Crystal oscillator with broad tuning capability

Abstract: A first transistor (16) is connected in grounded-collector-emitter-follower configuration to generate a high enough negative resistance to overcome the oscillating resistance of a crystal resonator (10) connected to the base electrode. A second transistor (43) connected in grounded-base configuration serves as a buffer and impedance transformer between the low impedance output of the first transistor and the high impedance of a load. An inductor (12) connected between the resonator and the first transistor input and a variable capacitance (24, 25, 26) approximating the shunt capacitance (11) of the resonator connected across the first transistor input form an impedance inverter which absorbs the resonator shunt capacitance and converts the effect of the resonator to a parallel tuned circuit that can be broadly tuned.

Description: This invention relates to crystal controlled oscillators of both bulk wave and surface acoustic wave varieties. One problem often encountered in the manufacture of crystal controlled oscillators in the HF to UHF frequency band is that some of the oscillators will not start under all of the specified operating conditions. This has been the case with oscillators of all three of the common configurations, Colpitts, Clapp and Pierce. To insure reliable starting, manufacturers of the oscillators have resorted to testing the oscillators at temperature extremes to reject non starters, or to specially selecting the crystal resonators, the transistors, or both. Obviously it is desirable, if possible, to eliminate the expense of these procedures. The apparent reason for poor starting is that negative resistance generated by the particular transistor amplifier at small signals is not great enough to overcome the oscillating resistance of the crystal resonator. The sum of the two resistances must be no greater than zero for the oscillator to start. It is well known that the resonator oscillating resistance is a function of the electrode structure used to launch the acoustic waves. Unfortunately, however, structural changes that tend to lower the oscillating resistance, at the same time increase the inter- electrode capacitance. This capacitance shunts the series resonant circuit of the resonator and limits the range of frequency through which the resonator can be "pulled." In fact, the ratio of the series resonant capacitance to the shunt capacitance is sometimes referred to as a figure of merit for tunability of the resonator. This ratio is particularly low in the case of surface acoustic wave (SAW) resonators. As a result of the unfortunate tradeoff between oscillating resistance and shunt capacitance, in addition to starting problems, crystal controlled oscillators in these frequency bands normally have very narrow pull ranges. Where variable frequency is needed, such as in a phase-locked loop, known circuits are unable to take advantage of the high Q that comes with operating a crystal resonator at resonance. They use the resonator either as a reactive component or as a delay line. This usually results in low Q and substantial oscillator noise. T. Matsuura et al. "SAW Voltage-Controlled Oscillator for PLL-FM Modulator", N.E.C. Research and Development, No. 70, July 1983, Tokyo discloses a Colpitts circuit arrangement of a crystal and first transistor used in a voltage-controlled oscillator employing a SAW resonator. A second transistor is connected as a buffer amplifier. According to this invention there is provided a crystal controlled oscillator as claimed in claim 1. Advantages of embodiments of the invention include a crystal controlled oscillator with reliable starting that can be manufactured without special product or component selection, and a variable frequency crystal controlled oscillator with a wide pull range and very low noise because the crystal resonator operates at resonance. Preferably an impedance inverter comprising an inductor connected between the resonator and the high impedance transistor input and a variable capacitance connected across the high impedance input, the capacitance value of which approximates the shunt capacitance of the crystal resonator, absorbs the shunt capacitance of the crystal resonator and converts the effect of the resonator from a series resonant circuit to a parallel resonant circuit that can be broadly tuned. The invention will now be described with reference to the accompanying drawings, in which: FIG. 1 is a generally accepted equivalent circuit of a crystal resonator, FIG. 2 is a simple block representation of an impedance inverter for use in the invention; FIG. 3 is a diagram of a simple pi section useful in explaining the operation of part of the invention; FIG. 4 is a particularly useful variable frequency embodiment of the invention; and FIG. 5 is a useful fixed frequency embodiment of the invention. Detailed Description Theory of operation: Referring to the equivalent circuit of a crystal resonator, FIG 1, the crystal element may be represented at resonance by the series combination of L R C R and R R shunted by interelectrode capacitance C o . For a typical crystal resonator operating in the HF to UHF frequency range, of either bulk or surface acoustic wave (SAW) variety, the oscillating resistance R R is relatively high between about 20 and 60 ohms. In a typical Pierce, Colpitts or Clapp oscillator circuit, on the other hand, the negative resistance facing the crystal resonator at low signal amplitude is relatively low. Typical values fall in the range of 20 to 50 ohms. This basic incompatibility between the range of resonator operating resistance and developed negative resistance explains the starting difficulties. The small signal developed negative resistance can be substantially increased if the oscillator transistor is connected in grounded collector, emitter follower connection. This results, however, in such a low output impedance that the circuit will not oscillate with a 50 ohm load. As a consequence, a second transistor is