CA2290862C - A frequency/phase comparison circuit with gated reference and signal inputs - Google Patents
A frequency/phase comparison circuit with gated reference and signal inputs Download PDFInfo
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- CA2290862C CA2290862C CA 2290862 CA2290862A CA2290862C CA 2290862 C CA2290862 C CA 2290862C CA 2290862 CA2290862 CA 2290862 CA 2290862 A CA2290862 A CA 2290862A CA 2290862 C CA2290862 C CA 2290862C
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- H—ELECTRICITY
- H03—ELECTRONIC CIRCUITRY
- H03L—AUTOMATIC CONTROL, STARTING, SYNCHRONISATION, OR STABILISATION OF GENERATORS OF ELECTRONIC OSCILLATIONS OR PULSES
- H03L7/00—Automatic control of frequency or phase; Synchronisation
- H03L7/06—Automatic control of frequency or phase; Synchronisation using a reference signal applied to a frequency- or phase-locked loop
- H03L7/16—Indirect frequency synthesis, i.e. generating a desired one of a number of predetermined frequencies using a frequency- or phase-locked loop
- H03L7/18—Indirect frequency synthesis, i.e. generating a desired one of a number of predetermined frequencies using a frequency- or phase-locked loop using a frequency divider or counter in the loop
-
- H—ELECTRICITY
- H03—ELECTRONIC CIRCUITRY
- H03D—DEMODULATION OR TRANSFERENCE OF MODULATION FROM ONE CARRIER TO ANOTHER
- H03D13/00—Circuits for comparing the phase or frequency of two mutually-independent oscillations
- H03D13/003—Circuits for comparing the phase or frequency of two mutually-independent oscillations in which both oscillations are converted by logic means into pulses which are applied to filtering or integrating means
- H03D13/004—Circuits for comparing the phase or frequency of two mutually-independent oscillations in which both oscillations are converted by logic means into pulses which are applied to filtering or integrating means the logic means delivering pulses at more than one terminal, e.g. up and down pulses
-
- H—ELECTRICITY
- H03—ELECTRONIC CIRCUITRY
- H03L—AUTOMATIC CONTROL, STARTING, SYNCHRONISATION, OR STABILISATION OF GENERATORS OF ELECTRONIC OSCILLATIONS OR PULSES
- H03L7/00—Automatic control of frequency or phase; Synchronisation
- H03L7/06—Automatic control of frequency or phase; Synchronisation using a reference signal applied to a frequency- or phase-locked loop
- H03L7/08—Details of the phase-locked loop
- H03L7/085—Details of the phase-locked loop concerning mainly the frequency- or phase-detection arrangement including the filtering or amplification of its output signal
- H03L7/089—Details of the phase-locked loop concerning mainly the frequency- or phase-detection arrangement including the filtering or amplification of its output signal the phase or frequency detector generating up-down pulses
- H03L7/0891—Details of the phase-locked loop concerning mainly the frequency- or phase-detection arrangement including the filtering or amplification of its output signal the phase or frequency detector generating up-down pulses the up-down pulses controlling source and sink current generators, e.g. a charge pump
-
- H—ELECTRICITY
- H03—ELECTRONIC CIRCUITRY
- H03L—AUTOMATIC CONTROL, STARTING, SYNCHRONISATION, OR STABILISATION OF GENERATORS OF ELECTRONIC OSCILLATIONS OR PULSES
- H03L7/00—Automatic control of frequency or phase; Synchronisation
- H03L7/06—Automatic control of frequency or phase; Synchronisation using a reference signal applied to a frequency- or phase-locked loop
- H03L7/08—Details of the phase-locked loop
- H03L7/099—Details of the phase-locked loop concerning mainly the controlled oscillator of the loop
-
- H—ELECTRICITY
- H03—ELECTRONIC CIRCUITRY
- H03L—AUTOMATIC CONTROL, STARTING, SYNCHRONISATION, OR STABILISATION OF GENERATORS OF ELECTRONIC OSCILLATIONS OR PULSES
- H03L7/00—Automatic control of frequency or phase; Synchronisation
- H03L7/06—Automatic control of frequency or phase; Synchronisation using a reference signal applied to a frequency- or phase-locked loop
- H03L7/08—Details of the phase-locked loop
- H03L7/14—Details of the phase-locked loop for assuring constant frequency when supply or correction voltages fail or are interrupted
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- H—ELECTRICITY
- H04—ELECTRIC COMMUNICATION TECHNIQUE
- H04L—TRANSMISSION OF DIGITAL INFORMATION, e.g. TELEGRAPHIC COMMUNICATION
- H04L27/00—Modulated-carrier systems
- H04L27/02—Amplitude-modulated carrier systems, e.g. using on-off keying; Single sideband or vestigial sideband modulation
-
- H—ELECTRICITY
- H03—ELECTRONIC CIRCUITRY
- H03L—AUTOMATIC CONTROL, STARTING, SYNCHRONISATION, OR STABILISATION OF GENERATORS OF ELECTRONIC OSCILLATIONS OR PULSES
- H03L2207/00—Indexing scheme relating to automatic control of frequency or phase and to synchronisation
- H03L2207/18—Temporarily disabling, deactivating or stopping the frequency counter or divider
-
- H—ELECTRICITY
- H04—ELECTRIC COMMUNICATION TECHNIQUE
- H04L—TRANSMISSION OF DIGITAL INFORMATION, e.g. TELEGRAPHIC COMMUNICATION
- H04L27/00—Modulated-carrier systems
- H04L27/0014—Carrier regulation
- H04L2027/0044—Control loops for carrier regulation
- H04L2027/0053—Closed loops
- H04L2027/0055—Closed loops single phase
Abstract
Disclosed is a frequency-locked loop (FLL), which attempts to bring about frequency and phase synchronization between two signals over the control bandwidth of the loop: a reference signal and a voltage-controlled oscillator (VCO) signal. For example, the FLL employs a reference signal generated by a crystal oscillator of frequency .function. REF and a VCO signal generated by the oscillations of an unquenched SRG resonator with tunable resonant frequency .function. RES.
These signals are connected to the inputs of a phase/frequency detector (PFD) which produces output pulses in response to the relationship between .function.REF
and .function.RES. These pulses are applied to a loop filter (LF) which creates a voltage using some kind of charge-storage element. This loop filter voltage is a so-called error voltage whose value is used to control the frequency of the resonator to bring the reference signal and VCO signal into phase synchrony.
These signals are connected to the inputs of a phase/frequency detector (PFD) which produces output pulses in response to the relationship between .function.REF
and .function.RES. These pulses are applied to a loop filter (LF) which creates a voltage using some kind of charge-storage element. This loop filter voltage is a so-called error voltage whose value is used to control the frequency of the resonator to bring the reference signal and VCO signal into phase synchrony.
Description
TITLE
A Frequency/Phase comparison circuit with gated reference and signal inputs FIELD OF THE INVENTION
The invention relates to automatic frequency comparison and/or control (AFC) of a phase/frequency of a signal with that of a reference. In a particu:ar embodiment, it is directed to a novel frequency-locked loop architecture which uses gated input and reference signals.
