Phase Conjugate Laser Optics

Chapter 5.4.3.2 - Bi-exponential oscillator buildup

5.4.3.2   Bi-exponential oscillator buildup   As can be seen in the hysteresis
of the data curves in Fig. 5.17, even when using the SBS loop geometry, the lowest
possible threshold is not achieved with the 60-ns input pulse rise times required for
500- to 1000-ns pulse amplification. One way of lowering the transient SBS
threshold and reducing the size of the observed hysteresis loop is to reduce the
temporal slope of the input pulse. To accomplish this, a Pockels cell was inserted in
the ring oscillator and was used to introduce a ~10% loss during the early part of the
oscillator buildup. This increased the time constant for the exponential growth to
150 ns, which is approximately 10 times the 15-ns Brillouin time constant for the
90 atm N2. The voltage from the Pockels cell is removed at an adjustable point
during the oscillator buildup as monitored by a photodiode. This point is adjusted to
occur just after the SBS phase conjugate mirror reaches threshold. When the loss
from the Pockels cell is removed from the oscillator resonator, the buildup time then
decreases from 150 ns to the 60 ns required for the previously described optimal
extraction from the laser amplifier. The slower buildup also helps to ensure single-
frequency output from the ring oscillator. Figure 5.18a shows a measured temporal


Figure 5.18. (a) Measured injected oscillator pulse used to generate 500-ns output pulses. The logarithmic plot shown in (b) illustrates the bi-exponential buildup used to lower the transient SBS threshold. The necessary dynamic range for the measured profile shown in this plot was achieved by dividing the curve into four temporal windows and simultaneously collecting each on separate channels of a digital oscilloscope with 10_ steps in gain between each channel.

profile of a typical oscillator input pulse. The bi-exponential output growth is clearly
seen in the logarithmic plot in Fig. 5.18b.

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