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High power RF generation with optically activated bulk GaAs devices |
| H843 |
High power RF generation with optically activated bulk GaAs devices
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| Patent Drawings: | |
| Inventor: |
Kim, et al. |
| Date Issued: |
November 6, 1990 |
| Application: |
07/374,105 |
| Filed: |
May 26, 1989 |
| Inventors: |
Bovino; Lawrence J. (Eatontown, NJ)
Kim; Anderson H. (Eatontown, NJ)
Weiner; Maurice (Ocean, NJ)
Youmans; Robert J. (Point Pleasant, NJ)
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| Assignee: |
The United States of America as represented by the Secretary of the Army (Washington, DC) |
| Primary Examiner: |
Tarcza; Thomas H. |
| Assistant Examiner: |
Wallace; Linda J. |
| Attorney Or Agent: |
Zelenka; Michael J.Knab; Ann M. |
| U.S. Class: |
250/214.1; 363/117 |
| Field Of Search: |
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| International Class: |
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| U.S Patent Documents: |
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| Foreign Patent Documents: |
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| Other References: |
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| Abstract: |
Utilizing sections of charged transmission line cables and optically-actied semiconductor switches, the direct generation of high power RF is demonstrated. |
| Claim: |
What is claimed is:
1. An optically-activated RF generator for producing high power RF pulse energy from applied DC energy comprising:
a transmission line having an output end, an open-terminated input end and a series of transmission line sections serially disposed between said input end and said output end, each of said transmission line sections having a signal transmittingconductor which is electrically isolated from the signal transmitting conductors of the adjoining transmission line sections in said series of sections and a signal return conductor which is electrically interconnected with the signal return conductorsof the adjoining transmission lines sections in said series of sections;
a DC power supply means coupled to the signal transmitting conductors of said series of transmission line sections for charging each of said signal transmitting conductors with DC voltage potential standing waves having a magnitude commensuratewith the magnitude of the RF pulse energy to be produced and polarities which are opposite to the polarities of the DC voltage potential standing waves to which the adjoining signal transmitting conductors in said series of transmission line sections arecharged;
a load;
a plurality of optically-activated GaAs normally-open switches, each of said switches having a block of GaAs and a pair of switch electrodes mounted on opposite faces of said block, at least one of said pair of switch electrodes having aplurality of light-transmitting apertures formed therein which permit light striking the electrode to reach the face of the block beneath the electrode;
a circuit means coupled to the switch electrodes of said plurality of GaAs switches for coupling one of said switches in series circuit with said load across the output end of said transmission line and for coupling each of the remainder of saidswitches in series circuit between the signal transmitting conductors of a different one of the pairs of adjoining transmission line sections in said transmission line;
a laser means for emitting pulses of light at a predetermined repetition rate, said light pulses being at a wavelength which will cause the blocks of GaAs in each of said plurality of switches to become electrically conductive; and
a fiber optic means coupled between said laser means and the light apertured electrodes of all of said plurality of GaAs switches for causing all of said switches to close and to thereby connect the signal transmitting conductor of saidtransmission line in series circuit with said load, whereby a RF pulse transmission of said DC voltage potential standing waves is transmitted to said load. |
| Description: |
TECHNICAL FIELD
This invention relates generally to radio frequency (RF) pulse
power generation and more particularly to apparatus for generating RF pulse power from direct current (DC) by means of GaAs direct Switches.
BACKGROUND OF THE INVENTION
The conversion of DC energy directly to RF pulses with efficiency has many potential applications. Among such uses are: high-power electrical pulses for pulsed power devices and plasma-physic experiments; high resolution radar and time domainmetrology; and the generation of megawatt level microwave and millimeter-wave pulses. These applications require the development of an appropriate switch or an array of switches which can switch high power with extremely fast rise time and zero jitter. A frozen wave generator has been developed, consisting of many segments of transmission line charged alternately with positive and negative voltage. Two adjacent segments are joined by a silicon switch which can be closed with a laser pulse. Thisconcept is described by Chang, et al., in "Direct DC to RF Conversion By Picosecond Optoelectronic Switching," IEEE MTT-S International Microwave Symposium Digest, May 1984 which is herein incorporated by reference. A great deal of effort has beendevoted to the investigation of photo-conductive semiconductor devices. Bulky microwave tubes and slow reset times have been associated with conventional RF generators. The present invention addresses these problems and more.
SUMMARY OF THE INVENTION
It is an object of the invention to produce an optically-activated RF generator with increased power output.
It is a further object of the invention to provide a RF generator having compact design which is capable of a fast rise time.
It is still a further object of the invention to produce a very cost effective RF generator.