used as a buffer to present an output impedance to match the load. Negative resistances in the order of 100 ohms are thereby available to eliminate the starting problem. With the availability of such high negative resistance, the pulling range restriction can also be greatly ameliorated. Consider again the shunt capacitance C o of the crystal resonator, FIG 1. If it were not for C o , additional capacitance added in series with the resonator would have the effect of reducing CR, thereby changing the resonant frequency. The only degradation to the quality factor Q of the circuit would be due to the resistance of the added variable capacitor. The presence of C o , however, prevents such simple addition. Consider, however, an impedance inverter, shown in FIG 2, in which, by definition Z out = K² Z in . If a crystal resonator were connected to the input terminals of the impedance inverter, it would look from the output like a parallel RLC circuit instead of the series RLC circuit of FIG 1. In theory, an impedance inverter in the form of a pi circuit with an inductance series arm would have to have negative inductance shunt arms. Fortunately, however, crystal oscillators are very narrow band devices, even those regarded as "broadly tunable". A very suitable approximation of the theoretical impedance inverter for narrow band operation can be made using real passive components. The pi section shown in FIG 3, in which L i is the value of series inductance and C i the value of shunt capacitance will perform impedance inversion at a frequency f o , when the following equation is satisfied: 2 π f o L i = 1 2 π f o C i , which incidentally = K. Furthermore, the troublesome capacitance C o can become the inverter input shunt capacitance C i , making it virtually disappear. The series resonant circuit that represents the crystal resonator now appears as a parallel resonant circuit at the output of the impedance inverter. Slight changes in the output inverter capacitance C i add directly to the parallel capacitance due to the crystal resonator to directly change the resonant frequency. The result is a significantly improved crystal oscillator circuit whose frequency can be varied over a relatively wide range with very little added noise or loss of stability. A particularly useful embodiment of the invention is shown in the schematic diagram of FIG 4, which may, for example be a SAW oscillator operating in the vicinity of 600 MHz. One side of a SAW resonator 10 is connected to ground; the other end is connected via an inductor 12 and a coupling capacitor to the base of a transistor 16. The inherent shunt parallel parasitic capacitance of SAW resonator 10 is shown as capacitor 11. The collector of transistor 16 is connected to a source of operation voltage B+, and the emitter is connected through a resistor 18 to ground. Biasing resistors 19 and 20 connect the base of transistor 16 to B+ and ground, respectively. The junction between inductor 12 and capacitor 14 is shunted to ground via several paths. One path is an inductance 22. A second path is the series combination of two varactor diodes 24 and 25, respectively and a capacitor 26. A third path includes a resistor 28 in series with the parallel combination of an inductor 29 and capacitor 30. The junction between varactor diodes 24 and 25 may be connected via a resistor 32 to a source of temperature compensating voltage 33, and the junction between varactor diode 25 and capacitor 26 may be connected via a voltage divider made up of resistors 35 and 36 to a frequency control voltage source 37. The emitter of transistor 16 may be connected via the series combination of a capacitor 40 and an inductor 41 to the emitter of a second transistor 43. The collector of transistor 43 is connected to operating voltage B+ via a resistor 45, and the emitter is connected to ground via resistor 46. A capacitor 48 connects the base of transistor 43 to ground, and a pair of biasing resistors 49 and 50 connect it to B+ and ground, respectively. Finally, a coupling capacitor 52 connects the collector of transistor 43 to the oscillator output terminal 54. To understand the operation and therefore the design considerations of the variable frequency oscillator of FIG 4, consider the following: The emitter-follower configuration of bipolar transistor 16 has a high input impedance. With a low impedance capacitive load connected to the emitter, transistor 16 generates about 150 ohms negative resistance facing the crystal resonator 10, enough to insure excellent starting characteristics without special selection of resonators or transistors. Biasing resistors 19 and 20 are at least an order of magnitude above this level to avoid substantially affecting it. Transistor 43 acts as an impedance-transforming buffer. Its low input impedance looking into the emitter supplies the low impedance load for transistor 16. Collector resistor 45 has a high enough resistance to allow the oscillator circuit to drive a load connected to output 54 of usually, but not necessarily, about 50 ohms. Capacitor 48 provides ac ground for the base electrode. In the embodiment, emitter resistor 18 is intentionally not bypassed in order to provide dc negative feedback to reduce low frequency noise. Capacitor 40 and inductor 41, which couple the two oscillator transistors, form a series tuned circuit slightly above the operating frequency. This tuned circuit provides unimpeded coupling at the operating frequency and helps prevent spurious frequencies. Resonator shunt capacitance 11, series inductor 12, and the shunt paths of inductor 22 and the series combination of varactor diodes 24 and 25 and capacitor 26 form an imnedance inverter 60. The shunt leg comprising elements 22, 24, 25 and 26, therefore, at the operating frequency represents a capacitance equal to the resonator parasitic shunt capacitance 11. The inductance of inductor 12 is therefore chosen to satisfy the relationship 2 π f o L₁₂ = 1 2 π f o C₁₁ , where L₁₂ is the inductance of inductor 12 and C₁₁ is capacitance 11. Capacitor 26 