Information
-
Patent Grant
-
6259337
-
Patent Number
6,259,337
-
Date Filed
Thursday, August 19, 199925 years ago
-
Date Issued
Tuesday, July 10, 200123 years ago
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Inventors
-
Original Assignees
-
Examiners
- Lee; Benny
- Glenn; Kimberly E
Agents
- Alkov; Leonard A.
- Lenzen, Jr.; Glenn H.
-
CPC
-
US Classifications
Field of Search
US
- 333 246
- 333 247
- 333 128
- 333 33
- 330 286
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International Classifications
-
Abstract
A coplanar waveguide structure for use in constructing a monolithic microwave integrated circuit high power amplifier. The coplanar waveguide structure is a coplanar transmission line segment having more than two ground plane electrodes and a plurality of signal/dc current carrying electrodes. The current carrying electrodes are each separated from an adjacent ground plane electrode by a gap. The coplanar waveguide structure forms a shunt inductor for the monolithic microwave integrated circuit high power amplifier. The electrodes are shorted at one end to form the shunt inductor. A center ground plane electrode is preferably at least twice the width of the signal carrying electrode. The gaps between the signal carrying electrode and the ground electrodes are preferably at least one half the width of the signal carrying electrode to minimize current crowding.
Description
BACKGROUND
The present invention relates generally to high power amplifiers, and more particularly, to an improved coplanar waveguide structure that forms an improved inductor for use with monolithic microwave integrated circuit high power amplifiers.
Prior art relating to monolithic microwave integrated circuit (MMIC) high power amplifier output matching circuit designs includes the following. Certain prior art MMIC high power amplifiers use microstrip based circuitry. Circuit loss diminishes with wider microstrip line width. The loss of the output matching circuit is of the order of 0.5 dB for conventional X-band power MMIC amplifiers. Microstrip based circuitry is not compatible with flip-chip module assembly techniques.
Other prior art MMIC high power amplifiers use a coplanar waveguide with a very wide signal carrying strip to meet dc current carrying requirements. Current crowding of coplanar waveguide with large strip-to-gap ratio leads to a low Q factor, and higher circuit loss. Flip-chip amplifier efficiency suffers when such lower Q, critical resonant circuit elements are employed.
It would therefore be desirable to have a coplanar waveguide structure for use with monolithic microwave integrated circuit high power amplifiers that improves upon conventional designs.
SUMMARY OF THE INVENTION
The present invention provides for a coplanar waveguide structure for use with a monolithic microwave integrated circuit high power amplifier. The coplanar waveguide structure comprises a coplanar transmission line segment having more than two ground plane electrodes and a plurality of signal/dc current carrying electrodes. The current carrying electrodes are each separated from an adjacent ground plane electrode by a gap. The coplanar waveguide structure forms an improved inductor for the monolithic microwave integrated circuit high power amplifier. A center ground plane electrode is preferably at least twice the width of the signal carrying electrode. The gaps between the signal carrying electrode and the ground electrodes are preferably at least one half the width of the signal carrying electrode to minimize current crowding.
The present invention uses a high Q planar inductor that is compatible with flip-chip MMIC technology. The effective width of the signal carrying metal strip is able to handle the dc current required for operation of the high power amplifier without risking current metal migration.
The present invention makes use of closely spaced, parallel coplanar waveguide (CPW) segments shorted at one end to form a shunt inductor at the output of high power flip-chip, monolithic microwave integrated circuit (MMIC) amplifiers. As a part of the output matching circuitry, the shunt inductors are at resonance with the drain-source capacitance of output-transistors at the RF signal frequency. Because there is less current crowding at the edge of the conductors, the coplanar inductor configuration offers higher circuit Q-factor compared with conventional CPW inductors with an identical strip width and characteristic impedance. The reduction in output matching circuit loss is critical to high efficiency operation of very high power flip-chip MMIC amplifiers, such as those used in active array radar.
The present invention improves the power added efficiency (PAE) of flip-chip, high power MMIC amplifiers for active array antenna applications. The present invention provides higher monolithic microwave integrated circuit amplifier efficiency through lower circuit loss at the output impedance transformer section. The use of a higher Q-factor coplanar inductor at the drain electrode of the output transistors serves to reduce signal loss per cycle. The reduction in RF power loss at the output of a high power amplifier directly impacts the power added efficiency of circuit operation. Higher RF amplifier efficiency leads to lower prime power demand, power supply size reduction, improved thermal management and lower system manufacturing cost.
The present invention may be used in all field effect transistor (FET) amplifiers, including MESFET and high electron mobility transistors (HEMT) based high power monolithic microwave integrated circuit (MMIC) amplifiers. The present invention will have beneficial impact on MMIC based, active array radar systems, and communication systems, developed by the assignee of the present invention.
