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zigzag slab ampli er architecture [8] and SBS phase conjugation Accurate wavefront correction is not just a requirement dictated by the divergence needs of an intended application of the laser High-beam-quality operation is rst necessary for high-average-power operation with high pulse energies, providing optimal ampli er beam ll and optical extraction as well as preventing damage to optical components In addition to the low output divergence enabled by nonlinear phase conjugation, other bene ts include very high pulse-to-pulse and long-term beam pointing stability as well as the ability to phase-lock multiple ampli er apertures to generate even higher-energy beams High beam quality also provides the option of very ef cient harmonic wavelength conversion Although the Nd:glass gain medium exhibits a lower fracture strength and lower thermal conductivity than do crystalline materials such as Nd:YAG, its availability in large volumes and its small cross section for stimulated emission (3.

to limit the dose delivered to the patient. Therefore detector ef ciency is a crucial consideration in selecting the detector system. The basic principle of image reconstruction is the same in ECT as in transmission CT except that the signal in ECT is composed of -rays that become attenuated during their ight from the emitting nuclei to the detectors. To minimize the contribution from scattered radiation, the ECT uses the characteristics of monoenergetic energy in setting up a counting window to discriminate the lower energy scattered radiation from the high-energy primary radiation. There are two major categories in ECT: single photon emission CT (SPECT) and positron emission CT (PET).

5 10220 cm2) make it well-suited to the storage requirements of high energy per pulse operation At the same time, the high saturation uence for Nd-doped phosphate glass and the potentially large thermally induced distortions resulting from its low thermal conductivity offer a signi cant challenge for the operation of a high-average-power ampli er system Good thermal management in the form of uniform pumping deposition, uniform cooling, and an optimized ampli er slab design is crucial to successful high-power operation Even under ideal conditions, the high uence required for ef cient energy extraction requires carefully designed beam transport and the accurate correction of the remaining thermally induced wavefront aberrations in the ampli er medium in order to avoid damage to optical components For this reason, the ashlamp-pumped Nd:glass ampli er system has been a valuable test bed for the development of high-average-power solid-state ampli er architectures.

S11, S21 (dB)

The result has been robust optical designs that are also readily applicable to high-average-power diode-pumped crystalline ampli er systems having lower optical uences We believe that through this development work, a number of valuable design principles have resulted which are directly applicable to SBS phase conjugated MOPA architectures in general, and these will be reviewed at the end of the chapter To illustrate the design principles for a high-pulse-energy, high-average-power, SBS phase conjugated MOPA, we have chosen to present summarized technical descriptions of three laser systems Each of these shares a common ashlamppumped Nd:glass ampli er design operating at 1053 nm [9] The rst system is a 25J/pulse, 15-ns laser using a liquid SBS phase conjugate mirror The second extends this pulse duration to 500 ns and uses a high-pressure-gas SBS cell with a selfpumped four-wave-mixing loop geometry to lower the phase conjugation threshold and to provide narrow spectral bandwidth.

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FIGURE 17-22: A working pointer will come in handy soon!