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Extra resources for The Fine Structure of Certain Lines and Energy Levels of Cadmium
Another significant technological difficulty in increasing the average output power of such a laser amplifier is the thermal management of the Ti:sapphire crystal which inevitably links the amplified pulse repetition rate and the pulse energy. Searching for a more economical approach, we have designed a laser system based on optical parametric chirped pulse amplification (OPCPA) [8,9]. -5 0 Time [fs] 5 10 110 120 130 Photon energy [eV] 140 50 60 70 80 90 Photoelectron energy [eV] Fig. 2. Generation of isolated attosecond pulses from the spectral edge of the higher-order harmonic emission, (a) optical driver fields for to various settings of the carrier-envelope phase, (b) corresponding XUV spectra in the cut-off region, (c) streak images proving the presence of an isolated attosecond pulse (for "cos"- and "-cos"-like fields) and a double pulse (for the "sin" field).
Whereas it is possible to generate 4-fs pulses using the pump wavelength around 400 nm , for the 532-nm pump, the gain bandwidth is significantly reduced and covers only about 125 THz. Pump pulses are obtained from a 20-Hz repetition-rate amplifier that is seeded by an independent picosecond seed oscillator. The repetition rates of the ps oscillator and of the fs Tiisapphire oscillator are actively locked to an external master clock with an estimated rms timing jitter below 2 ps. The broadband pulses from the fs oscillator are stretched in a negative dispersion stretcher to match the pump pulse duration.
2(B)). T h e corresponding temporal intensity and phase were retrieved. 8 fs (center wavelength: 580 nm) (see Fig. 3). 75fs). This is the shortest clean single TL pulse in the visible and near-infrared region. 0 Time [fs] Fig. 3. Retrieved temporal profiles. Pulse intensities (A) before and (B) (i) after 2nd feedback compensations and (ii) temporal phase after 2nd feedback compensation, (iii) Temporal intensity of Fourier transform limited pulses. References 1. A. Baltuska, T. Fuji, and T. Kobayashi, Opt.