8. 1  Successful Achievement of High-Efficiency Wavelength Conversion in the Search for a Blue Pulsed Laser
 


Fig. 8-1 Second harmonic generation from pulsed lasers

Two pulses produced by dividing a short pulse from a Ti:sapphire (fundamental: ~800 nm) laser are diffracted from separate gratings at angles so that each pulse wavefront is tilted at the appropriate angle to propagate in the nonlinear crystal. With the introduction of a frequency distribution (chirp) into the two pulses, second-harmonic generation then occurs when they are superimposed. By adjusting the mismatch of phase- and group-velocity between the two fundamental and second-harmonic pulses, an efficient second-harmonic pulse is produced.


Fig. 8-2 Efficiency of conversion into second-harmonic pulses

Energy conversion efficiency is plotted against input fundamental laser intensity. By the present method, a maximum efficiency of 30% is achieved at 25 GW/cm2. Note that conversion efficiencies without frequency chirp in the fundamental pulses are less than 0.4%.



A 100 TW Ti: sapphire laser which has been developed at JAERI produces ultrashort laser pulses of less than 20 fs duration at about 800 nm. We are attempting to convert the wavelengths of such pulses into shorter values. Our hope is that a shorter wavelength laser, i.e., one having larger photon energy, will bring rapid progress in developing X-ray lasers and in research on the interaction of laser radiation with plasmas.
Laser wavelength (or frequency) conversion is typically made by means of a second-(or higher order) harmonic generation scheme using nonlinear optical crystals such as KH2PO4 (KDP) and BaB2O4 (BBO). This technique is well established for lasers having a uniform frequency. Frequencies of short laser pulses, however, inevitably have a broad distribution. Consequently, adjusting them in a frequency-doubling scheme is difficult.
Our solution involves dispersing the input pulse by means of optical gratings so that each frequency component enters the nonlinear crystal at the appropriate angle to give optimal phase matching (Fig. 8-1). Two fundamental pulses are incident on the nonlinear crystal at angles adjusted so that their pulse wave fronts may propagate in the crystal. On superposition in the crystal, they generate a second-harmonic pulse. Moreover, self-compression of the second-harmonic pulse so generated can also be accomplished by adjusting the incidence angles of the fundamental pulses.
In the preliminary experiments where an efficiency of 0.4% was expected, 30% efficiency was achieved (Fig. 8-2). Under proper conditions, as high as 70% is found to be possible.



Reference
M. Aoyama et al., Noncollinear Second-Harmonic Generation with Compensation of Phase Mismatch by Controlling Frequency Chirp and Tilted Pulse Fronts of Femtosecond Laser Pulses, Jpn. J. Appl. Phys., 39, 3394 (2000).

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Persistent Quest - Research Activities 2001
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