BRIEF DESCRIPTION OF THE DRAWINGS
The various features and advantages of the present invention may be more readily understood with reference to the following detailed description taken in conjunction with the accompanying drawings, wherein like reference numerals designate like structural elements, and in which:
FIG. 1
illustrates an equivalent circuit of a transistor amplifier output matching transformer with lossless reactive circuit elements;
FIG. 1
a
illustrates an alternative representation of the transistor amplifier output matching transformer of
FIG. 1
;
FIG. 2
illustrates an equivalent circuit of a transistor amplifier output matching transformer with realistic lossy circuit elements;
FIG. 3
illustrates a conventional coplanar waveguide for use in a MMIC high power amplifier; and
FIG. 4
illustrates an exemplary high Q-factor coplanar waveguide in accordance with the principles of the present invention for use in an improved MMIC high power amplifier.
DETAILED DESCRIPTION
High power, flip-chip MMIC technology promises significant cost savings for active array radar transceiver module manufacturing. This emerging technology has not yet reached full potential because of certain circuit performance concerns. Recently, a very high power (over 7 W), two-stage, flip-chip MMIC amplifier operating over nearly the entire X-band frequency range has been developed by the assignee of the present invention.
However, despite the high output power and broad bandwidth characteristics, flip-chip MMIC amplifiers seem to exhibit slightly lower power added efficiency (PAE), compared with their counterparts using a face up design. The present invention provides means to improve flip-chip MMIC power amplifier efficiency through RF signal loss reduction at the output matching circuitry.
Circuit loss at the output impedance transformer section of an RF amplifier dictates the maximum achievable power added efficiency. It is therefore critically important to reduce the matching circuit loss at the output of a MMIC amplifier to a minimum.
Referring to the drawing figures,
FIGS. 1 and 2
show equivalent circuits of a portion of a high power amplifier
10
comprising a typical field effect transistor (FET) or pseudomorphic high electron mobility transistor (pHEMT) based MMIC HPA output matching section
20
.
FIG. 1
shows the equivalent circuit of the output matching transformer section
20
of the amplifier
10
having lossless reactive circuit elements.
FIG. 2
shows the equivalent circuit of the output matching transformer section of the amplifier
10
having realistic lossy circuit elements.
The transistor
11
is represented by a constant current source
11
, a shunt capacitor (Cds)
12
and a drain inductance (Ld)
13
. A first section of an RF impedance transformation network
14
adjacent the output transistor
11
typically includes a shunt inductor
15
at resonance with the effective source drain capacitance
12
of the transistor
11
. A resistive load (R)
16
is approximately equal to the dc load line of the output transistor
11
.
Ohmic loss of transmission line segments
17
forming a part of the output transformer section
14
and the Q-factor of the shunt inductor
15
both contribute to amplifier power added efficiency degradation. The characteristic impedance of the transmission line segments
17
connecting the drain of the output transistor
11
to the RF load
16
is typically in the 40 ohm to 70 ohm range.
FIG. 1
a
illustrates an alternative representation of the transistor amplifier output matching transformer section
20
of
FIG. 1
wherein the shunt inductor
15
is provided by a transmission line segment
17
a
and a bypass capacitor
18
. A short (less than a quarter of a wavelength long at the RF signal frequency) transmission line segment
17
a
is terminated by a large by-pass capacitor
18
(RF short) at one end to form the shunt inductor
15
. It is typically formed using a wide metal strip to accommodate the dc bias current required to operate the output transistor
11
of the power amplifier
10
. The dc current density at the inductor
15
must remain below 4E
5
A/cm{circumflex over ( )}2 to prevent premature circuit failure caused by current induced metal migration.
In the case of conventional face-up MMIC amplifiers
10
with microstrip based circuitry, wider strip width leads to reduced current density and lower transmission line loss. Also, lower Q-factor (higher circuit loss) is exhibited by coplanar waveguide based flip-chip circuitry using a wide center strip especially if gaps between the center strip and ground planes are not expanded.
Current crowding at the edge of electrodes forming coplanar waveguide is the real culprit. The energy stored in the LC resonant circuit (comprising the shunt capacitor (Cds)
12
and drain inductance (Ld)
13
plus the external shunt inductor
15
spends half the time in the capacitor
12
and half the time in the inductors
13
,
15
. Increased shunt inductor loss, which can be expressed as a shunt resistor
21
(R
1
) shown in
FIG. 2
will divert some of the current from the transistor
11
(constant current source
11
) from the RF load
16
. A part of the RF current from the transistor
11
is consumed in the shunt resistor
21
(R
1
), resulting in amplifier power added efficient degradation.
FIG. 3
illustrates a conventional coplanar waveguide structure
30
over which the present invention provides an improvement. The conventional coplanar waveguide structure
30
forms an inductor
15
used in the output matching transformer section
20
of a conventional high power amplifier
10
. The conventional coplanar waveguide structure
30
comprises two outer ground plane electrodes
31
separated by gaps
32
from a single signal electrode
33
. Ground straps
34
are provided to bridge the two ground plane electrodes
31
.
