“…Let us consider the typical two-tone test (see Fig.1a), in which a non-linear RF device is driven by a signal x(t) composed of two equal-magnitude tones at different, but very close, frequencies, in the form, (1) where A is the amplitude of each test tone, and ω b is the frequency difference between them. Assuming, as it is the case in most situations, a third-order non-linear model for the RF block, the response y(t) of the system can be written as, (2) Expanding (2), and discarding the out-of-band components, the response y(t) can be expressed as [16], (3) In reference [15] we propose the analysis of the response envelope taking advantage of its frequency properties.…”