초강력 펨토초 레이저마당 내의 원자조작을 통한 결맞는 X-선 광원 개발 = Coherent X-Ray source development by manipulating atoms in a super-intense femtosecond laser field

목차 (Table of Contents)

• 목차
• Ch. 1. Research Objectives and Evaluation Criteria = 2
• A. Proposed objectives = 2
• B. Evaluation criteria = 3
• Ch. 2. Current Trend and Future Directions = 4
• Ch. 3. Progress Analysis = 12
• A. Degree of objective fulfillment = 12
• B. Self evaluation = 21
• Ch. 4. Planned Approaches for the Research(methods) = 24
• Ch. 5. Results = 29
• A. Research details = 29
• B. Research results = 39
• Ch. 6. Details of Research Achievements = 43
• A. Journal papers = 43
• B. International Conferences = 45
• Appendix (Ⅰ) Research results of FY 1999
• A.1. High harmonic X-ray generation = 1
• A.1.1. Continuously tunable high harmonic X-ray generation from atoms in an intense femtosecond laser field = 1
• A.1.2. Nonadiabatic blueshift of high harmonics from Ar and Ne atoms in an intense femtosecond laser field = 10
• A.1.3. Control of the spectral structure of high harmonics using chirped laser pulses = 32
• A.1.4. Selection of high harmonics from a single quantum path for attosecond pulse generation = 42
• A.2. Theory development of high harmonic generation = 53
• A.2.1. Coherent sum technique = 54
• A.2.2. Time-frequency analysis = 61
• A.3. Operation and development of femtosecond terawatt lasers = 79
• A.3.1. Development of a 1 kHz femtosecond terawatt laser = 79
• A.3.2. Temporal structure of chirped laser pulses = 96
• A.3.3. Focused spot size and intensity measurement in a femtosecond terawatt Ti : sapphire laser = 111
• A.3.4. Incorporation of a cavity-dumped oscillator in a femtosecond terawatt Ti : sapphire laser = 119
• Appendix (Ⅱ) Research results of FY 2000
• A.1. High harmonic X-ray generation
• A.1.1. Coherent control of high-order harmonics with chirped femtosecond laser pulses = 1
• A.1.2. Continuously tunable high-harmonic x-rays from atoms in an intense femtosecond laser field = 10
• A.1.3. Bright, low-divergence high-order harmonic generation in a long gas jet = 22
• A.2. Theory development of high harmonic generation
• A.2.1. Self-phase modulation of laser pulse propagating in an ionizing medium = 30
• A.2.2. Propagation of high-order harmonics = 34
• A.2.3. Attosecond pulse generation = 37
• A.3. Operation and development of femtosecond terawatt lasers
• A.3.1. Development of a 1 kHz femtosecond terawatt laser = 47
• A.3.2. Graphical interpretation of instantaneous carrier frequency of chirped femtosecond pulses using the Wigner time-frequency distribution = 68
• A.3.3. Temporal characterization of femtosecond laser pulses using spectral phase interferometry for direct electric-field reconstruction(SPIDER) = 81
• A.3.4. Adaptive pulse compression using a mirco-machined deformable mirror = 5
• A.4. Emission of a hot electron jet from intense femtosecend laser-cluster interactions = 105
• Appendix (Ⅲ) Research results of FY 2001
• A.1. High harmonic x-ray generation
• A.1.1. Chirp analysis of high-order harmonics from atoms driven by intense femtosecond laser pulse = 1
• A.1.2. Generation of high harmonics with low beam divergence and good wavelength tunability = 13
• A.1.3. Wave-front phase measurements of high-order harmonic beams using the point-diffraction interferometry = 20
• A.2. Theory of high harmonic generation
• A.2.1. Time-frequency analysis of high harmonic generation = 29
• A.2.2. Ion momentum distributions for He single and double Ionization in strong laser field = 35
• A.2.3. Frequency dependence of non-sequential double ionization = 50
• A.3. Development of high power femtosecond laser technology
• A.3.1. Performance improvement of a 1 kHz femtosecond high-power laser = 60
• A.3.2. Electric-field recovery of sub-10-fs laser pulses from interferometric autocorrelation using an evolutionary strategy = 69
• A.3.3. Measurement of shot-to- shot carrier-envelope phase slip of femtosecond laser pulses = 83