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Figure 14 shows the storage density, expressed in bits per square inch, versus the available n of the first class of materials for a family of required η. 3, an FT lens with F = 2, R = S = 35◦ , and there is a reference beam swing angle of ±35◦ at the medium plane. 1 (see the subsection entitled “Interpage Cross-talk Noise” and Fig. 10 for the rationale behind this choice). The SLM has 512 × 512 pixels. , Bragg selectivity). One sees from this particular example that the storage 16 HOLOGRAPHIC STORAGE Fig.

Barbastathis M. Levene D. Psaltis Shift multiplexing with spherical reference waves, Appl. , 35: 2403–2417, 1996. 24. V. N. Morozov Theory of holograms formed using a coded reference beam, Sov. J. Quantum. , 7: 961–964, 1977. 25. A. A. Vasil’ev S. P. Kotova V. N. Morozov Pseudorandom signals as key words in an associative holographic memory, Sov. J. Quantum. , 9: 1440–1441, 1979. 26. C. Denz et al. Volume hologram multiplexing using deterministic phase encoding method, Opt. , 85: 171–176, 1991.

For α = 2 (2π-criteria), p0 < 1, and therefore the first term in Eq. (24) does not contribute. 083 or SNRpe ≥ 12. Because Eq. (27) gives the worst-case estimate, we provide in Fig. 10 a direct numerical simulation of cross-talk using Eq. (25). 06 at the edge of the left side. 44 with this particular example. 1, as can be seen from Fig. 10. ” Detector Noise. The CCD noise consists of several sources of Johnson thermal noises at the sense node and at the preamps. These noises are lumped together to provide the rms noise electrons QCCDN .

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26.Image Processing by John G. Webster (Editor)

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