. The Bell System technical journal . a>C, wC ^(^^) R,= 1 + (a)CR). COL; R2=Rs+Ri + KM Rs + R, Fig. 13 — Point contact rectifier and equivalent circuits. * W. Shockley, Electrons and Holes in Semiconductors, New York: D. VanNostrand Co., Inc., 1950, p. 284. WAFER TYPE MILLIMETER WAVE RECTIFIERS 1399 itf Rs, assuming a circular contact area, may be calculated from the for-mula, Rs = p/4ri .* For the above example, Rs = 18 ohms. Barrier Resistance The approximate operating value of the barrier resistance, /?, may bedetermined from a knowledge of the intermediate frequency impedanceof a typica


. The Bell System technical journal . a>C, wC ^(^^) R,= 1 + (a)CR). COL; R2=Rs+Ri + KM Rs + R, Fig. 13 — Point contact rectifier and equivalent circuits. * W. Shockley, Electrons and Holes in Semiconductors, New York: D. VanNostrand Co., Inc., 1950, p. 284. WAFER TYPE MILLIMETER WAVE RECTIFIERS 1399 itf Rs, assuming a circular contact area, may be calculated from the for-mula, Rs = p/4ri .* For the above example, Rs = 18 ohms. Barrier Resistance The approximate operating value of the barrier resistance, /?, may bedetermined from a knowledge of the intermediate frequency impedanceof a typical rectifier. A. B. Cra^^^ord has sho-wn that the optimum inter-mediate frequency output impedance of a crystal mixer rectifier is afunction of the exponent of the static characteristic of the rectifier andthe impedance presented to the rectifier at the image and signal fre-quencies. This information is presented in Fig. in G. C. South-worths In the millimeter wave case it is a good assumption thatthe impedances for the signal and image frequencies ar


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Keywords: ., bookcentury1900, bookdecade1920, booksubjecttechnology, bookyear1