is added in series with variable capacitance 25, in accordance with common practice to lower the slope of the varactor characteristic and make tuning more linear. Resistors 35 and 36 are chosen to set the optimum operating point of varactor diode 25. Matching varactor diode 24 is connected in series with diode 25, and temperature compensating voltage may be injected at the junction via input 33 and resistor 32, again in accordance with common practice. Since the two shunt arms of the pi configured impedance inverter 60 must present the same impedance, inductor 22 is added in parallel with the two diodes and capacitor 26 to match the resonator parasitic shunt capacitance, C₁₁. The use of impedance inverter 60, in making the resonator look like a parallel tuned circuit, also makes it more likely to oscillate at spurious frequencies. Inductor 29 and capacitor 30 are chosen to provide parallel resonance at the oscillator operating frequency. They therefore represent an open circuit over the operating range and a low impedance, limited by the value of resistor 28, to dampen and thereby prevent oscillation outside the desired range. The particular embodiment shown in FIG 4 using a SAW resonator operating at 622 MHz has demonstrated a frequency pull range in excess of 500 KHz and a phase noise level of better than -95 dBc at 1 KHz away from the carrier. Where a fixed frequency temperature compensated oscillator is desired, the circuit of FIG 5 can be very useful. In this figure, the components which are similar to those in the embodiment of FIG 4 have similar identifying numbers preceded by the prefix 1. Transistor 116 is therefore connected as a grounded-collector emitter-follower and transistor 143 as an impedance-transformer buffer to provide reliable starting. In this case, since a wide tuning range is not desired, an impedance inverter need not be included. Inductor 113 is actually a small inductance to tune out the capacitive impedance generated by the transistor circuit. The two varactor diodes for temperature compensation, 124 and 125, may be connected between transistor emitters, with the compensating voltage injected between them from input 133. I have thus described a novel construction for crystal oscillators of both fixed and variable frequency types, which eliminate the common starting problem. In addition, the variable frequency variety operates over a broad tuning range without operating the crystal out of resonance, but by shifting the resonance. It will be obvious to those skilled in oscillator design that many modifications of the embodiments described may be made

Claims: A crystal controlled oscillator including a first transistor (16) connected in a grounded collector-emitter-follower configuration to provide a relatively high impedance input at its base electrode and a relatively low impedance output at its emitter electrode, a crystal resonator (10) connected between the high impedance input and ground, and a second transistor (43) connected as a buffer amplifier to the first transistor (16) CHARACTERIZED BY: the second transistor (43) having a grounded base configuration and a relatively low impedance input connected to the low impedance output of the first transistor and a relatively high impedance output for connection to a load. An oscillator as claimed in claim 1, wherein the connection between the crystal resonator and the high impedance input includes inductance means (12). An oscillator as claimed in claim 1 or 2, wherein the first transistor low impedance output includes unbypassed emitter resistance means to reduce low frequency noise. An oscillator as claimed in claim 1, 2 or 3, wherein the connection between the first and second transistors includes two varactor diodes (124,125) connected in series, and there is provided temperature compensating voltage input means (133) connected to the junction between the diodes for receiving a voltage to reduce changes in the frequency of the oscillator due to changes in operating temperature. An oscillator as claimed in claim 1, including impedance inverting means (60) connected between the crystal resonator and the high impedance input for converting the effect of the resonator on the first transistor from a series resonant circuit to a parallel resonant circuit. An oscillator as claimed in claim 5, wherein the impedance inverting means includes inductance means (12) connected between the crystal resonator and the high impedance input, and variable capacitance means (24,25,26) connected across the high impedance input for varying the resonant frequency of the crystal resonator, the variable capacitance means having a capacitance value approximating the shunt capacitance (11) of the crystal resonator. An oscillator as claimed in claim 6 wherein the variable capacitance means includes a first varactor diode (25) and a fixed capacitor (26) connected in series, and frequency control voltage input means (35,36,37) connected to the junction between the first varactor diode and the fixed capacitor for receiving a resonant frequency controlling voltage. An oscillator as claimed in claim 7, wherein the variable capacitance means includes a second varactor diode (24) connected to the first varactor diode, and temperature compensating voltage input means (32,33) connected to the junction between the first and second varactor diodes for receiving a temperature compensating voltage. An oscillator as claimed in claim 5,6,7 or 8, including a parallel resonant circuit (29,30) resonant in the operating frequency range of the oscillator connected across the high impedance input to suppress spurious frequency operation. An oscillator as claimed in claim 5,6,7, 8 or 9, wherein the connection between the first transistor low impedance output and the second transistor low impedance input includes a series resonant circuit (40,41) to suppress spurious frequency operation.

Inventors: GONDA JOSEPH, GONDA, JOSEPH
Applicants: AT & T CORP, AT&T CORP.
Application year: 1990
Main classification: H03B5
IPC codes: H03B1, H03B5, H03B7