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Picosecond pulse

Especially with LTG GaAs, materials became available that were nearly ideal for time-resolved THz spectroscopy. Due to the low growth temperature and the slight As excess incorporated, clusters are fonned which act as recombination sites for the excited carriers, leading to lifetimes of <250 fs [45], With such recombination lifetunes, THz radiators such as dipole anteimae or log-periodic spirals placed onto optoelectronic substrates and pumped with ultrafast lasers can be used to generate sub-picosecond pulses with optical bandwidths of 2-4 THz. Moreover, coherent sub-picosecond detection is possible, which enables both... [Pg.1249]

Mollenauer L F, Stolen R H and Gordon J P 1980 Experimental observation of picosecond pulse narrowing and solitons in optical fibres Phys. Rev. Lett. 45 1095-7... [Pg.1993]

Fig. 4. Temporal pulse characteristics of lasers (a) millisecond laser pulse (b) relaxation oscillations (c) Q-switched pulse (d) mode-locked train of pulses, where Fis the distance between mirrors and i is the velocity of light for L = 37.5 cm, 2L j c = 2.5 ns (e) ultrafast (femtosecond or picosecond) pulse. Fig. 4. Temporal pulse characteristics of lasers (a) millisecond laser pulse (b) relaxation oscillations (c) Q-switched pulse (d) mode-locked train of pulses, where Fis the distance between mirrors and i is the velocity of light for L = 37.5 cm, 2L j c = 2.5 ns (e) ultrafast (femtosecond or picosecond) pulse.
It is also possible to switch a single picosecond pulse out of the train of mode-locked pulses using an electrooptic switch. It is possible to obtain a single pulse having duration in the picosecond regime or even less. Pulses with durations in the regime of a few hundred femtoseconds (10 s) are also available (Fig. 4e). [Pg.5]

The disadvantage of lasers with nanosecond-picosecond pulse duration for depth profiling is the predominantly thermal character of the ablation process [4.229]. For metals the irradiated spot is melted and much of the material is evaporated from the melt. The melting of the sample causes modification and mixing of different layers followed by changes of phase composition during material evaporation (preferential volatilization) and bulk re-solidification [4.230] this reduces the lateral and depth resolution of LA-based techniques. [Pg.233]

The electron itself is frequently used as a primary source of radiation, various kinds of accelerators being available for that purpose. Particularly important are pulsed electron sources, such as the nanosecond and picosecond pulse radiolysis machines, which allow very fast radiation-induced reactions to be studied (Tabata et al, 1991). Note that secondary electron radiation always constitutes a significant part of energy transferred by heavy charged particles. For these reasons, the electron occupies a central role in radiation chemistry. [Pg.6]

With the advent of picosecond-pulse radiolysis and laser technologies, it has been possible to study geminate-ion recombination (Jonah et al, 1979 Sauer and Jonah, 1980 Tagawa et al 1982a, b) and subsequently electron-ion recombination (Katsumura et al, 1982 Tagawa et al, 1983 Jonah, 1983) in hydrocarbon liquids. Using cyclohexane solutions of 9,10-diphenylanthracene (DPA) and p-terphenyl (PT), Jonah et al. (1979) observed light emission from the first excited state of the solutes, interpreted in terms of solute cation-anion recombination. In the early work of Sauer and Jonah (1980), the kinetics of solute excited state formation was studied in cyclohexane solutions of DPA and PT, and some inconsistency with respect to the solution of the diffusion equation was noted.1... [Pg.295]

Since then, number of researcher have studied and experimented with TRS including Chance and Oda [61] [63] [76] [80] [81] [73] [82] [113] [114], TRS instruments rely on a picosecond pulsed laser with a detector that is designed to detect the time evolution of the light intensity [44], With the time profile of light intensity through the medium, it is possible to measure both absorption and reduced scattering coefficients [32], A ma-... [Pg.344]

Picosecond pulses (lps = 10 12s) are produced by mode locking, where the electronics of the instrumentation open and close the shutter at the round-trip frequency of the cavity. [Pg.24]