BACKGROUND OF THE INVENTION
The AFC of the invention will be described in connection with a superregenerative (SRG) radio receiver, though the invention should find other AFC applications. SRG radio receivers are used widely for reception of RF
(radio frequency) signals because of its circuit simplicity and exceptionally high signal sensitivity. SRG radio receivers require a stable tuned circuit which is realized by the used of some kind of AFC. It should be noted that frequency and phase can be used interchangeably and the invention can be described by using in either term.
It is however decided that "frequency" is used throughout the present specification.
A block diagram of a simple SRG receiver is depicted in Figure 1. The input signal V~. is an RF signal at a fixed frequency f~ which is modulated with amplitude-shift keying (ASK); digital data is often transmitted as binary data. V~
is connected to some kind of resonant circuit with natural center frequency fps.
This resonant circuit is connected to some kind of Q control circuit such that overall resonator O is variable, controlled by a deterministic. signal Vq. In Figure 1, the resonant circuit is an LC tank circuit with the parallel conductance go representing losses in the passive components, i.e., finite tank Q, and a transconductor gm configured as a tunable negative resistor, but other kinds of circuit (e.g., a ring oscillator) are possible. The resonator output voltage VAS is connected to an envelope detector followed by a band pass filter (BPF), the combination of which produces a voltage VoU.t. which contains the demodulated data.
Operation of the SRG receiver just described is as follows. The 0 control circuit is driven with a periodic voltage (period Tq, frequency fq = 1/Tq) such that for the majority of the period, the resonator is made very slightly unstable.
VAS
begins to oscillate, building in amplitude with an envelope whose shape is exponential; if left to build for a sufficient period of time, the shape ceases to be exponential because it eventually succumbs to an amplitude limiting mechanism.
Usually such a mechanism is inherent to the SRG, for example nonlinearity in the Q control circuit or finite power supply voltage. For the remaining small portion of Tq, the Q control is driven such that the resonator is very stable, to the point that any built-up oscillations rapidly die out and VAS falls to near zero. This is known as "quenching the oscillation". The quench frequency must be at least twice the data rate as the quenching is a form of sampling of the data and the sampling rate is governed by normal Nyquist restrictions.
The method of data detection at V~ works as follows. During the portion of Tq when VAS is permitted to oscillate, the oscillations commence because of wideband thermal noise inherent to any practical electrical system; this creates a nonzero voltage on VAS, and positive feedback inside the resonator passband ensures noise components at frequencies close to fps are amplified more than those at other frequencies. As a result, the frequency of the built-up oscillation immediately prior to quenching is the same as the natural center frequency of the resonator. If there is coherent energy at the RF input V~. (i.e., a carrier) that falls within the passband of the resonator, then the build-up of resonator oscillations is encouraged: the initial voltage at VAS has a larger magnitude than it would if only noise were present. The time constant of the exponential build-up is determined by the setting of Vq alone, and so it is the same whether or not passband energy on V~ is present; the more energy present on V~, therefore, the greater the final amplitude of the oscillation. Thus, the energy build-up on VAS is proportional to the passband power on V~ and an envelope detectorBPF combination is sufficient to generate a signal proportional to this latter quantity. The envelope detector maintains the subcarrier position of the data relative to the carrier while translating the modulated signal to baseband. Hence, unmodulated signals translate to do and are rejected by the baseband BPF, while the data pass through the BPF. Of course the BPF must be appropriately matched to the data frequency.
Figure 2 illustrates typical waveforms and waveform envelopes during the operation of the receiver, all being time coordinated. Vq represent a periodical control signal for quenching. VAS envelope shows exponential build-ups and decays of oscillation amplitude.
Usual embodiments of SRG receivers use a resonator with a fixed center frequency. They require this center frequency to be set fairly precisely because the resonator passband is very narrow during operation (this improves sensitivity to weak RF signals). Component tolerances are often sufficiently poor that fps can only be set with enough accuracy via mechanical means (for example, 1 S trimming the value of a tunable capacitor by hand) prior to first use of the receiver. Thereafter, fps cannot be changed over the life of the circuit unless it is recalibrated. Manual setting of the resonator frequency is error-prone and expensive; more seriously, fps might drift after calibration, for example, due to component aging or temperature variations. As noted above, the Vq control is operated such that when the resonator is made to oscillate, the band of frequencies to which the oscillator is sensitive is very narrow; even a slight frequency drift can be enough to mean the transmitted data on V~. is no longer within the resonator passband, which means the SRG receiver is no longer capable of receiving the data.
The present invention addresses these problems by the use of the automatic phase/frequency control in general. Its basic concept is applicable to a variety of areas in which phase/frequency control is needed. The invention, however, is described in detail in connection with the SRG in which the resonator center frequency is made tunable (for example, by replacing the capacitor in an LC-based resonator with a varactor), and the AFC of the invention is provided for adjusting f~S with no e:cternal mechanical control. Moreover, the invention provides a means of controlling fps during receiver operation so that the center frequency is held fi:ced, even in the face of mechanisms which would otherwise cause the frequency to drift.
Other advantages, objects and features of the present invention will be readily apparent to those skilled in the art from a review of the following detailed description of preferred embodiments in conjunction with the accompanying drawings and claims.
SUtIMARY OF THE INVENTION
Briefly stated, the invention is directed to a frequency comparison circuit for comparing frequencies of a variable signal and a reference signal. The frequency comparison circuit includes a phase frequency detector for comparing frequencies of the variable signal and the reference signal and for generating an output that depends upon the relationship of the frequencies; and gate modules at the inputs of the phase frequency detector for gating the variable signal and the reference signal so that only a portion of the variable signal and reference signal are repetitively applied to the inputs of the phase frequency detector for processing.
In accordance with another aspect, the invention is directed to a frequency lock loop circuit for maintaining a predetermined frequency relationship between a detected signal and a reference signal. The frequency lock loop circuit includes a variable tuning circuit for adjusting its tuning frequency to generate the detected signal and a frequency comparator for comparing the frequencies of the detected and reference signals and for generating an output responsive to their frequency relationship. The frequency lock loop circuit further includes a gate module for applying repetitively and coincidentally only a predetermined portion of the detected signal and the reference signal to the frequency comparator for generating the output, and a loop circuit connecting the variable tuning circuit and the frequency comparator for applying the output to the variable tuning circuit to adjust its tuning frequency so that the predetermined frequency relationship is maintained between the detected signal and the reference signal.
In accordance with yet a further aspect the invention is directed to an RF
receiver of the superregenerative type for detecting an amplitude shift keyed RF
signal at a predetermined frequency. The RF receiver includes an RF amplifier for amplifying the RF signal, an RF tuning circuit connected to the RF
amplifier and tuned to the RF signal at the predetermined frequency for generating a detected signal, and a quenching circuit attached to the RF tuning circuit for quenching periodically the oscillation of the RF tuning circuit. The RF
receiver further includes an envelope detector connected to the RF tuning circuit for producing amplitude shift keyed data carried on the detected signal, a reference signal generator for generating a reference signal, and a loop module connected to the RF tuning circuit and the reference generator for generating a locking output in response to frequency relationship between the reference signal and the detected signal. In the RF receiver, there are provided further a frequency adjusting circuit connected to the RF tuning circuit for adjusting the predetermined frequency to lock it to the reference frequency, and a gate module for sampling the detected signal and the reference signal for a portion thereof to be inputted to the loop module for generating the locking output.
