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given fm add, if their phases are random the PPSDs of the two oscillators add at any value of fm : S (fm ) = S 1 (fm ) + S 2 (fm ). (9.14) Thus the nal value phase noise spectrum will be the sum of the PPSDs of the incoming signal plus all of the LOs used in frequency conversion (plus possibly other phase noise discussed in this chapter). Eq. (9.14) represents the addition of two uncorrelated noise sources. In some cases a single noise source may arrive at a destination by more than one path so that the resulting deviations in phase are correlated. In such cases the deviations, not their variances, must be added (allowing the possibility of cancellation). A transfer function must be written for phase modulation from source to destination. S is then determined by multiplying S at its source by the squared magnitude of that transfer function. The resulting S can then be added to other randomly related components according to Eq. (9.14). For example, two frequency synthesizers, each using the same frequency reference, may generate a rst and second LO. The transfer function for phase deviations from the reference to some point after the second mixer will include the effects of the paths through the two synthesizers, including delays, frequency (phase) multiplications, and possibly the ltering effects of PLLs. Low-frequency phase deviations processed through these two paths may add or subtract, depending on the frequency conversion plan. Since phase undergoes the same processing as frequency, their transfer function will match the frequency conversion plan at zero modulation frequency, but not generally at high modulation frequencies. Other examples of coherent addition of noise can be seen in Section 9.5.3 below and in Egan, 1998, pages 329 331. itextsharp compare pdf c# How to get a table in pdf file by using PDFSHARP. - C# Corner
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