Investigation of a power combiner made of two FET oscillators for an active array are reported. As an approach by a quasi-optical method, a two-dimensional planar array of strongly coupled oscillators by direct connection through a microstrip line is used. In-phase condition between the oscillators as well as in-phase condition of each radiation wave was accomplished by regulating length of feed microstrip lines. The radiation elements of 1 lambda-slot are embedded in a circuit ground plane. At an operation frequency of 20 GHz, in both H- and E-planes, reasonable sigma radiation patterns were obtained which have good agreement with theoretical patterns

Itoh, Tatsuo

Kawasaki, Shigeo

English

NASA Technical Reports Server

Third International Symposium on Space Terahertz Technology Page 37
2x2 QUASI-OPTICAL
POWER COMBINER ARRAY
AT 20 GHz N9 3 -
Shigeo Kawasaki and Tatsuo Itoh
Department of Electrical Engineering
University of California
Los Angeles, CA 90024
ABSTRACT
Investigation of a power combiner made of two FET oscillators for an active array
are reported. As an approach by a quasi-optical method, a two-dimensional planar array of
strongly coupled oscillators by direct connection through a microstrip line is used. In-
phase condition between the oscillators as well as in-phase condition of each radiation wave
was accomplished by regulating length of feed microstrip lines. The radiation elements of
lX,-slot are embedded in a circuit ground plane. At an operation frequency of 20 GHz, in
both H- and E-planes, reasonable Z radiation patterns were obtained which have good
agreement with theoretical patterns.
INTRODUCTION
Quasi-optical circuits have been of growing interest for compact and simple
microwave and millimeter-wave systems. Among many solid-state devices, FETs are
preferred as an active source for applications based on the MMIC technologyfl].
However, due to low efficiency, individual FET has limited capability of the power
generation at higher operating frequencies. Therefore, a power combining technique is
https://ntrs.nasa.gov/search.jsp?R=19930018541 2020-03-17T05:46:04+00:00Z
Page 38 Third International Symposium on Space Terahertz Technology
essential for high power and high frequency systems. Further, the need for such systems
has resulted in a variety of power combining configuration using FETs.
As one of such power combiners, the planar grid oscillator using MESFETs has
been developed in a distributed fashion[2]. Also, the weakly coupling oscillator array in a
periodic fashion supported by a reflector element has been reported[3]. Recently, using
external injection locking, the power combiner array with feedback FET oscillators was
made[4]. However, due to a multimoding problem, the power combiner array with strong
coupling has not made great progress to date. Regarding linear spatial power combiner
arrays with strong coupling, we have already reported a few results obtained under the
stratified structure[5],[6]. Through these results, in-phase operation for high combining
efficiency was facilitated.
In this paper, we describe design and experimental results of a quasi-optical spatial
power combiner array made of two negative resistance HEMT oscillators and 4 slots.
Radiation patterns from the slots aligned as 2x2 were compared with theoretical patterns in
both H-plane and E-plane. Further, through these patterns, it was confirmed that the
radiation waves from each slots were in-phase.
DESIGN
In order to demonstrate topology for the MMIC technology, the circuit was made in
a layered structure by adopting slot radiators in a circuit ground plane. Fig. 1 shows the
configuration of 2x2 spatial power combiner array designed at 20 GHz. The circuit
structure made of two negative resistance oscillators and feed lines is etched on the top side
of the substrate, while the slot radiators shown by cross-hatched sections in Fig. 1 are
embedded in the ground plane of the bottom side of the same substrate. Each oscillator
was designed with -50 Q for an input impedance. Since both sides of the substrate can be
effectively used, the slot radiators in the circuit ground plane increase design flexibility.
Third International Symposium on Space Terahertz Technology Page 39
RF energy generated from one FET oscillator is divided and delivered to two slots
aligned in the E-plane. In addition, a part of this energy is used to lock the other oscillator
through a direct coupling between the two oscillators. The locked and amplified signal
flows into another two slots aligned in the E-plane as well. Each pair of the slots aligned in
the E-plane are connected in series. Therefore, this 2x2 array consists of two slots aligned
in the E-plane and two slots aligned in the H-plane with IX separation between the centers
of two slots. The direct connection of two slots in H-plane separated by a thin line
enhances high packaging density.
D
FET
Slot Radiator
(Bottom Side)
«- X/4
Transition
Transformer
/ 2 Z o
FET • 0
Fig. 1 Circuit Configuration
Page 40 Third International Symposium on Space Terahertz Technology
According to the previous results about the direct connection of oscillators[6], when
the distance between two branch-points from the oscillators (shown as A and B in Fig. 1)
is an odd number of half wavelength, the radiation waves from the two branching points A
and B are in-phase. Since the length of a straight line between A and B is IX, a microstrip
line with X/2 should be added. As a result, the radiation waves from the slots in H-plane
can have the same phase.
The distance between two centers of slots is IX. Thus, the divided energy from
one branching point A or B can reach the centers of both slots at the same time. This
results in an anti-phase radiation. For the in-phase condition, one of these pass must have
additional X/2 to invert the phase on one of the slots. By means of this control of pass
length between an oscillator and a slot as well as between two oscillators, the in-phase