BRIEF DESCRIPTION OF THE DRAWINGS
Figure 1 is a schematic block diagram of a known SRG receiver.
Figure 2 shows typical shapes of waves and wave envelopes during operation of the SRG receiver shown in Figure 1.
Figure 3 is a schematic block diagram of a SRG receiver according to one embodiment of the invention.
Figure 4 is a gate circuit that can be used in an embodiment of the invention.
Figure 5 is a timing diagram according to an embodiment of the invention.
Figure 6 is another gate circuit that can be used in an embodiment of the invention.
Figure 7 shows waveforms of some signals used to describe the invention.
Figure 8 is a computer simulation result of one embodiment of the invention.
DETAILED DESCRIPTION OF THE INVENTION
An embodiment of the invention as applied to a SRG receiver is shown in the dashed box of Figure 3. Frequency-locked loop (FLL) is known and it is used where frequency and/or phase synchronization must be maintained between two signals over the control bandwidth of the loop. In the figure, two signals are a reference signal and a voltage-controlled oscillator (VCO) signal. The reference signal is generated by a crystal oscillator 30 of frequency f~F, and the VCO
signal is generated by the oscillations of an unquenched SRG resonator (possibly passed through a limiting amplifier 32) with tunable resonant frequency f~S. The VCO
signal is VAS. In some embodiments, either or both of the reference and VCO
signals can be reduced in frequency by dividing by certain factors. As examples, the figure shows dividers as =R (divide-by-R) and =N (divide-by-N) blocks e.g., counters. These (and possibly divided-down) signals are connected to the inputs of a phase/frequency detector (PFD). A PFD circuit is a known circuit which compares the phases of two input signals at its R and V inputs, denoted "R"
and "V" for "reference" and "VCO". If a reference rising edge precedes a VCO
rising edge, an "up" pulse denoted "U" is generated at the U output, while a VCO edge preceding a reference edge generates a "down" ("D") pulse at the D output.
These pulses are used to control the current sources 34 and 36 in a charge-pump circuit whose net current is applied to a loop filter (LF) which includes some kind of charge-storage element e.g., a capacitor, and generates a voltage VLF. This loop filter voltage VLF is a so-called error voltage whose value is used to control the frequency of the resonator by way of a varactor 38. The combination of PFD, charge pump, and LF is connected such that the error voltage is used to bring the reference signal and VCO signal into phase synchrony. The FLL equilibrium condition can be shown to be REF f RES
R _ N (1) As seen from the above equation, the resonator frequency fps can be set by appropriate choice of f~F, R and N. This equilibrium is maintained by the average frequency of the noise in the SRG receiver alone and does not require a data signal present at V~ to maintain frequency control of the resonator.
Referring further for Figure 3, each =R and =N block is a digital circuit which counts positive-going transitions at its input; when the count reaches R
or N, as appropriate, the block's output switches to the opposite binary state (from 0 to 1 or 1 to 0, as appropriate). Often, R and N are integer powers of two and the blocks are implemented as dividers made up of a chain of flip-flops. As described earlier, the =N block receives its input from the resonator signal (VCO signal or VAS), possibly amplified by a limiter circuit, e.g., a block shown by 32. In the case of an SRG receiver, the oscillations of the resonator are periodically quenched by Vq to near-zero levels, after which time they must exponentially (slowly in the beginning) build in amplitude. Therefore, for much of the period of Vq, resonator oscillations have neither sufficient amplitude nor regular-enough zero crossings to reliably drive the =N block. It is only for some small fraction of the quench period just prior to quenching that the resonator oscillations are sufficiently large for the =N block to count correctly. By contrast, the crystal always produces large fixed-amplitude oscillations with regular zero crossings, so there is no danger of the =R block counting incorrectly. Likewise, in cases where there is no =N block, the VCO signal may not have sufficient amplitude to drive PFD correctly.
According to the basic concept of the invention, the VCO signal is gated to ensure that only a portion thereof which is strong enough to drive =N block (or the PFD V input, in the case of no frequency division) correctly is applied to the input. The same gating must be applied to the =R block (or the PFD R input, in g the case of no frequency division) and the outputs of the PFD for generating a proper error signal at VLF.
The preferred embodiment of the invention shown in Figure 3 features a coupling between the FLL enable signal VE;~ (gating signal) and the SRG
resonator O control voltage Vq (VCO signal). Therefore, were it not for t1'~e gating signal V~,,, the combination of correct =R counting and incorrect =N counting (when VAS is too small) would cause equation ( 1 ) not to be satisfied, which in turn would result in the resonator being tuned to a frequency other than the desired one. In the invention, V~,, is controlled such that the divider blocks count only when VAS is of sufficient amplitude to ensure accurate counting, which ensures the relationship in (1) holds and the resonator is tuned to the desired frequency. In this embodiment, V~,, is asserted for a fixed period prior to the quenching of resonator oscillations, then negated at the same instant that quenching is commenced, though it is possible to negate some time prior to the start of quenching. The duty cycles of VEN and Vq need not be related, but the periods of both signals will be the same, namely, Tq.
While the concept described above is sound, a further improvement may be possible. Referring further to Figure 3, such improvements are described.
In the embodiment of Figure 3, no timing relationship between gating signal VE,,, and the reference voltage signal VHF is enforced. Thus, it is possible for V~ to become enabled or disabled at arbitrary phases of a cycle of V~. But this leads to the following subtlety: let us suppose the switch 40 which is controlled by VErr were a simple digital AND gate with inputs V~ and V~ and output VoB, as shown in Figure 4. Then under certain circumstances, it would be possible for an extra count to be erroneously registered. A.n example of those circumstances appears in the timing diagram of Figure 5. If a falling edge of V~,, occurs while V~. is high, and the immediately subsequent rising edge of V~,, also occurs while VHF is high, then an unwanted rising edge is generated on VoB, as shown inside the dotted ellipse in Figure 5. This edge is unwanted because it leads to an incorrect count and hence locking to an improper frequency. One possible means to correct this error is to gate V~ with V~,, such that their output resembles VoG
as shown in Figure ~. An example of a gating circuit which gives this behaviour is shown in Figure 6, though this is by no means the only method to correct the problem. A circuit like Figure 6 can be used for both the VHF and VAS switches 40 and 42 in the preferred embodiment to ensure the correct counts are obtained;
however, a simple AuID gate structure such as Figure 4 will suffice for the V~-controlled switches 44 and 46 at the outputs of the PFD. The essential operation of the invention requires that the FLL be completely disabled when V~,, is negated, then reenabled with the same state as that which existed during the previous enable period when V~ is next asserted.
