Abstract:A wavelength-independent method for optical gating, based on the optical Kerr effect, has been demonstrated. Using this method, we produced 100-ps, 10-kW, two-wavelength pulses (10.3 and 10.6 microm) with a signal-to-background ratio contrast of 10(5) by slicing a long CO2 pulse. The capability of gating consecutive pulses separated on a picosecond time scale with this method is also shown.
“…Since the temporal measurements are performed using a streak camera, the 10 μm radiation is first converted to visible light by copropagating the output radiation with a red diode probe laser through a CS 2 Kerr cell [13]. Due to the fast (∼1 ps) response time of CS 2 , this interaction effectively transcribes the temporal information of the 10 μm pump to the visible probe.…”
We report on the generation of supercontinuum radiation from 2 to 20 μm in a 67 mm long GaAs crystal pumped by a train of 3 ps CO2 laser pulses. Temporal measurements indicate that sub-picosecond pulse splitting is involved in the production of such wide-bandwidth radiation in GaAs. The results show that the observed spectral broadening is heavily influenced by four-wave mixing and stimulated Raman scattering.
“…Since the temporal measurements are performed using a streak camera, the 10 μm radiation is first converted to visible light by copropagating the output radiation with a red diode probe laser through a CS 2 Kerr cell [13]. Due to the fast (∼1 ps) response time of CS 2 , this interaction effectively transcribes the temporal information of the 10 μm pump to the visible probe.…”
We report on the generation of supercontinuum radiation from 2 to 20 μm in a 67 mm long GaAs crystal pumped by a train of 3 ps CO2 laser pulses. Temporal measurements indicate that sub-picosecond pulse splitting is involved in the production of such wide-bandwidth radiation in GaAs. The results show that the observed spectral broadening is heavily influenced by four-wave mixing and stimulated Raman scattering.
“…This strategy has been applied to generate, 20 GW (60 mJ, 3 ps) CO 2 laser pulses. Figure 3 is a streak camera measurement of the output of this system, upconverted to the visible range [12]. Similar to the simulated pulse train of Fig.…”
Section: Gw 3 Ps High Repetition Rate Co 2 Laser System At the Nmentioning
Abstract.We hereby present an ongoing experiment where high power, sub-picosecond 10 µm laser pulses will be produced at 1 Hz. To achieve this 3 ps pulses of a 2 GW CO 2 laser were broadened via self-phase modulation in GaAs and compressed in a dispersive element. Temporal and spectral data are presented which demonstrate the possibility of compression by more than a factor of 3.
“…A 200 ns-long pulse from a gratingtunable, single-longitudinal mode TEA CO 2 laser is used for this purpose. In order to generate a picosecond seed pulse, the 10 µm output beam is modulated by an ultrafast 1 µm pulse from a Nd:glass CPA system in a Kerr nonlinear medium [13]. The Kerr modulator can be used in combination with a Ge semiconductor switch to increase the contrast of a sliced pulse.…”
Section: Current Status Of Picosecond Co 2 Lasersmentioning
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