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frequency-selective element. The measurements are shown in Fig. 9.14. Figure 9.14a shows that the center wavelength has a standard deviation of less than 0.02 nm, which is less than one longitudinal mode spacing of about 0.11 nm; as a result, no mode hopping occurs within 100 hours of operation. Figure 9.14b demonstrates that the uctuations of the output power are less than 1.4% of standard deviation. However, an increase in the uctuation level is seen after approximately 50 hours of single-mode operation. This re ects an increase in the temperature uctuations in the surrounding environment, which easily could be avoided by applying temperature stabilization to the etalon. The results in Fig. 9.14 reveal that both the output power and the wavelength of the phase conjugate laser diode array are extremely stable. The reason for such stable output is due to the fact that the phase conjugating crystal dynamically optimizes its internal grating structure to meet the condition of constructive interference in the external cavity.

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FIGURE 14.7. Stepping the phase (top) and integrating over a phase shift (bottom) are alternative methods for temporal phase shifting.

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This chapter has focused on narrowband beamforming and has shown techniques enabling beam patterns with certain characteristics to be designed. Although the discussion has focused on the ULA and uniform planar array, the theory has been generalised enabling it to be applied to non-uniform array structures including circular and spherical arrays. Specific techniques for beamforming with circular arrays is discussed in chapter 5. The functions of the phase and amplitude weights applied to linear and planar arrays have been demonstrated. Examples of phase and amplitude weightings have been given. Furthermore, the impact of element spacing on the generation of (unwanted) grating lobes has been shown. Following this, numerous window functions have been introduced and compared. Beam synthesis through the use of the Dolph-Chebyshev technique has been demonstrated, which enables beam patterns with constant sidelobe levels to be constructed.

FIGURE 13.1. Schematic diagram of an optical imaging system. A point object P at a height h from the optical axis OA is imaged at P0 at a height h0 . AS is the aperture stop, EnP is the entrance pupil, ExP is the exit pupil, and CR is the chief ray.

Figure 30-10: Renaming a file, once called newblank.html, in the Files tab. The file on the server does not change to correspond.

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By using the doubled output redirector (>>), the output of the command is appended to the end of the file instead of replacing the contents of the file. Like the single operator, the double operator creates the file if it doesn t already exist. The double operator can be useful if you want to run a command several different times and compare the output, or if you want to log the operation of several different commands.

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