It was noted earlier that the invention is not required to have fq, the frequency of Vq, to be related to any of the quantities f~F, f~F/R, f~S, or f~s/N. It might appear that this will, under certain conditions, make it impossible for the loop to lock properly because phase continuity is lacking. Although the reference signal is likely to be a square wave, for the moment consider it as a sinusoidal wave so that its division into 360° of phase is more apparent. In Figure 7 depicted is a sinusoidal reference signal and binary VE,,, gating signal. Because the FLL is disabled when V~ is deasserted, V~ may be considered as chopping the reference voltage waveform V~ as depicted in the bottom diagram (it does the same to the resonator voltage VAS). From the FLL's perspective, both reference and resonator voltages appear as a series of segments of continuous waves, and as shown in Figure 7, there is no guarantee that the phase of either signal is the same from the end of one enable period to the start of the next. Even if VHF and V~
were forced into phase continuity by generating them from the same voltage source, there would still be timing fitter, noise, etc., meaning that the reference phase as seen by the FLL would deviate slightly from perfectly continuous. Not only is the reference voltage phase as seen by the FLL potentially discontinuous, but the resonator voltage phase is guaranteed to be discontinuous in an SRG
receiver. When RF input data is absent, resonator oscillations start through thermal noise processes, which means the final oscillation will have a phase that is random and uniformly distributed over the interval [-n, ~] radians. When RF
input data is present, the final resonator oscillation phase tends to align with that of the RF input, but sources of noise unavoidably present inside the resonator bandwidth lead to some deviation of oscillator phase compared to that of the RF input.
It is not the intent of the invention to lock perfectly to the desired frequency f~, but merely for the resonator to be held centered near the correct frequency with a minimum of modulation. The locking frequency is a random variable F with a probability distribution centered at f~ as desired and a standard deviation that is a function of a number of parameters such as the enable duty 10 cycle, the loop filter bandwidth, the charge pump current, etc. Moreover, when fps is far away from f~, the FLL does indeed pull the loop into lock at f~ as determined by equation (1). So long as V~,, is asserted only when the resonator oscillations are of sufficient amplitude to successfully drive the =N block, phase discontinuity can be made not to hinder correct operation of the SRG receiver by appropriate choices of parameters. That is to say, the variance of the locking frequency ~~. can be made small enough such that f~ is always within the passband of the resonator, and that the frequency control loop does not affect the phase of the incoming ASK signal.
In summary, the invention is distinguished from prior art by (a) the addition of an enable signal V~,, whose value gates the inputs to the division blocks as well as the PFD outputs, (b) the sampled nature of the loop, (c) the relaxing of the requirement that input data be present (the invention works when thermal noise alone causes the oscillation), and (d) the relaxing of the usual requirement that a mirror cell be used to control the active filter. Frequency control is done on the filter while operating regardless of the. presence or absence of data.
Figure 8 is a computer simulation of fps as a function of time built with a special-purpose program to study the pull-in and locking behaviour of this sampled FLL. The initial frequency was 305MHz, and f~F = 4MHz, R =32, and N = 2520 were used, meaning from (I) that the expected locking frequency is fps = 3 I SMHz. V~ was asserted for a fraction of Tq given by (3 = 0.13, and it is seen that the loop successfully pulls into lock after about 1.8s. The slew rate of the loop filter voltage in V/s can be shown to be given by SRLF = ~Ip 2C (~) where IP is the charge pump current and in the case of a so-called Type II
loop filter, the kind depicted in Figure 3, C is the sum of the small and large capacitors.
For an initial frequency error, the acquisition time ta~q can be shown to be 2~~f~C
(3) p R
where KR is the tuning gain of the resonator in MHZ/V. Finally, the fitter 6 LF on the loop filter voltage after the loop achieves lock is found to be related to 0.6 2 IpRLFa l 2 TR V
q where 6 ~ is the standard deviation of the time fitter on the reference frequency zero crossings and in the case of a Type II loop filter, RLF is the loop filter resistor.
Numerous modifications, variations, and adaptations may be made to the particular embodiments of the invention described above without departing from the scope of the invention, which is defined in the claims.
A Frequency/Phase comparison circuit with gated reference and signal inputs FIELD OF THE INVENTION
The invention relates to automatic frequency comparison and/or control (AFC) of a phase/frequency of a signal with that of a reference. In a particu:ar embodiment, it is directed to a novel frequency-locked loop architecture which uses gated input and reference signals.
BACKGROUND OF THE INVENTION
The AFC of the invention will be described in connection with a superregenerative (SRG) radio receiver, though the invention should find other AFC applications. SRG radio receivers are used widely for reception of RF
(radio frequency) signals because of its circuit simplicity and exceptionally high signal sensitivity. SRG radio receivers require a stable tuned circuit which is realized by the used of some kind of AFC. It should be noted that frequency and phase can be used interchangeably and the invention can be described by using in either term.
It is however decided that "frequency" is used throughout the present specification.
A block diagram of a simple SRG receiver is depicted in Figure 1. The input signal V~. is an RF signal at a fixed frequency f~ which is modulated with amplitude-shift keying (ASK); digital data is often transmitted as binary data. V~
is connected to some kind of resonant circuit with natural center frequency fps.
This resonant circuit is connected to some kind of Q control circuit such that overall resonator O is variable, controlled by a deterministic. signal Vq. In Figure 1, the resonant circuit is an LC tank circuit with the parallel conductance go representing losses in the passive components, i.e., finite tank Q, and a transconductor gm configured as a tunable negative resistor, but other kinds of circuit (e.g., a ring oscillator) are possible. The resonator output voltage VAS is connected to an envelope detector followed by a band pass filter (BPF), the combination of which produces a voltage VoU.t. which contains the demodulated data.
Operation of the SRG receiver just described is as follows. The 0 control circuit is driven with a periodic voltage (period Tq, frequency fq = 1/Tq) such that for the majority of the period, the resonator is made very slightly unstable.
VAS
begins to oscillate, building in amplitude with an envelope whose shape is exponential; if left to build for a sufficient period of time, the shape ceases to be exponential because it eventually succumbs to an amplitude limiting mechanism.
Usually such a mechanism is inherent to the SRG, for example nonlinearity in the Q control circuit or finite power supply voltage. For the remaining small portion of Tq, the Q control is driven such that the resonator is very stable, to the point that any built-up oscillations rapidly die out and VAS falls to near zero. This is known as "quenching the oscillation". The quench frequency must be at least twice the data rate as the quenching is a form of sampling of the data and the sampling rate is governed by normal Nyquist restrictions.
The method of data detection at V~ works as follows. During the portion of Tq when VAS is permitted to oscillate, the oscillations commence because of wideband thermal noise inherent to any practical electrical system; this creates a nonzero voltage on VAS, and positive feedback inside the resonator passband ensures noise components at frequencies close to fps are amplified more than those at other frequencies. As a result, the frequency of the built-up oscillation immediately prior to quenching is the same as the natural center frequency of the resonator. If there is coherent energy at the RF input V~. (i.e., a carrier) that falls within the passband of the resonator, then the build-up of resonator oscillations is encouraged: the initial voltage at VAS has a larger magnitude than it would if only noise were present. The time constant of the exponential build-up is determined by the setting of Vq alone, and so it is the same whether or not passband energy on V~ is present; the more energy present on V~, therefore, the greater the final amplitude of the oscillation. Thus, the energy build-up on VAS is proportional to the passband power on V~ and an envelope detectorBPF combination is sufficient to generate a signal proportional to this latter quantity. The envelope detector maintains the subcarrier position of the data relative to the carrier while translating the modulated signal to baseband. Hence, unmodulated signals translate to do and are rejected by the baseband BPF, while the data pass through the BPF. Of course the BPF must be appropriately matched to the data frequency.
