IEEE TRANSACTIONS ON ADVANCED PACKAGING, VOL. 33,NO. 1,FEBRUARY 2010 285
The Impact of On-Wafer Calibration Method on the
Measured Results of Coplanar Waveguide Circuits
Qian Li and Kathleen L. Melde, Senior Member, IEEE
Abstract—This paper compares four commonly used on-wafer
calibration methods including multiline thru-reflect-line (TRL),
line-reflect-reflect-match, line-reflect-match, and short-open-load-
thru, for three diverse coplanar waveguide (CPW) circuits. The
magnitudes and phases of and of the CPW circuits
are compared to quantify how the specific calibration method
influences measured scattering parameters. Special care is taken
to ensure that the measured scattering parameters are normalized
to the same reference impedance and reference plane for accurate
comparison. The measured results are compared with full-wave
simulations to provide additional assessment of accuracy. A
method to de-embed the discontinuity of the CPW at the probe
tip and the CPW of the test structures is presented. The effect
of probe-to-device-under-test discontinuity is effectively modeled
by one- or two- section of shunt capacitor and series inductor.
The results show that the multiline TRL calibration method
provides the highest transmission coefficient repeatability on not
well-matched circuits and highest accuracy on the three circuits
in this paper up to 40 GHz.
Index Terms—Coplanar waveguide (CPW), high-frequency
packaging, on-wafer measurements.
I. INTRODUCTION
T
HE high-frequency performance of high-speed digital
and wireless circuits has attracted increased attention.
High-frequency modeling and simulation tools can be used to
rapidly develop new circuit structures, yet the models must
often be verified by comparison to broadband measurements.
On-wafer measurements of coplanar waveguide (CPW) struc-
tures are widely used since they can easily interface with
probe stations. This eliminates the need for connectorized test
structures. The important factors to consider include which
calibration method to use, how to fabricate the necessary
calibration artifacts, and the impact that the calibration method
may have on the measurement results. The increase in clock
speeds and the push to higher frequencies of operation mean
that many of the calibration approaches typically used at lower
frequencies must be reevaluated. The verification of accurate
high-frequency design and analysis tools mean that the mea-
sured results on the test structures must also be very accurate
Manuscript received September 26, 2008; revised May 13, 2009. First pub-
lished October 02, 2009; current version published February 26, 2010. This
work was supported by the Semiconductor Research Corporation (SRC) under
Task ID 1292.063. This work was recommended for publication by Associate
Editor J. Tan upon evaluation of the reviewers comments.
The authors are with the Department of Electrical and Computer Engineering,
University of Arizona, Tucson, AZ 85721 USA (e-mail: melde@ece.arizona.
edu).
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/TADVP.2009.2025365
at increasingly higher frequencies. In this paper, we compare
the differences in the results and the implementation of some
commonly-used calibration methods. We assess the repeata-
bility and compare the results of the measurements of several
different types of CPW circuits to full-wave simulations.
The calibrations are based on different error models and
may have significant effects on the measurement accuracy
and repeatability. Multiline thru-reflect-line TRL (ML-TRL),
line-reflect-reflect-match (LRRM), line-reflect-match (LRM),
and short-open-load-thru (SOLT) are popular on-wafer calibra-
tion methods and are available in [1]. The ML-TRL calibration
artifacts and the device-under-test (DUT) typically reside on
the same substrate. This dramatically reduces errors due to
differences of the substrate materials or CPW dimensions
between the calibration standards and DUT. The standards
used for LRRM, LRM, and SOLT are realized on a commer-
cially-available impedance standard substrate (ISS). There may
be differences between the CPW dimensions and materials of
the ISS (for calibration) and the DUT (for measurement) that
affect the measurement results at high frequency [2].
Previously reported calibration comparison techniques pri-
marily focus on the error bound of the worst-case measure-
ments [2], [3]. Some other comparison techniques [4] are based
on measurements of different verification standards, such as
open-stubs and a straight line standard. This paper presents a
new approach that provides guidance and insight into the im-
pact of calibrations on measured results. The impact of the cal-
ibration method is applied to specific CPW circuit structures
used by design engineers. The investigation includes a diverse
set of CPW structures that include a straight transmission line,
a stepped impedance line, and a bandpass filter. These struc-
tures exhibit diverse responses, such as low reflection (for the
line), and a narrow filter response. In this paper, the average and
standard deviation of the measured -parameters are compared.
This paper compares the impact of the measured results ob-
tained from the different calibrations to full-wave simulations.
The simulations are used to provide another assessment of mea-
surement accuracy. The discussion is intended to be broad and
to relate to engineers who must compare measured results with
simulations. Some of the previous work on this subject have fo-
cused primarily on the measurements and relate to those gen-
erally familiar with the techniques and terminology. Before the
comparisons are conducted, all of the scattering parameters are
normalized so that the measured results are referenced to the
same port impedance and reference plane. This is an important
point to consider, since some calibrations approaches are refer-
enced to a 50 termination and some are not. An accurate com-
parison of accuracy and to simulated results requires that they all
be normalized to the same reference impedance and plane. The
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