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FIGURE 1 Geometry of diffraction by a rectangular grating. P1: GPJ/GLQ P2: FJU Final Pages Encyclopedia of Physical Science and Technology EN004I-174 June 8, 2001 17:22 423 Diffractive Optical Components FIGURE 2 Operating regimes of transmissive diffraction gratings: (a) multiwave regime, (b) two-wave regime, and (c) zero-order regime. The propagation angle of each diffracted wave may be obtained from the grating equation given by n P sin θP,i = n C sin θin − i λ0 / (1) where λ0 is the free-space wavelength, i is an integer, and P is either C or S depending on the region under consideration.
1999). “Electron Holography,” Springer-Verlag, Berlin. Tsuno, K. (1997). Magnetic Lenses for Electron Microscopy. In “Handbook of Charged Particle Optics” (J. ), pp. 143–175, CRC Press, Boca Raton, FL. Wollnik, H. (1987). “Optics of Charged Particles,” Academic Press, Orlando. P1: GPJ/GLQ P2: FJU Final Pages Qu: 00, 00, 00, 00 Encyclopedia of Physical Science and Technology EN004I-174 June 8, 2001 17:22 Diffractive Optical Components R. Magnusson University of Connecticut D. Shin University of Texas at Arlington I.
19 was used to realize a GMR laser mirror. The flat output mirror of the dye laser with broadband output (800–920 nm) was replaced with the GMR filter and the birefringent tuning element removed. Lasing occurred at a wavelength of ∼860 nm. The laser power was ∼100 mW when pumped with an Ar+ laser emitting a power of ∼5 W at a 514-nm wavelength. 3 nm. This linewidth was set by the GMR filter linewidth at the threshold reflectance for laser oscillation to occur; in this case at ∼95% reflectance value in Fig.