Figure 2 illustrates typical waveforms and waveform envelopes during the operation of the receiver, all being time coordinated. Vq represent a periodical control signal for quenching. VAS envelope shows exponential build-ups and decays of oscillation amplitude.
Usual embodiments of SRG receivers use a resonator with a fixed center frequency. They require this center frequency to be set fairly precisely because the resonator passband is very narrow during operation (this improves sensitivity to weak RF signals). Component tolerances are often sufficiently poor that fps can only be set with enough accuracy via mechanical means (for example, 1 S trimming the value of a tunable capacitor by hand) prior to first use of the receiver. Thereafter, fps cannot be changed over the life of the circuit unless it is recalibrated. Manual setting of the resonator frequency is error-prone and expensive; more seriously, fps might drift after calibration, for example, due to component aging or temperature variations. As noted above, the Vq control is operated such that when the resonator is made to oscillate, the band of frequencies to which the oscillator is sensitive is very narrow; even a slight frequency drift can be enough to mean the transmitted data on V~. is no longer within the resonator passband, which means the SRG receiver is no longer capable of receiving the data.
The present invention addresses these problems by the use of the automatic phase/frequency control in general. Its basic concept is applicable to a variety of areas in which phase/frequency control is needed. The invention, however, is described in detail in connection with the SRG in which the resonator center frequency is made tunable (for example, by replacing the capacitor in an LC-based resonator with a varactor), and the AFC of the invention is provided for adjusting f~S with no e:cternal mechanical control. Moreover, the invention provides a means of controlling fps during receiver operation so that the center frequency is held fi:ced, even in the face of mechanisms which would otherwise cause the frequency to drift.
Other advantages, objects and features of the present invention will be readily apparent to those skilled in the art from a review of the following detailed description of preferred embodiments in conjunction with the accompanying drawings and claims.
SUtIMARY OF THE INVENTION
Briefly stated, the invention is directed to a frequency comparison circuit for comparing frequencies of a variable signal and a reference signal. The frequency comparison circuit includes a phase frequency detector for comparing frequencies of the variable signal and the reference signal and for generating an output that depends upon the relationship of the frequencies; and gate modules at the inputs of the phase frequency detector for gating the variable signal and the reference signal so that only a portion of the variable signal and reference signal are repetitively applied to the inputs of the phase frequency detector for processing.
In accordance with another aspect, the invention is directed to a frequency lock loop circuit for maintaining a predetermined frequency relationship between a detected signal and a reference signal. The frequency lock loop circuit includes a variable tuning circuit for adjusting its tuning frequency to generate the detected signal and a frequency comparator for comparing the frequencies of the detected and reference signals and for generating an output responsive to their frequency relationship. The frequency lock loop circuit further includes a gate module for applying repetitively and coincidentally only a predetermined portion of the detected signal and the reference signal to the frequency comparator for generating the output, and a loop circuit connecting the variable tuning circuit and the frequency comparator for applying the output to the variable tuning circuit to adjust its tuning frequency so that the predetermined frequency relationship is maintained between the detected signal and the reference signal.
In accordance with yet a further aspect the invention is directed to an RF
receiver of the superregenerative type for detecting an amplitude shift keyed RF
signal at a predetermined frequency. The RF receiver includes an RF amplifier for amplifying the RF signal, an RF tuning circuit connected to the RF
amplifier and tuned to the RF signal at the predetermined frequency for generating a detected signal, and a quenching circuit attached to the RF tuning circuit for quenching periodically the oscillation of the RF tuning circuit. The RF
receiver further includes an envelope detector connected to the RF tuning circuit for producing amplitude shift keyed data carried on the detected signal, a reference signal generator for generating a reference signal, and a loop module connected to the RF tuning circuit and the reference generator for generating a locking output in response to frequency relationship between the reference signal and the detected signal. In the RF receiver, there are provided further a frequency adjusting circuit connected to the RF tuning circuit for adjusting the predetermined frequency to lock it to the reference frequency, and a gate module for sampling the detected signal and the reference signal for a portion thereof to be inputted to the loop module for generating the locking output.
BRIEF DESCRIPTION OF THE DRAWINGS
Figure 1 is a schematic block diagram of a known SRG receiver.
Figure 2 shows typical shapes of waves and wave envelopes during operation of the SRG receiver shown in Figure 1.
Figure 3 is a schematic block diagram of a SRG receiver according to one embodiment of the invention.
Figure 4 is a gate circuit that can be used in an embodiment of the invention.
Figure 5 is a timing diagram according to an embodiment of the invention.
Figure 6 is another gate circuit that can be used in an embodiment of the invention.
Figure 7 shows waveforms of some signals used to describe the invention.
Figure 8 is a computer simulation result of one embodiment of the invention.
DETAILED DESCRIPTION OF THE INVENTION
An embodiment of the invention as applied to a SRG receiver is shown in the dashed box of Figure 3. Frequency-locked loop (FLL) is known and it is used where frequency and/or phase synchronization must be maintained between two signals over the control bandwidth of the loop. In the figure, two signals are a reference signal and a voltage-controlled oscillator (VCO) signal. The reference signal is generated by a crystal oscillator 30 of frequency f~F, and the VCO
signal is generated by the oscillations of an unquenched SRG resonator (possibly passed through a limiting amplifier 32) with tunable resonant frequency f~S. The VCO
signal is VAS. In some embodiments, either or both of the reference and VCO
signals can be reduced in frequency by dividing by certain factors. As examples, the figure shows dividers as =R (divide-by-R) and =N (divide-by-N) blocks e.g., counters. These (and possibly divided-down) signals are connected to the inputs of a phase/frequency detector (PFD). A PFD circuit is a known circuit which compares the phases of two input signals at its R and V inputs, denoted "R"
and "V" for "reference" and "VCO". If a reference rising edge precedes a VCO
rising edge, an "up" pulse denoted "U" is generated at the U output, while a VCO edge preceding a reference edge generates a "down" ("D") pulse at the D output.
These pulses are used to control the current sources 34 and 36 in a charge-pump circuit whose net current is applied to a loop filter (LF) which includes some kind of charge-storage element e.g., a capacitor, and generates a voltage VLF. This loop filter voltage VLF is a so-called error voltage whose value is used to control the frequency of the resonator by way of a varactor 38. The combination of PFD, charge pump, and LF is connected such that the error voltage is used to bring the reference signal and VCO signal into phase synchrony. The FLL equilibrium condition can be shown to be REF f RES
R _ N (1) As seen from the above equation, the resonator frequency fps can be set by appropriate choice of f~F, R and N. This equilibrium is maintained by the average frequency of the noise in the SRG receiver alone and does not require a data signal present at V~ to maintain frequency control of the resonator.
