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The main beam can be steered by applying a phase taper across the elements of the array. For example, by applying phases of 0" and 70" to each element of a two-element array with X/2 spacing between the elements, the beam is steered to 35", as shown in figure 2.3. The figure also shows the radiation pattern when zero phase weights are applied, i.e., the main beam is steered towards boresight and a gain of 3 dB is shown. The following section describes a method for computing the required weights to steer the main beam to a desired angle. Phase weights for narrowband arrays, which is the focus of this chapter, are applied by a phase shifter, However, where wideband beamforming is considered, which is the focus of chapter 4,it is important to distinguish between phase-shifter arrays and delay arrays. The first generates a phase shift for a certain frequency of

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necessary, however, to note that the thermal grating system had greater losses than the gain-grating system Losses arise from the NRTE that had a backward transmission (T2) somewhat less than 80% (principally due to the Glan-air polarizer losses), and the thermal absorption cell has a transmission of 74% These loss elements are most severe because they are the nal elements after the ampli ers and before the output of the laser system It implies an energy before these elements of almost 400 mJ (or 35% energy extraction ef ciency and 80% ef ciency within the lasing mode volume) The NRTE in the gain-grating system is not so severe since it is intermediate to the two ampli er rods and hence the transmission loss is not at the high power output side of the cavity.

k n X j n m T j Bj n;m : j j 1 k n X j m Sj Bj n;j m : j j 1 k 1 n XX n 0 m 0 k 1 n XX n 0 m 0

Proof. The least squares criterion J ( t ) is the sum of four scalar terms:

This discussion suggests that a more ef cient version of this cavity might be to place the nal ampli er next to the thermal cell, although this would mean that this ampli er is more saturated by the input beam before it has been attenuated by the forward pass of the NRTE While the loss of the NRTE can, in principle, be reduced to a negligible level, the loss due to the absorption of the solution in the thermal cell is inherent to the system since it is necessary for production of the dynamic nonlinear grating mechanism A lower absorption in the cell can be used then in this case, but the threshold input energy would be increased since the induced grating diffraction ef ciency is dependent on the absorption of the cell [see Eq (52)].

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