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IEEE TRANSACTIONS ON MICROWAVE THEORY AND TECHNIQUES 1
Model Order Reduction of Nonlinear Transmission
Lines Using Interpolatory Proper
Orthogonal Decomposition
Behzad Nouri , Member, IEEE, and Michel S. Nakhla , Life Fellow, IEEE
Abstract—A new method is presented for simulation of
nonlinear transmission line circuits based on proper orthogonal
decomposition reduction techniques coupled with an efficient
interpolatory algorithm. Evaluation of the nonlinear function and
corresponding Jacobian is performed in the reduced domain.
A key criterion is developed for a priori determination of the
dimension of the interpolation space leading to a substantial
reduction in the computational cost. The proposed algorithm is
applicable to general nonlinear circuits and does not impose any
constraints on the topology of the pertinent circuit or type of the
nonlinear components.
Index Terms— Interpolation space, model order reduc-
tion (MOR), nonlinear transmission line (NLTL), orthogonal
basis, proper orthogonal decomposition (POD), singular-value
decomposition (SVD).
I. I NTRODUCTION
W
ITH the rapid advances in both optical and millimeter-
wave semiconductor devices and systems, the demand
for incorporation of nonlinear transmission lines (NLTLs) in
high-frequency designs is rapidly increasing [1]–[5]. NLTLs
have shown significant promise in the applications such as
high-power RF pulse generation [6], [7], large-bandwidth fre-
quency multipliers [2], electrical soliton oscillators [8]–[11],
picosecond pulse generators [12], low-power ultra-wideband
(UWB) impulse radio transmitters [13], [14], passive inter-
modulation of analog and digital signals [1], [15], pulse
shaping [16], and pulse compressor in both UWB and collision
avoidance radar systems [17].
However, simulation and optimization of circuits containing
NLTLs are a challenging task due to the large computational
complexity associated with the traditional high-frequency
large-signal transmission line models. On the other hand,
model order reduction (MOR) has proven to be an effective
tool in reducing the computational cost associated with large
Manuscript received May 2, 2018; revised August 18, 2018 and
October 26, 2018; accepted October 30, 2018. This work was supported
in part by the Natural Sciences and Engineering Research Council of
Canada (NSERC). This paper is an expanded version from the IEEE MTT-S
International Microwave Symposium (IMS2018), Philadelphia, PA, USA,
June 10–15, 2018. (Corresponding author: Behzad Nouri.)
The authors are with the Department of Electronics, Carleton Uni-
versity, Ottawa, ON K1S 5B6, Canada (e-mail: sbnouri@doe.carleton.ca;
msn@doe.carleton.ca).
Color versions of one or more of the figures in this paper are available
online at http://ieeexplore.ieee.org.
Digital Object Identifier 10.1109/TMTT.2018.2880759
linear and nonlinear circuits and enabling design tasks that
are not possible otherwise. MOR is based on developing
systematic algorithms for replacing complex models with
much simpler ones that still accurately capture the essential
features of the original large system. This is achieved by
projecting the equations describing the large system into
a lower dimensional subspace. Several methods have been
proposed in [18] and [19] for the reduction of nonlinear
circuits. Due to its reliability, proper orthogonal decomposition
(POD) [20]–[23] is the most suitable reduction method for
large strongly nonlinear circuit applications. While a straight-
forward implementation of the nonlinear reduction algorithms,
in general, and POD-Galerkin, in particular, often yields a very
low-order reduced model, the computational complexity for
the evaluation of the resulting reduced-order model (ROM)
is often the same as the complexity of the full (unreduced)
circuit. This major computational drawback is due to the fact
that the ROM still requires the evaluation of the unreduced
nonlinear function and its Jacobian in the original domain
instead of the reduced domain. This limitation can undermine
any advantage that could be gained from reducing the size of
the original model.
To avoid this computational drawback, the trajectory piece-
wise linear approach [24] was proposed based on the approxi-
mation of nonlinear dynamics using a weighted sum of a set of
linear models derived from the linearization of the nonlinear
circuit at several operating points. However, the accuracy and
efficiency of this approach are not consistently reliable particu-
larly for circuits with highly nonlinear functions which cannot
be approximated well using low-degree piecewise polynomi-
als. In order to achieve a sufficient accuracy, a large number
of linearization points and higher degree polynomials are gen-
erally required leading to increased computational cost [25].
This fact eventually renders the trajectory-piecewise-based
method intractable. Several alternative approaches have been
proposed to tackle the problem of reducing the complexity
of evaluating the nonlinear function and associated Jacobian.
The main variants of these approaches can be categorized
as gappy POD [26], [27], missing point estimation [28], [29],
the empirical interpolation method (EIM) [30] and its dis-
crete variant so-called as discrete EIM (DEIM) [31]. These
approaches are closely related in the sense that they all use
some selected set of spatial points (the subset of components of
the vector-valued nonlinear function that are to be computed).
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