Referring further for Figure 3, each =R and =N block is a digital circuit which counts positive-going transitions at its input; when the count reaches R
or N, as appropriate, the block's output switches to the opposite binary state (from 0 to 1 or 1 to 0, as appropriate). Often, R and N are integer powers of two and the blocks are implemented as dividers made up of a chain of flip-flops. As described earlier, the =N block receives its input from the resonator signal (VCO signal or VAS), possibly amplified by a limiter circuit, e.g., a block shown by 32. In the case of an SRG receiver, the oscillations of the resonator are periodically quenched by Vq to near-zero levels, after which time they must exponentially (slowly in the beginning) build in amplitude. Therefore, for much of the period of Vq, resonator oscillations have neither sufficient amplitude nor regular-enough zero crossings to reliably drive the =N block. It is only for some small fraction of the quench period just prior to quenching that the resonator oscillations are sufficiently large for the =N block to count correctly. By contrast, the crystal always produces large fixed-amplitude oscillations with regular zero crossings, so there is no danger of the =R block counting incorrectly. Likewise, in cases where there is no =N block, the VCO signal may not have sufficient amplitude to drive PFD correctly.
According to the basic concept of the invention, the VCO signal is gated to ensure that only a portion thereof which is strong enough to drive =N block (or the PFD V input, in the case of no frequency division) correctly is applied to the input. The same gating must be applied to the =R block (or the PFD R input, in g the case of no frequency division) and the outputs of the PFD for generating a proper error signal at VLF.
The preferred embodiment of the invention shown in Figure 3 features a coupling between the FLL enable signal VE;~ (gating signal) and the SRG
resonator O control voltage Vq (VCO signal). Therefore, were it not for t1'~e gating signal V~,,, the combination of correct =R counting and incorrect =N counting (when VAS is too small) would cause equation ( 1 ) not to be satisfied, which in turn would result in the resonator being tuned to a frequency other than the desired one. In the invention, V~,, is controlled such that the divider blocks count only when VAS is of sufficient amplitude to ensure accurate counting, which ensures the relationship in (1) holds and the resonator is tuned to the desired frequency. In this embodiment, V~,, is asserted for a fixed period prior to the quenching of resonator oscillations, then negated at the same instant that quenching is commenced, though it is possible to negate some time prior to the start of quenching. The duty cycles of VEN and Vq need not be related, but the periods of both signals will be the same, namely, Tq.
While the concept described above is sound, a further improvement may be possible. Referring further to Figure 3, such improvements are described.
In the embodiment of Figure 3, no timing relationship between gating signal VE,,, and the reference voltage signal VHF is enforced. Thus, it is possible for V~ to become enabled or disabled at arbitrary phases of a cycle of V~. But this leads to the following subtlety: let us suppose the switch 40 which is controlled by VErr were a simple digital AND gate with inputs V~ and V~ and output VoB, as shown in Figure 4. Then under certain circumstances, it would be possible for an extra count to be erroneously registered. A.n example of those circumstances appears in the timing diagram of Figure 5. If a falling edge of V~,, occurs while V~. is high, and the immediately subsequent rising edge of V~,, also occurs while VHF is high, then an unwanted rising edge is generated on VoB, as shown inside the dotted ellipse in Figure 5. This edge is unwanted because it leads to an incorrect count and hence locking to an improper frequency. One possible means to correct this error is to gate V~ with V~,, such that their output resembles VoG
as shown in Figure ~. An example of a gating circuit which gives this behaviour is shown in Figure 6, though this is by no means the only method to correct the problem. A circuit like Figure 6 can be used for both the VHF and VAS switches 40 and 42 in the preferred embodiment to ensure the correct counts are obtained;
however, a simple AuID gate structure such as Figure 4 will suffice for the V~-controlled switches 44 and 46 at the outputs of the PFD. The essential operation of the invention requires that the FLL be completely disabled when V~,, is negated, then reenabled with the same state as that which existed during the previous enable period when V~ is next asserted.
It was noted earlier that the invention is not required to have fq, the frequency of Vq, to be related to any of the quantities f~F, f~F/R, f~S, or f~s/N. It might appear that this will, under certain conditions, make it impossible for the loop to lock properly because phase continuity is lacking. Although the reference signal is likely to be a square wave, for the moment consider it as a sinusoidal wave so that its division into 360° of phase is more apparent. In Figure 7 depicted is a sinusoidal reference signal and binary VE,,, gating signal. Because the FLL is disabled when V~ is deasserted, V~ may be considered as chopping the reference voltage waveform V~ as depicted in the bottom diagram (it does the same to the resonator voltage VAS). From the FLL's perspective, both reference and resonator voltages appear as a series of segments of continuous waves, and as shown in Figure 7, there is no guarantee that the phase of either signal is the same from the end of one enable period to the start of the next. Even if VHF and V~
were forced into phase continuity by generating them from the same voltage source, there would still be timing fitter, noise, etc., meaning that the reference phase as seen by the FLL would deviate slightly from perfectly continuous. Not only is the reference voltage phase as seen by the FLL potentially discontinuous, but the resonator voltage phase is guaranteed to be discontinuous in an SRG
receiver. When RF input data is absent, resonator oscillations start through thermal noise processes, which means the final oscillation will have a phase that is random and uniformly distributed over the interval [-n, ~] radians. When RF
input data is present, the final resonator oscillation phase tends to align with that of the RF input, but sources of noise unavoidably present inside the resonator bandwidth lead to some deviation of oscillator phase compared to that of the RF input.
It is not the intent of the invention to lock perfectly to the desired frequency f~, but merely for the resonator to be held centered near the correct frequency with a minimum of modulation. The locking frequency is a random variable F with a probability distribution centered at f~ as desired and a standard deviation that is a function of a number of parameters such as the enable duty 10 cycle, the loop filter bandwidth, the charge pump current, etc. Moreover, when fps is far away from f~, the FLL does indeed pull the loop into lock at f~ as determined by equation (1). So long as V~,, is asserted only when the resonator oscillations are of sufficient amplitude to successfully drive the =N block, phase discontinuity can be made not to hinder correct operation of the SRG receiver by appropriate choices of parameters. That is to say, the variance of the locking frequency ~~. can be made small enough such that f~ is always within the passband of the resonator, and that the frequency control loop does not affect the phase of the incoming ASK signal.
In summary, the invention is distinguished from prior art by (a) the addition of an enable signal V~,, whose value gates the inputs to the division blocks as well as the PFD outputs, (b) the sampled nature of the loop, (c) the relaxing of the requirement that input data be present (the invention works when thermal noise alone causes the oscillation), and (d) the relaxing of the usual requirement that a mirror cell be used to control the active filter. Frequency control is done on the filter while operating regardless of the. presence or absence of data.
Figure 8 is a computer simulation of fps as a function of time built with a special-purpose program to study the pull-in and locking behaviour of this sampled FLL. The initial frequency was 305MHz, and f~F = 4MHz, R =32, and N = 2520 were used, meaning from (I) that the expected locking frequency is fps = 3 I SMHz. V~ was asserted for a fraction of Tq given by (3 = 0.13, and it is seen that the loop successfully pulls into lock after about 1.8s. The slew rate of the loop filter voltage in V/s can be shown to be given by SRLF = ~Ip 2C (~) where IP is the charge pump current and in the case of a so-called Type II
loop filter, the kind depicted in Figure 3, C is the sum of the small and large capacitors.
For an initial frequency error, the acquisition time ta~q can be shown to be 2~~f~C
(3) p R
where KR is the tuning gain of the resonator in MHZ/V. Finally, the fitter 6 LF on the loop filter voltage after the loop achieves lock is found to be related to 0.6 2 IpRLFa l 2 TR V
q where 6 ~ is the standard deviation of the time fitter on the reference frequency zero crossings and in the case of a Type II loop filter, RLF is the loop filter resistor.
