 824 |
| Single-stage Pulse Compression and High-EnergySupercontinuum generation from a Chirped-pulseoscillator | 825 |
| Introduction | 825 |
| Experimental setup | 826 |
| Results and Discussion | 826 |
| An All-Optical Synchrotron
|