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Solid State Electronics
journal homepage: www.elsevier.com/locate/sse
Near-field scanning microwave microscope platform based on a coaxial
cavity resonator for the characterization of semiconductor structures
Bendehiba Abadlia Bagdad, Carmen Lozano, Francisco Gamiz
⁎
Nanoelectronics Research Group, CITIC, University of Granada, 18071 Granada, Spain
ARTICLE INFO
Keywords:
Near-field scanning microwave microscopy
(NSMM)
Coaxial cavity resonators
Non-destructive characterization
Thin film semiconductor structures
ABSTRACT
A Near-Field Scanning Microwave Microscope (NSMM) for the characterization of semiconductor structures has
been designed, simulated and fabricated. The present NSMM system is based on a home-made coaxial-cavity
resonator which is fed by a Keysight N5242A PNA-X Network Analyzer. The inner conductor of the coaxial
resonator is connected to a sharpened tungsten tip, which was fabricated by an electrochemical process. The
reflection and transmission coefficients S
11
,S
21
, the resonance frequency f
r
and the quality factor Q of the
resonant cavity are measured as the semiconductor structure is scanned by the sharpened probe tip while the
sample-tip distance is kept constant in the near-field region. The interaction between the probe tip and the
sample under test provides variations of these parameters which are related to the topographical and dielectric
properties of a very small region of the material under the probe tip. Thus, a 2D image of the evolution of the S
11
,
S
21
,f
r
and Q parameters on the surface of the device under test is obtained. This image can be related to space
changes in the topography, dielectric properties and composition of the semiconductor structure.
1. Introduction
Near-field scanning microwave microscopy (NSMM) is a technique
used for the non-destructive characterization of materials at microwave
frequency range. An NSMM system consists of a sharpened metallic tip,
mounted on the center conductor of a high-quality coaxial resonator.
The coaxial resonator is fed by a microwave signal supplied by a Vector
Network Analyzer (VNA). The transmission coefficient S
21,
(resp. re-
flection coefficient, S
11
) of the cavity, measured by the VNA, shows a
characteristic transmission maximum (resp. reflection minimum) at the
resonant frequency, f
r0
, for which it was designed, and a particular
quality factor, Q
0
, which also depends on the geometry of the cavity.
When the probe tip is placed close enough (in the near field region) to
the device under test (DUT), a shift in the resonant frequency f
r
and a
modification of the quality factor, Q, of the coaxial-cavity resonator are
produced depending on the impedance of the tip-sample interaction.
These changes are continuously measured by the VNA. The shift of the
resonant frequency depends on the distance between the tip and the
sample and the electromagnetic properties of the sample under test,
such as the conductivity, sheet resistance, or dielectric constant, and
their spatial variations [1–4]. If the distance between the tip and the
surface of the sample is kept constant, the shift in f
r
only depends on the
electromagnetic properties of a very small area (of the size of the tip
dimensions) of the DUT near the probe tip. The sample is then scanned
by the tip of the cavity while the distance between tip-sample is kept
constant and the resonant frequency of the cavity is continuously
measured by the VNA. The 2D representation of the resonant frequency,
f
r
, quality factor Q, and magnitude of the transmission |S
21
| and re-
flection |S
11
| coefficients of the coaxial-cavity resonator provides a map
of the electromagnetic properties of the sample under test. Therefore,
the high spatial resolution of the NSMM technique allows us to non-
destructively characterize semiconductor structures with high sensi-
tivity and with nanoscale resolution without damaging them [5,6].
Thus, we can evaluate, for example, the quality of the interfaces, layer
thickness variations, doping and concentrations, etc. [7].
Fig. 1 shows the scheme of the NSMM structure with the main parts
of the system, such as the VNA that continuously feeds a coaxial-cavity
resonator with a conductive tip connected at the end of its inner con-
ductor.
The designed coaxial-cavity resonator provides a very high-quality
factor and its potential to characterize metallic materials has been al-
ready demonstrated by several groups [7,8]. In this paper, the design,
simulation and set up of a NSMM platform based on a coaxial-cavity
resonator have been carried out. Then, the transmission and reflection
coefficients S
21
,S
11
of the resonant cavity is continuously measured and
monitored by a vector network analyzer, while a sharpened tungsten tip
https://doi.org/10.1016/j.sse.2019.03.052
⁎
Corresponding author.
E-mail address: fgamiz@ugr.es (F. Gamiz).
Solid State Electronics xxx (xxxx) xxx–xxx
0038-1101/ © 2019 Elsevier Ltd. All rights reserved.
Please cite this article as: Bendehiba Abadlia Bagdad, Carmen Lozano and Francisco Gamiz, Solid State Electronics,
https://doi.org/10.1016/j.sse.2019.03.052