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Flow of validating the de-embedding method. S= S11 S21 S12 S22 = −1 T21 T11 −1 T11 −1 T22 − T21 T11 T12 −1 −T11 T12 . (72) The as-measured T-matrix for Fig. 13(a) is Tmeas = TL TTL TR . In order to de-embed TTL from Tmeas , the THRU (Fig. 13(b)) is measured, and the result (Tthru = TL TR ) is transformed into the block-diagonal form S˜ thru . Since each of the resultant 2 × 2 diagonal blocks of S˜ thru is symmetric by assumption, the method in Section 3 can be applied to determine TL and TR . Then, the characteristics of the TLs are obtained by −1 .
S. G. Lee, (2005). “Ultra-Wideband CMOS low noise amplifier”, electronics letters, vol. -W. -S. Kang, P. -T. -G. Lee An (2005). “UltraWideband CMOS Low Noise Amplifier for 3–5-GHz UWB System”, IEEE Journal of Solid-States Circuits, Vol. 40, N° 2, pp544-547, March 2005 Willy M. C. Sansen, (2006). “Analog Design Essentials”, Springer, 2006, chap. 1  P. K. , (2008). “Emerging Technologies in Software Defined Receivers,” in Proc.
We now have to find the transformation matrices. As before, we assume throughout that the THRU is reciprocal and hence the associated S-matrix symmetric. A thru-only de-embedding method for on-wafer characterization of multiport networks So2o1before 25 Se2e1before Se2e1OS Se2e1TH So2o1OS So2o1TH Fig. 11. Even-mode (broken lines) and odd-mode (solid lines) transmission coefficients for a pair of transmission lines (Fig. , 2008). Our goal is to transform a 2n × 2n scattering matrix S into the following block-diagonal form: S˜ = Sm1 ..