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Parametric Amplifiers by J. C. Decroly

By J. C. Decroly

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42) The summation in (lAI) is limited to the harmonics of frequency between (ne - VI)w and (ne + Vl)W. 44) v, V, Txs(t) ", 2: v= L ranc + v sin vwt - v= - VI Tb nc + v cos vwt VI At a given instant t, the complex amplitudes of the useful signal and of the components of the parasitic signal, in phase or in quadrature with the useful signal, are as shown in Fig. 1. 1 Taking condition (b) into account (high signal-to-noise ratio), it follows from Fig. 47) where 2B is the bandwidth of the LF filter (va::;; VI).

143), this noise is calculated at the amplifier input, but this time with the intervention of the transducer gain G, which is expressed by a temperature Top, called the operational temperature of the system. 175) to which it is equivalent when GlN = G. 174) shows that the use oflow-noise amplifiers, that is those with a low value of T eff , is justified only if Tl is at the very most of the same order of magnitude as T err . On the other hand, when GlN #- G, the value of Tl is the determining factor in the choice of the parameters of the amplifier so as to cause the value of Top to be aminimum.

112) This formula will now be applied to the determination of the equivalent spectral noise temperature of the generator obtained if we place an attenuator at a temperature T (Fig. 114) we obtain: T eq = IZ24R+ RZol2 G(T I 2 o IZ 2 + Zol2 [GT I 4R 2 R o + T eff ) + (!!.. 4. Noise factor and effective noise temperature of a chain consisting of several two-ports Let us consider a chain composed of two two-ports QI and Q2 connected in cascade (Fig. 9). 120) It follows that the normalized noise factor (nI chain Ql' Q2 is given by = 4kT oR 1) of the I ~B GalG2GOn~ d!

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