Numerous modifications, variations, and adaptations may be made to the particular embodiments of the invention described above without departing from the scope of the invention, which is defined in the claims.
Claims (26)
1. A frequency comparison circuit for comparing frequencies of a variable signal and a reference signal comprising:
a phase frequency detector for comparing frequencies of a variable signal and a reference signal and for generating an output that depends upon a relationship of said frequencies;
a gate module including a first gate for gating the variable signal to be inputted to a first input of the phase frequency detector and a second gate for gating the reference signal to be inputted to a second input of the frequency detector;
and a control circuit for controlling the first gate and the second gate so that the variable signal and the reference signal are gated coincidentally and repetitively for a predetermined portion thereof.
a phase frequency detector for comparing frequencies of a variable signal and a reference signal and for generating an output that depends upon a relationship of said frequencies;
a gate module including a first gate for gating the variable signal to be inputted to a first input of the phase frequency detector and a second gate for gating the reference signal to be inputted to a second input of the frequency detector;
and a control circuit for controlling the first gate and the second gate so that the variable signal and the reference signal are gated coincidentally and repetitively for a predetermined portion thereof.
2. The frequency comparison circuit according to claim 1, wherein the predetermined portion of the variable signal having a magnitude sufficient to operate the phase frequency detector.
3. The frequency comparison circuit according to claim 1 or 2, further comprising one or both of the following circuits;
a first divider module for dividing in frequency the variable signal before being inputted to the phase frequency detector, and a second divider circuit for dividing in frequency the reference signal before being inputted to the phase frequency detector.
a first divider module for dividing in frequency the variable signal before being inputted to the phase frequency detector, and a second divider circuit for dividing in frequency the reference signal before being inputted to the phase frequency detector.
4. The frequency comparison circuit according to claim 1, wherein the variable signal and the reference signal are digital in nature and the frequency comparison circuit further comprising one or both of the following circuits;
a ÷N divider circuit for dividing the variable signal before being inputted to the phase frequency detector, and a ÷R divider circuit for dividing the reference signal before being inputted to the phase frequency detector, where N and R are real numbers.
a ÷N divider circuit for dividing the variable signal before being inputted to the phase frequency detector, and a ÷R divider circuit for dividing the reference signal before being inputted to the phase frequency detector, where N and R are real numbers.
5. The frequency comparison circuit according to claim 4, wherein the phase frequency detector is a digital module for comparing frequencies of two digital signals at the first input and the second input and for producing an output signal either at a first output of the phase frequency detector when the frequency of one of the two digital signals is larger than that of the other or at a second output of the phase frequency detector when the frequency relationship is opposite, and said frequency comparison circuit further comprises an output gate module including a first output gate connected to the first output and a second output gate connected to the second output for gating respective outputs from the phase frequency detector.
6. The frequency comparison circuit according to claim 5, further comprising:
a charge circuit at each of the outputs of the phase frequency detector for generating electrical charges in response to the outputs of the first output and the second output of the phase frequency detector, and an output filter connected to the charge circuit for filtering the electrical charge generated thereby to produce a filter output indicative of the frequency relationship of the variable signal and the reference signal.
a charge circuit at each of the outputs of the phase frequency detector for generating electrical charges in response to the outputs of the first output and the second output of the phase frequency detector, and an output filter connected to the charge circuit for filtering the electrical charge generated thereby to produce a filter output indicative of the frequency relationship of the variable signal and the reference signal.
7. The frequency comparison circuit according to any one of claims 1-6, further comprising:
an output gate for gating an output of the phase frequency detector, the control circuit controlling the first gate and the second gate and the output gate so that the variable signal and the reference signal and the output of the phase frequency detector are gated coincidentally and repetitively for a predetermined portion thereof, the predetermined portion of the variable signal having a magnitude sufficient to operate the phase frequency detector.
an output gate for gating an output of the phase frequency detector, the control circuit controlling the first gate and the second gate and the output gate so that the variable signal and the reference signal and the output of the phase frequency detector are gated coincidentally and repetitively for a predetermined portion thereof, the predetermined portion of the variable signal having a magnitude sufficient to operate the phase frequency detector.
8. A frequency lock loop circuit for maintaining a predetermined frequency relationship between a detected signal and a reference signal, comprising:
a variable tuning circuit for adjusting its tuning frequency to generate a detected signal;
a frequency comparator for comparing the frequencies of the detected signal and a reference signal and for generating an output responsive to a relationship of the frequencies;
a gate module for applying repetitively and coincidentally only a predetermined portion of the detected signal and the reference signal to first and second inputs of the frequency comparator for generating the output, said gate module including a first gate for gating the detected signal to be inputted to the first input and a second gate for gating the reference signal to be inputted to the second input, and a loop circuit connecting the variable tuning circuit and the frequency comparator for applying the output to the variable tuning circuit to adjust its tuning frequency so that the predetermined frequency relationship is maintained between the detected signal and the reference signal.
a variable tuning circuit for adjusting its tuning frequency to generate a detected signal;
a frequency comparator for comparing the frequencies of the detected signal and a reference signal and for generating an output responsive to a relationship of the frequencies;
a gate module for applying repetitively and coincidentally only a predetermined portion of the detected signal and the reference signal to first and second inputs of the frequency comparator for generating the output, said gate module including a first gate for gating the detected signal to be inputted to the first input and a second gate for gating the reference signal to be inputted to the second input, and a loop circuit connecting the variable tuning circuit and the frequency comparator for applying the output to the variable tuning circuit to adjust its tuning frequency so that the predetermined frequency relationship is maintained between the detected signal and the reference signal.
9. The frequency lock loop circuit according to claim 8, further comprising:
a detector circuit for detecting an incoming signal at a predetermined frequency to generate the detected signal, the detector circuit having the variable tuning circuit for adjusting the predetermined frequency; and the gate module gating the detected signal and the reference signal only a predetermined portion of each thereof, the detected signal having a magnitude sufficient to operate the frequency comparator during the predetermined portion.
a detector circuit for detecting an incoming signal at a predetermined frequency to generate the detected signal, the detector circuit having the variable tuning circuit for adjusting the predetermined frequency; and the gate module gating the detected signal and the reference signal only a predetermined portion of each thereof, the detected signal having a magnitude sufficient to operate the frequency comparator during the predetermined portion.
10. The frequency lock loop circuit according to claim 9, further comprising:
frequency dividers provided between the gate module and the frequency comparator for dividing the frequencies of the reference signal and the detected signal.
frequency dividers provided between the gate module and the frequency comparator for dividing the frequencies of the reference signal and the detected signal.
11. The frequency lock loop circuit according to claim 9, wherein the detected signal and the reference signal are digital in nature, and the frequency lock loop circuit further comprises one or both of the followings:
a ÷N divider circuit for dividing the detected signal before being applied to the frequency comparator, and a ÷R divider circuit for dividing the reference signal before being applied to the frequency comparator, wherein N and R are real numbers.
a ÷N divider circuit for dividing the detected signal before being applied to the frequency comparator, and a ÷R divider circuit for dividing the reference signal before being applied to the frequency comparator, wherein N and R are real numbers.