Figure 6.4. Wavelength distribution of output from a picosecond pulsed titanium sapphire laser. Output at... Figure 6.4. Wavelength distribution of output from a picosecond pulsed titanium sapphire laser. Output at...
Most optical centers show luminescence decay times in the nanoseconds-milliseconds range. However, many other physical processes involved in optical spectroscopy are produced in the picoseconds-femtoseconds range, and mnch more complicated instrumentation becomes necessary. For instance, interband Inminescence in solids, which is of particular interest in semiconductors, can involve decay times in the range of picoseconds. Pulses generated from solid state lasers have already reached this femtosecond domain. [Pg.108]

A common way to treat the problem of a picosecond pulse propagation in regular dielectric waveguide with Kerr nonlinearity was to solve the nonlinear Schrodinger equation (NLSE) for the slowly varying temporal amplitude of electrical field ... [Pg.151]

Y.Q. Li, D. Guzun, G. Salamo, and M. Xiao, High-efficiency blue-light generation by frequency doubling of picosecond pulses in a thick KNbOs crystal. Journal of the Optical Society of America B 20(6), 1285-1289 (2003). [Pg.225]

An interesting method for generation of a broad wavelength continuum with a time duration of some picoseconds has been deseribed by Busch et al. I61e) By focussing the intense mode locked laser beam from a frequency-doubled neodynium laser into various liquids (H2O, P2O, etc.) a light continuum can be generated which spans several thousand wave numbers and yet has a picosecond pulse duration. This enables absorption spectroscopy measurements to be made in the picosecond time scale. [Pg.37]

Periasamy, A., Wodnicki, R, Wang, X.R, et al. 1996. Time-resolved fluorescence lifetime imaging microscopy using a picosecond pulsed tunable dye laser system. Rev. Sci. Instrum. 67 3722. [Pg.70]

Petrov, G. L, Yakovlev, V. V., and Minkovski, N. I. 2003. Near-infrared continuum generation of femtosecond and picosecond pulses in doped optical fibers. Appl. Phys. B 77 219-25. [Pg.164]

With the development of the picosecond pulse radiolysis, the kinetics data of the geminate ion recombination have been directly obtained. The history of picosecond and subpicosecond pulse radiolysis is shown in Fig. 7. Very recently, the first construction of the femtosecond pulse radiolysis and the improvement of the subpicosecond pulse radiolysis started in Osaka University. [Pg.278]

The first picosecond pulse radiolysis experiment was carried out in the late 1960s by the so-called stroboscopic method (generally pomp and probe method) at University of... [Pg.278]

Now several picosecond pulse radiolysis systems are operating in Argonne National Laboratory, Brookhaven National Laboratory and University of Tokyo and are under construction in University of Paris South and Waseda University, although only one sub-picopulse radiolysis is operating in Osaka University. [Pg.282]

Reactions of e. It is convenient to consider these reactions here. That the electron can react with solutes before it becomes solvated is clearly demonstrated by the data in Fig. 3, which were obtained by picosecond pulse radiolysis [31]. The data show that there is no good correlation between the C37 value of a solute and its rate constant k for reaction with measured at the same high concentrations of solute used to determine C37. The parameter C37 is the concentration of solute that lowers the earliest measurable value of G(gaq) to 37% of the value obtained in the absence of solute. A linear correlation between C37 and k would be expected if the solute merely reacted with e before this earliest time of... [Pg.340]

Details of the picosecond pulse radiolysis system for emission (7) and absorption (8) spectroscopies with response time of 20 and 60 ps, respectively, including a specially designed linear accelerator (9) and very fast response optical detection system have been reported previously. The typical pulse radiolysis systems are shown in Figures 1 and 2. The detection system for emission spectroscopy is composed of a streak camera (C979, HTV), a SIT... [Pg.151]

Figure 1. The schematic diagram of the picosecond pulse radiolysis system for emission spectroscopy. Figure 1. The schematic diagram of the picosecond pulse radiolysis system for emission spectroscopy.

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See also in sourсe #XX -- [ Pg.24 ]

See also in sourсe #XX -- [ Pg.278 ]




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Picosecond

Picosecond Pulsed Dye Lasers

Picosecond laser pulse

Picosecond laser pulse excitation

Picosecond laser pulses, and

Picosecond laser pulses, reliability

Picosecond pulse radiolysis

Picosecond-pulsed laser

Pulse picosecond time resolution

Pulse trains, picosecond

Relaxation processes, picosecond laser pulse study

Twin picosecond pulse system

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