Field of the Invention
The present invention relates to the field of microwave signal processing circuitry and, more particularly, to amplifier circuits which provide low-noise, small-signal amplification in the X-band, an oscillator circuits which include such amplifier circuits.
Background of the Invention
Military and commercial communication and radar systems have a critical need for reliable, low-noise, high-efficiency, solid-state amplifiers, particularly for use in oscillator circuitry.
The performance of a microwave feedback oscillator such as a dielectric resonator oscillator (DRO) or cavity oscillator is limited by the 1/f noise of the loop amplifiers. At low frequencies (below 4 GHz), bipolar junction transistor (BJT) amplifiers have generally been employed in the oscillator circuits because of their excellent noise characteristics. However, for higher frequencies (over 4 GHz), such as in the X-band, gallium arsenide field effect transistor (GaAs FET) amplifiers have been employed, although they have poorer noise characteristics than BJT amplifiers, because of the lack of a two-port BJT amplifier. A comparison of the respective phase noise characteristics of GaAs FET and BJT amplifiers is set forth in Montress et al., "Residual Phase Noise Measurements of VHF, LIHF and Microwave Components," Proceedings of the 43rd Annual Frequency Control Symposium, IEEE Catalog No. 89CH2690-6, June 1989.
Thus, the primary reason for the utilization of GaAs FET amplifiers in these oscillators instead of BJT amplifiers is that, to date, a two-port BJT amplifier has not been developed for operation at these higher frequencies. However, as may be readily appreciated by those skilled in the art, the incorporation of BJT amplifiers in oscillators operating at higher frequencies would greatly improve their performance. Since the close-in phase-noise performance of known two-port amplifiers and oscillators currently employed in the X-band is limited by the performance of the GaAs FETs, introduction of BJTs for these higher frequency applications would result in an improvement in the system noise floor.
Summary of the Invention
Accordingly, it is an object of the present invention to provide a low-phase-noise X-band amplifier.
A further object is to provide a two-port BJT amplifier which may be readily incorporated in a high frequency microwave feedback oscillator.
According to one aspect of the invention, an X-band (8-12 GHz) amplifier comprises a BJT arranged for receiving an X-band signal, amplifying the signal and providing the amplified signal to further circuitry.
Input and output matching networks are advantageously provided for the BJT. Each network may have a first end for connection to a BJT and a second end for connection to a terminal, and may comprise a series connection of a first inductor, a first capacitor and a second inductor extending from the first end to the second end in that order; a third inductor connected between ground and the connection point of the first capacitor and the second inductor; and a second capacitor connected between ground and the second end.
According to another aspect of the invention, the various reactance components may be implemented on a dielectric board, for example by microstriplines and/or shaped cladding portions.
According to a further aspect, an X-band oscillator may comprise the X-band amplifier described herein, and a feedback circuit interconnecting an output and an input of the amplifier. The feedback circuit may comprise first and second feedback means, for example microstriplines, which may be coupled to a dielectric resonator.
The high frequency BJT amplifier discussed herein is capable of providing a noise level of -145 dBc/Hz or better at 100 Hz offset frequency at an operating frequency of 8.7 GHz (X-band). Typical GaAs amplifiers exhibit a noise level of -125 dBc/Hz at this frequency. Thus, the BJT amplifier has the potential to improve a microwave oscillator's phase noise by as much as 20 dB. It should be noted that the dynamic range of a radar system is usually limited by the frequency source of the system.
The enhanced phase-noise performance of this invention is a significant improvement over present systems operating in this frequency regime, approximately 8-12.4 GHz. A major advantage of the X-band BJT amplifier is that the close-in residual phase noise of a BJT is about 10 to 30 dB better than that of a gallium arsenide field effect transistor (GaAs FET).
Other features and advantages of the present invention will become apparent from the following description of the invention which refers to the accompanying drawings.
Brief Description of the Drawings
Other features and advantages of the present invention will become apparent from the following description of the invention which refers to the accompanying drawings.
FIG. 1 is a schematic diagram of an X-band BJT amplifier according to an embodiment of the present invention.
FIG. 2 is a schematic diagram of a microstrip implementation of the X-band BJT amplifier.
FIGS. 3 and 4 are gain profiles illustrating gain vs. frequency over a broad frequency range and a narrow frequency range, respectively.