FIG. 4
illustrates an exemplary high Q-factor coplanar waveguide structure
40
in accordance with the principles of the present invention that forms an improved inductor
15
used in the output matching transformer section
20
of a high power amplifier
10
. The coplanar waveguide structure
40
comprises a coplanar transmission line segment
41
having more than two ground plane electrodes
3
1
, and comprises more than one signal (and dc current) carrying electrode
33
. One or more signal straps
35
couple RF/dc signals between the respective signal carrying electrodes
33
.
FIG. 4
shows an example of such an inductor
15
with two signal carrying electrodes
33
. RF current is more evenly distributed because the transmission line segment
41
is actually two lines in parallel. The shunt inductor
15
in this novel configuration provides for an inductor
15
with higher Q, and lower loss. The end result is improved amplifier power added efficiency for a flip-chip MMIC high power amplifier employing the high Q-factor coplanar waveguide
40
.
It is desirable to have the sum of the widths of the two signal carrying electrodes
33
of the high Q-factor coplanar waveguide
40
shown in
FIG. 4
be equal to the width of the single signal carrying electrode
33
of the shunt inductor
15
of the conventional coplanar waveguide
30
shown in
FIG. 3. A
center ground plane electrode
31
is preferably at least twice the width of each of the two signal carrying electrodes
33
. Current crowding is minimized if the gaps
32
between the signal carrying electrodes
33
and the ground electrodes
31
are at least one half the width of the signal carrying electrodes
33
.
Thus, a coplanar waveguide structure for use with monolithic microwave integrated circuit high power amplifiers has been disclosed. It is to be understood that the above-described embodiment is merely illustrative of one of the many specific embodiments that represent applications of the principles of the present invention. Clearly, numerous and other arrangements can be readily devised by those skilled in the art without departing from the scope of the invention.
Claims
- 1. A coplanar waveguide structure for use with a high power amplifier, comprising:a coplanar transmission line segment having more than two ground plane electrodes and a plurality of signal/dc current carrying electrodes, which current carrying electrodes are each separated from an adjacent ground plane electrode by a gap, which coplanar waveguide structure forms a shunt inductor for the high power amplifier, wherein a center ground plane electrode is at least twice the width of the signal carrying electrode.
- 2. The coplanar waveguide structure recited in claim 1 wherein the coplanar waveguide segments are shorted at one end to form the shunt inductor.
- 3. The coplanar waveguide structure recited in claim 1 wherein the high power amplifier comprises a flip-chip, monolithic microwave integrated circuit amplifier.
- 4. A coplanar waveguide structure for use with a monolithic microwave integrated circuit high power amplifier, comprising:a coplanar transmission line segment having more than two ground plane electrodes and a plurality of signal/dc current carrying electrodes, which current carrying electrodes are each separated from an adjacent ground plane electrode by a gap, which electrodes are shorted at one end to form a shunt inductor for the monolithic microwave integrated circuit high power amplifier, wherein a center ground plane electrode is at least twice the width of the signal carrying electrode.
- 5. A coplanar waveguide structure for use with a monolithic microwave integrated circuit high power amplifier, comprising:a coplanar transmission line segment having more than two ground plane electrodes and a plurality of signal/dc current carrying electrodes, which current carrying electrodes are each separated from an adjacent ground plane electrode by a gap, which gaps are at least one half the width of the signal carrying electrodes, and wherein a center ground plane electrode is at least twice the width of the signal carrying electrodes, which coplanar waveguide structure forms a shunt inductor for the monolithic microwave integrated circuit high power amplifier.
- 6. A coplanar wavguide structure for use with a high power amplifier, comprising:a coplanar transmission line segment having more than two ground plane electrodes and a plurality of signal/dc current carrying electrodes, which current carrying electrodes are each separated form an adjacent ground plane electrode by a gap, which coplanar waveguide structure forms a shunt inductor for the high power amplifier, wherein the gaps between the signal carrying electrode and the ground electrodes are at least one half of the width of the signal carrying electrode to minimize current crowding.
- 7. The coplanar waveguide structure recited in claim 6 wherein the coplanar waveguide segments are shorted at one end to form the shunt inductor.
- 8. The coplanar waveguide structure recited in claim 6 wherein the high power amplifier comprises a flip-chip, monolithic microwave integrated circuit amplifier.
- 9. A coplanar waveguide structure for use with a monolithic microwave integrated circuit high power amplifier, comprising:a coplanar transmission line segment having more than two ground plane electrodes and a plurality of signal/dc current carrying electrodes, which current carrying electrodes are each separated from an adjacent ground plane electrode by a gap, which electrodes are shorted at one end to form a shunt inductor for the monolithic microwave integrated circuit high power amplifier, wherein the gaps between the signal carrying electrode and ground electrodes are at least one half the width of the signal carrying electrode to minimize current crowding.
US Referenced Citations (1)
Number |
Name |
Date |
Kind |
5528203 |
Mohwinkel et al. |
Jun 1996 |
|