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The method through which a picture is shaped, processed, and displayed should be conceptualized as a series of actual occasions referred to as the imaging chain. via mathematically modeling the imaging chain, we will achieve perception into the connection among the digital camera layout parameters and the ensuing photograph caliber.
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The ongoing development and aid in bills linked to fiber optic expertise linked to fiber sensors enable software components that have been formerly inaccessible. those traits are anticipated to proceed as new innovations turn into to be had and older ones are effectively tailored to new purposes.
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1975). Radio Phys. Quantum Electron. 18, 204-211. Gol'denberg, A. , Pankratova, T. , and Petelin, M. I. (1972). Soviet Patent 226044, priority July 16, 1967, granted 1972. Granatstein, V. L. (1977). Private communication. Granatstein, V. , and Godlove, T. F. (1978). Memorandum Report No. C. Hirshfield, J. , and Granatstein, V. L. (1977). IEEE Trans. Microwave Theory Tech. MTT-25, 522-527. Hirshfield, J. , Bernstein, I. , and Wachtel, J. M. (1965). IEEE J. Quantum Electron. QE-1, 237-245. Jory, H.
And Shestakovich, V. P. (1974). Radiotekh. Elektron. 19(5), 1046-1056 [Engl. : Radio Eng. Electron. Phys. 19, 96-103]. Manheimer, W. , and Granatstein, V. L. (1977). Memorandum Report No. C. Moiseev, M. , and Nusinovich, G. S. (1974). Radio Phys. Quantum Electron. 17, 1305-1311. 54 J. L. HIRSHFIELD Moiseyev, M. , Rogacheva, G. , and Yulpatov, V. K. (1968). All-Union Scientific Session in honor of Radio Day. Annotations and summaries of papers, Izd. NTORES im A. S. Popova, Moscow, p. 6. Nikolayev, L.
The phase-angle averaged equations of motion were analyzed numerically for weakly relativistic electrons. Each electron beam layer of half-wave width was simulated by eight infinitessimal charge layers, each of which was represented by a sequence of sixteen groups of electrons uniformly distributed over one period of phase in the initial reference plane. This gave a coupled set of 2 x 8 x 16 = 256 difference equations for the quasi-particle amplitudes and phase. Critical parameters were the normalized electron transit time through the interaction zone T = αωί, the initial fre quency detuning parameter σ = (ω — «Ω)/αω, and the field parameter v" 1 = <χ(2ω/ηΩβΙ\ where n = 1, 2, 3 , .