FIG. 5 is a schematic diagram of a dielectric resonator oscillator incorporating the X-band BJT amplifier.
Detailed Description of Embodiments of the Invention
A schematic diagram of an X-band amplifier which embodies the invention can be seen in FIG. 1. The input matching network is designed to provide a conjugate match for maximum small-signal gain. An inductance L.sub.1I is used to rotate the impedance looking into the transistor. A capacitance C.sub.1I is used to block DC signals. An inductance L.sub.3I forms a circle on the real axis. An inductance L.sub.2I and a capacitance C.sub.2I transform the circle to a source impedance, in the present case, 50 ohms.
The output matching network is identical in topology to the input matching network. However the output impedance of the amplification stage is different from the input impedance. Therefore L.sub.1O, L.sub.2O, L.sub.3O, C.sub.1O and C.sub.2O will have different values from those of the corresponding input components.
A microstrip implementation of the lumped element design of FIG. 1 is shown in FIG. 2. The circuit is constructed on a 10-mil-thick Duroid board with copper cladding on both sides of the board. The relative dielectric constant of Duroid is about 2.2. Duroid was selected because of its high Q. Standard photolithographic techniques were used for fabrication.
The amplification stage includes a commercially available silicon bipolar junction transistor, for example NE64408, and a standard biasing network. The transistor was operated above the upper frequency limit of 6 GHz specified by the manufacturer. Therefore, the selection of the correct biasing point is critical if maximum gain is to be obtained. The bias attachment point was found by probing different parts of the input and output network. The point is insensitive to gain variation.
Once the board was fabricated and the components comprising the biasing, matching and amplification circuitry were assembled in a suitable fixture, performance verification began. The results of the testing can be seen in FIGS. 3 and 4. The amplifier had a gain of 6 dB at 8.78 GHz. Tuning of the amplifier will improve the overall performance. The gain of the amplifier can be increased by 6 dB to 8 dB by tuning the input and output matching networks. Tuning is achieved by trimming the shorted stub and/or by changing the capacitance values.
Besides constructing this device on Duroid, this X-band BJT amplifier can also be designed to work on metallized ceramic substrates, such as gold on alumina. The amplifier can also be designed with discrete components instead of a hybrid design which is implied with the microstrip version.
The novel microstrip input and output matching network is designed to provide optimal source and load impedance for maximum gain and is the preferred mode of building this device. The X-band BJT amplifier will have improved noise performance, on the order of a 10-30 dB improvement, over a GaAs FET amplifier in this frequency regime. This BJT amplifier is reliable, cost-effective and based on a simple novel design.
The X-band BJT amplifier when used in an oscillator will have superior noise performance, but the output power will not be as large as in an oscillator that uses a gallium arsenide field effect transistor (GaAs FET) amplifier in the oscillator loop. Therefore, to obtain the improved noise performance along with increased output power, a low-noise GaAs FET amplifier (not shown) can be used to augment the output power of the oscillator external to the oscillator loop. This addition will dramatically increase output power while preserving the superior noise performance of the oscillator.
FIG. 5 shows the BJT amplifier incorporated in a dielectric resonator oscillator. As seen, it is preferred that two amplifiers be utilized to overcome the insertion loss of the dielectric resonator and power splitter loss. As shown, there is a feedback circuit which receives a signal from the amplifier output terminal and feeds back the signal to the amplifier input terminal. This feedback circuit is formed on the board and in connected to the amplifier input terminal via a power splitter which has an input terminal and two output terminals wherein the input terminal is connected to the amplifier output terminal and the two output terminals output the signal to an RF output as an output signal of the oscillator and feeds back the signal to the amplifier through open-ended microstrip lines. As those skilled in the art will readily appreciate, even a second feedback circuit may be formed on the board and connected to the power splitter RF output terminal. This second feedback circuit will feed back the RF output to the first feedback circuit. The pair of 50-ohm open-ended microstriplines are respectively connected to the amplifier input and output terminals. The microstriplines are both coupled to a dielectric resonator mounted between them on the Duroid board.
Although the present invention has been described in relation to particular embodiments thereof, many other variations and modifications and other uses will become apparent to those skilled in the art. It is preferred, therefore, that the present invention be limited not by the specific disclosure herein, but only by the appended claims.