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Fig. 15

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Shifting the input spectral densities with  ± ΔνLO =  ± 10   MHz and multiplying by the (IF) bandpass shape (see Fig. 2) returns the “measured” spectra Psig,ref. The upper panel shows the results for the simpler case, while the lower panel includes a standing wave contribution (νsw = 50   MHz). Note that for the method described in Sect. 4.4 we used a smaller standing wave frequency (νsw = νLO = 10   MHz) in contrast to the other examples in order to avoid resonances (see also Sect. 4.4.1).

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