12. The frequency lock loop circuit according to any one of claims 9-11, wherein the detector circuit comprises a superregenerative detector having the variable tuning circuit and a quenching circuit for quenching oscillations of the variable tuning circuit.
13. The frequency lock loop circuit according to any one of claims 9-12, further comprising a reference signal generator for generating the reference signal.
14. The frequency lock loop circuit according to claim 13, the reference signal generator comprises a crystal oscillator.
15. The frequency lock loop circuit according to claim 12, wherein the gate module and the quenching circuit are operated at a same repetition rate but with different duty cycles.
16. The frequency lock loop circuit according to any one of claims 9-15, wherein the incoming signal is an RF signal modulated with amplitude-shift keying.
17. The frequency lock loop circuit according to claim 8 further comprising:
a control circuit for controlling the first gate and the second gate so that the detected signal and the reference signal axe gated coincidentally and repetitively for a predetermined portion thereof, the predetermined portion of the detected signal having a magnitude sufficient to operate the frequency comparator.
a control circuit for controlling the first gate and the second gate so that the detected signal and the reference signal axe gated coincidentally and repetitively for a predetermined portion thereof, the predetermined portion of the detected signal having a magnitude sufficient to operate the frequency comparator.
18. The frequency lock loop circuit according to claim 17 further comprising:
an output gate for gating an output of the frequency comparator, and the control circuit controlling the first gate and the second gate and the output gate so that the detected signal and the reference signal and the output of the frequency comparator are gated coincidentally and repetitively for a predetermined portion thereof, the predetermined portion of the detected signal having a magnitude sufficient to operate the frequency comparator.
an output gate for gating an output of the frequency comparator, and the control circuit controlling the first gate and the second gate and the output gate so that the detected signal and the reference signal and the output of the frequency comparator are gated coincidentally and repetitively for a predetermined portion thereof, the predetermined portion of the detected signal having a magnitude sufficient to operate the frequency comparator.
19. An RF receiver of the superregenerative type for detecting an amplitude shift keyed RF signal at a predetermined frequency comprising:
an RF amplifier for amplifying an RF signal;
an RF tuning circuit connected to the RF amplifier and tuned to the RF signal at the predetermined frequency for generating a detected signal;
a quenching circuit attached to the RF tuning circuit for quenching periodically the oscillation of the RF tuning circuit;
an envelope detector connected to the RF tuning circuit for producing amplitude shift keyed data carried on the detected signal;
a reference signal generator for generating a reference signal;
a loop module connected to the RF tuning circuit and the reference signal generator for generating a locking output in response to frequency relationship between the reference signal and the detected signal;
a frequency adjusting circuit connected to the RF tuning circuit for adjusting the predetermined frequency to lock it to a frequency of the reference signal;
and a gate module including a first gate and a second gate, the first gate gating the detected signal and a second gate gating the reference signal, the first and second gates sampling the detected signal and the reference signal repetitively and coincidentally for a portion thereof to be inputted to the loop module for generating the locking output.
an RF amplifier for amplifying an RF signal;
an RF tuning circuit connected to the RF amplifier and tuned to the RF signal at the predetermined frequency for generating a detected signal;
a quenching circuit attached to the RF tuning circuit for quenching periodically the oscillation of the RF tuning circuit;
an envelope detector connected to the RF tuning circuit for producing amplitude shift keyed data carried on the detected signal;
a reference signal generator for generating a reference signal;
a loop module connected to the RF tuning circuit and the reference signal generator for generating a locking output in response to frequency relationship between the reference signal and the detected signal;
a frequency adjusting circuit connected to the RF tuning circuit for adjusting the predetermined frequency to lock it to a frequency of the reference signal;
and a gate module including a first gate and a second gate, the first gate gating the detected signal and a second gate gating the reference signal, the first and second gates sampling the detected signal and the reference signal repetitively and coincidentally for a portion thereof to be inputted to the loop module for generating the locking output.
20. The RF receiver according to claim 19, wherein the loop module further comprises frequency dividers for dividing the frequencies of the detected signal and the reference signal.
21. The RF receiver according to claim 20, further comprising a charge storage device for generating an output charge in response to the locking output.
22. The RF receiver according to claim 21, wherein the RF tuning circuit comprises a voltage controlled oscillator and a frequency adjusting element which is responsive to the output charge from the charge storage device.
23. The RF receiver according to claim 19, wherein the reference signal and the detected signal are digital in nature and the loop module further comprises a phase frequency detector and one or both of the followings:
a ~N divider circuit for dividing the detected signal before being applied to the phase frequency detector, and a ~R divider circuit for dividing the reference signal before being applied to the phase frequency detector, wherein N and R are real numbers.
a ~N divider circuit for dividing the detected signal before being applied to the phase frequency detector, and a ~R divider circuit for dividing the reference signal before being applied to the phase frequency detector, wherein N and R are real numbers.
24. The RF receiver according to any one of claims 19-23 wherein the gate module further comprises a gate at the output of the loop module for sampling the locking output coincidentally with the sampling of the detected signal and the reference signal.
25. The RF receiver according to claim 19, wherein the loop module comprises a phase frequency detector for comparing frequencies of the output of the first gate and the output of the second gate, and a control circuit for controlling the first gate and the second gate so that the detected signal and the reference signal are gated coincidentally and repetitively for a predetermined portion thereof, the predetermined portion of the detected signal having a magnitude sufficient to operate the phase frequency detector.
26. The RF receiver according to claim 25 further comprising:
an output gate for gating an output of the phase frequency detector, the control circuit for controlling the first gate and the second gate and the output gate so that the detected signal and the reference signal and the output of the phase frequency detector are gated coincidentally and repetitively for a predetermined portion thereof, the predetermined portion of the detected signal having a magnitude sufficient to operate the phase frequency detector.
an output gate for gating an output of the phase frequency detector, the control circuit for controlling the first gate and the second gate and the output gate so that the detected signal and the reference signal and the output of the phase frequency detector are gated coincidentally and repetitively for a predetermined portion thereof, the predetermined portion of the detected signal having a magnitude sufficient to operate the phase frequency detector.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| CA 2290862 CA2290862C (en) | 1999-01-27 | 1999-11-25 | A frequency/phase comparison circuit with gated reference and signal inputs |
Applications Claiming Priority (3)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| CA002260456A CA2260456A1 (en) | 1999-01-27 | 1999-01-27 | A frequency-locked loop with gated reference and vco inputs |
| CA2,260,456 | 1999-01-27 | ||
| CA 2290862 CA2290862C (en) | 1999-01-27 | 1999-11-25 | A frequency/phase comparison circuit with gated reference and signal inputs |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| CA2290862A1 CA2290862A1 (en) | 2000-07-27 |
| CA2290862C true CA2290862C (en) | 2004-05-11 |
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| CA 2290862 Expired - Fee Related CA2290862C (en) | 1999-01-27 | 1999-11-25 | A frequency/phase comparison circuit with gated reference and signal inputs |
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| ES2542776T3 (en) | 2011-06-21 | 2015-08-11 | Schneider Electric Industries Sas | Phase comparison device with double connection terminal |
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