The above and other objects are achieved in accordance with the invention wherein a transmission line is comprised of an output end, an open-terminated input end and a series of transmission line sections being serially disposed between the inputend and the output end. Each transmission line section has a signal transmitting conductor which is electrically isolated from the signal transmitting conductors of the adjoining transmission line sections in the series of sections and a signal returnconductor which is electrically interconnected with the signal return conductors of the adjoining transmission line sections in the series of sections. A DC power supply means is coupled to the signal transmitting conductors of the series oftransmission line sections for charging each of the signal transmitting conductors with DC voltage potential standing waves having a magnitude commensurate with the magnitude of the RF pulse energy to be produced and polarities which are opposite to thepolarities of the DC voltage potential standing waves to which the adjoining signal transmitting conductors in the series of transmission line sections are charged. A plurality of optically-activated GaAs normally-open switches which each have a blockof GaAs and a pair of switch electrodes mounted on opposite faces of the block are coupled in series with a load. At least one of pair of switch electrodes has a plurality of light-transmitting apertures formed therein which permit light striking theelectrode to reach the face of the block beneath the electrode. A circuit means is coupled to the switch electrodes of the plurality of GaAs switches for coupling one of the switches in series circuit with a load across the output end of thetransmission line and for coupling each of the remainder of switches in series circuit between the signal transmitting conductors of a different one of the pairs of adjoining transmission line sections in the transmission line. A fiber optic means iscoupled between a laser means and the light apertured electrodes of all of the plurality of GaAs switches. The laser means emits pulses of light at a predetermined repetition rate, the light pulses being at a wavelength which will cause the blocks ofGaAs in each of the plurality of switches to close and to thereby connect the signal transmitting conductor of the transmission line in series circuit with the load, whereby a RF pulse transmission of the DC voltage potential standing waves istransmitted to the load.
BRIEF DESCRIPTION OF THE DRAWINGS
FIG. 1 is a schematic diagram of a three-switch RF generator.
FIG. 2 displays a waveform from the RF generator.
FIG. 3 illustrates a gridded optically activated switch (OAS) device.
FIG. 4 is the graphic response of a laser light pulse leaving the fiber optic bundle.
FIG. 5 displays a switch current waveform.
FIG. 6 illustrates a RF waveform obtained by a current transformer.
DETAILED DESCRIPTION OF THE DRAWINGS
The RF generator consists of charged coaxial transmission lines (PFL) and gridded GaAs OAS devices. As shown in FIG. 1, the circuit has three segments of PFL's charged by positive and negative voltage Vo. Adjacent PFL's are connected with abulk GaAs OAS. Since semi-insulating GaAs has a high resistivity (>10.sup.7 ohm-cm), the leakage current is negligible. When all switches are fired simultaneously, the standing waves, which have amplitude Vo/2, start to move in the forward andbackward directions. The forward wave travels toward the output load and appears on the load resistor. The backward wave moves toward the open termination end, is totally reflected from the open termination end, and then moves back toward the outputload. The half period of the RF generated is the transit time for the standing wave to travel across the PFL of length L. The repetition frequency of the burst of RF is determined by the repetition rate of laser system. The predicted generation of theRF burst is given in FIG. 2.
In most high power bulk OAS devices the light is introduced perpendicular to the applied field direction. Although these devices showed very high power capability, multiple OAS operation required highly efficient devices as well. Recently,optically activated gridded silicon PIN diodes demonstrated high efficiency. Utilizing this concept, optically activated gridded bulk GaAs devices were designed and fabricated at ETDL. The typical bulk GaAs OAS is shown in FIG. 3. In these switchesthe light is introduced parallel to the applied field direction. The test results of these devices shows significant improvement of efficiency. With light from a 20 ns Q-switched Nd:YAG laser, emanating a fiber optic bundle, the switch turn-on wassustained for 150 ns without distortion. The FIG. 4 shows the laser light pulse waveform leaving the fiber optic bundle. FIG. 5 shows the resulting switch current waveform with a 200 ns PFL, biased at 2 KV. The OAS was turned on with laser energy assmall as 0.8 mJ. The current latch-on and low threshold laser energy is assumed due to field-introduced avalanche effect. On-state voltage was very small. The parametric relationship of applied voltage, optical energy, and output pulse width will bediscussed elsewhere.
It is necessary to supply each of the switches with sufficient laser energy. This was implemented with fiber optic bundles. The advantage of this technique is that each bundle may contain varying fiber lengths, thus effectively increasing thewidth of the light pulse and insuring the switch stays on, until all forward and backward waves pass through.
This is particularly critical for switch number 3, which must stay on the longest time In this experiment, however, it was unnecessary to use varying fiber lengths, since the OAS gridded device stayed on fairly long, up to 150 ns. In order toachieve wider burst pulse widths, however, the use of incremental fiber lengths may be expected to play a role.
Each switch was tested individually at 2 KV DC bias with 0.8 mJ light energy from a Q-switched Nd:YAG laser (20 ns pulse width). The coaxial cable lengths of the 3-stage generator were 9 feet, 9 feet, and 4.5 feet respectively, with ananticipated total pulsewidth of 67.5 ns. Since this width is less than the recovery time (150 ns) of the OAS, simultaneous triggering of the switches was employed, and thus equal lengths of fibers were used to convey the light to the switches. Atypical waveform, is shown in FIG. 6, obtained by a current transformer, the Tektronix CT-1.
The maximum current achieved was approximately 12 amps, with a pulsewidth of about 100 ns, instead of the anticipated values of 20 amps and 67.5 ns. The longer pulsewidth, as well as the lower current amplitude, are caused primarily byinductance in the connections between OAS devices. This inductance will be eliminated by incorporating the switch into the transmission line. Narrower light pulses also will be used to minimize the effect of the risetime of the light signal. Unequaldistribution of the light among the various switches must also be addressed.
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