Chapter 3
CMOS THz Model i n g
3.1 Introduction
Accurate device models that can take into account the loss from strong
frequency-dependent dispersion and non-quasi-static effects must be c onsid-
ered in CMOS-based THz design. As the most fundamental passive structure,
the accurate modeling of transmission line (T-line) is very important in various
designs [96, 97]. T-line is traditionally char acterized by distributed integer-
order RLGC model as shown in Fig. 3.1(a) [98]. Drude’s classical rela xation-
effect model is deployed for the skin effect w ith R
S
[99, 100]. In addition, the
loss due to diele ctric polarization and dipole rotation can be modeled by a
dielectric-loss of G
D
. However, such an integer-order model is insufficient to
describe the T-line performance a t THz region because the loss term in T-
line is difficult to model the dispersion loss and non-quasi-static effects [101],
which can c ause large deviation at THz freq ue nc y region. Such impact is fur-
ther verified by the measurement r esults and circuit level simulations in this
paper. Moreover, the traditio nal T-line model has a causality issue. Physically,
the real and imaginary parts of both permittivity ε(ω) and permeability µ(ω)
in a propagation medium are not independent of each other, but follow the
Kramers–Kronig relation [102]. As such, the extracted RLC G parameters in
the traditional T-line model may result in a non-causal response in the model
that can induce both accuracy and convergence pr oblems in the time-domain
simulation.
The concept o f fractiona l-order model has been examined to model ca-
pacitor (C) and inductor (L) at high frequenc y region. The I-V relation of a
capacitor is found to follow the fractional-order [103], and the eddy current
and hysteresis effect in inductors are also observed with fractional-order re-
lation [104]. It motivates us to re-examine the RLCG T-line model at THz
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