condition was obtained in both H-plane and E-plane.
In addition to the consideration of phase condition, input matching condition needs
to be taken into account. A one-stage X/4 transformer is inserted from a center of a slot
toward a branched feed line connected to the branch-point A or B. In order to
electromagnetically couple a feed line with a slot radiator, a X/4 microstrip-to-slotline is
adopted.
On the other hand, the slot radiators were also designed at 20 GHz with a IX slot
length and a 0.08 IX slot width. Since input impedance of the center feed IX slot radiator
provides the circuit with 50 Q load, the slot and the 50 Q feed line are matched in the
steady state oscillation condition.
EXPERIMENTAL RESULTS
The circuit were fabricated on 31 mil thick substrate with £,-=2.33, using NEC
NE32484 package HJFETs. The negative resistance FET oscillator was optimized at 21
GHz with 5 % margin by using small signal S parameters so that the actual circuit can also
Third International Symposium on Space Terahertz Technology Page 41
be operated at 20 GHz. The maximum operation frequency of 19.5 GHz was observed
from the fabricated circuit as shown in Fig. 2.
It is found that, in this two-
device power combiner case,
a frequency margin of 7.7 %
is required under the design
condition of -50 Q, for an
input impedance, in reference
[1], we investigated the
frequency margin of a single
quasi-optical oscillator with a
single slot using the same
v
NE32484. In this case, the
frequency margin of 4.4 % pjg> 2 Operation SpCGtrum
was obtained.
Compared with this previous results, the difference between the operation frequency and
the design frequency is increased. This implies that, in the case of a large number of FET
combiners, accumulation of a difference of input impedances due to such frequency
difference becomes a cause of load pulling, and, due to this phenomenon, the frequency
difference is increasingly enhanced. The tuning range obtained by changing the applied DC
voltages, Vds (2.6-5.0 V) and Vgs (-1.0—1.6 V), was 121 MHz.
Radiation patterns in both the H-plane and the E-plane are shown in Fig. 3. In both
cases, it is easy to find out null points around ±30° which result from array factor. For
comparison, the theoretical analysis was carried out by using the point matching method to
obtain numerical data from the Pocklington type integral equation. In the calculation, the
voltage ratio of two source generators to excite each slot was set to 1, while the phase
difference of these generators was set to 0. Using these data, theoretical radiation patterns
Page 42 Third International Symposium on Space Terahertz Technology
m
I OH
o
Q.
0)
*• -10-(0
0)
CC
-20
experiment
theory
- 1 0 0 0
Angle (degree) 100
Experiment
(2x2 H-plane)
Vds=4.0 V
lds=45 mA
Vgs=-1.81 V
fo=19.14 GHz
Theory
Pockilngton I.E.
Voltage Ratio=1.0
Phase Difference=0
Comparision in Radiation Pattern (H Plane)
m
0>
5
o
QL
0)
JS
o>
OC
10-
01
-10-
-20
experiment
theory
-100 100
Angle (degree)
Experiment
(2x2 E-plane)
Vds=4.0 V
lds=40 mA
Vgs=-1.82 V
fO=19.15 Ghz
Theory
Pocklington I.E.
Voltage Ratio=1.0
Phase Difference=0
Comparision in Radiation Pattern (E plane)
Fig. 3 Radiation Patterns
Third International Symposium on Space Terahertz Technology Page 43
are obtained as shown in Fig.3 for both the H-plane and the E-plane. Agreement around
the main beams is good.
Sidelobes in the E-plane becomes lager than those in the H-plane because of a
single element factor. This fact is shown in the theoretical patterns in Fig. 3. However, the
sidelobes obtained from the experiment were still large in both H-plane and E-plane. These
discrepancies may result from the inadequate experimental setup.
CONCLUSIONS
Design and experimental results of a 2x2 quasi-optical spatial power combiner was
reported as a prototype of two dimensional quasi-optical power combiner array. Although
the impedance matching conditions as well as the in-phase condition have been taken into
account carefully, the difference of the operation frequency (19.2-19.5 GHz) to the design
frequency (20 GHz) has increased. In the case of a large array, more attention should be
paid to avoid increase of this frequency difference resulting in phenomena such as load
pulling.
In both the H-plane and the E-plane of a 2x2 quasi-optical power combiner array, £
radiation patterns were obtained by controlling the lengths of feed lines. Good agreement
between the experiment and the theory was obtained about mainlobes in both radiation
patterns.
It is believed that,through this prototype circuit, the fundamental data for a
monolithic quasi-optical power combiner array were obtained.
ACKNOWLEDGEMENT
This work was supported by US Army Research Office under contract DAAL 03-
88-K-0005.
Page 44 Third International Symposium on Space Terahertz Technology
REFERENCES
[1] S. Kawasaki and T. Itoh, "24 GHz FET Oscillator with Slot Antenna for Quasi-Optical
Transmitter", 16th In't Conf. on IR & MMW, Switzerland, Aug. 1991, pp 286-287
[2] Z.B. Popovic, R.M. Weikle II, M. Kim and D.B. Rutledge, "A 100-MESFET Planar
Grid Oscillator", IEEE Trans. Microwave Theory Tech., vol. 39, pp 193-200, Feb.
1991
[3] R.A. York and R.C. Compton, "Quasi-Optical Power Combining Using Mutually
Synchronized Oscillator Arrays", IEEE Trans. Microwave Theory Tech., vol. 39, pp
1000-1009, June 1991
[4] J. Birkeland and T. Itoh,"Two-Port FET Oscillators with Applications to Active
Arrays", IEEE Microwave and Guided Wave Lett., vol.1, ppl!2-113, May 1991
[5] S. Kawasaki and T. Itoh, "40 GHz Quasi-Optical Second Harmonic Spatial Power
Combiner Using FETs and Slots", to be published in 1992 IEEE MTT-S Int'l
Microwave Symposium, Albuquerque, NM.
[6] S. Kawasaki and T. Itoh, "6-Element Periodic and Nonperiodic Linear Arrays for
Quasi-Optical Spatial Power Combiner", to be published in URSI Radio Science
Meeting, Chicago IL, July 1992


The 2x2 quasi-optical power combiner array at 20 GHz

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