Fractional-N type frequency synthesizer

Oscillators – Automatic frequency stabilization using a phase or frequency... – Afc with logic elements

Reexamination Certificate

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C327S105000, C327S291000

Reexamination Certificate

active

06570452

ABSTRACT:

FIELD OF THE INVENTION
This relates to a fractional-N type frequency synthesizer.
BACKGROUND OF THE INVENTION
Frequency synthesizers generate an output signal having a frequency that is a multiple of a reference frequency. In a typical prior art circuit shown in
FIG. 1
which is reproduced from
FIG. 1
of U.S. Pat. No. 3,217,267, the operation of the frequency synthesizer is controlled by a phase lock loop (PLL) in which a variable frequency oscillator
2
is locked to the frequency of a known reference frequency
8
by a phase discriminator
6
. In such arrangement, the oscillator typically is a voltage controlled oscillator (VCO) and the phase discriminator generates an output voltage that is proportional to the phase difference between the known reference frequency and the output of the oscillator. The output voltage of the phase discriminator is applied as an error signal to control the output frequency of the VCO.
To provide for different output frequencies from the VCO, a variable frequency divisor
4
is used to divide the output frequency before it is compared with the reference frequency. As a result, the output frequency from the VCO is an exact multiple of the reference frequency; and, if the divisor is an integer, the smallest increment in the VCO output frequency is equal to the reference frequency. Thus, to provide a small step size between adjacent output frequencies when using an integer divisor, a very low reference frequency is required. A low reference frequency, however, introduces a variety of unacceptable effects.
To avoid the use of a low reference frequency, circuits have been devised for dividing the output frequency by a fractional number. The prior art circuit shown in
FIG. 2
which is
FIG. 1
of U.S. Pat. No. 5,038,117, comprises a voltage controlled oscillator
11
, a fractional divider
13
, a phase comparator
15
and a filter
17
. A control circuit
18
controls the integer component N and the fractional component .F by which the output frequency is divided. As is known in the art, different techniques may be used to effect fractional N division. In one such technique, division by N.F is achieved by averaging the divisor such that the output frequency is divided by N for .F of a duty cycle and by N+1 for (1−.F) of the duty cycle.
Further details concerning such fractional-N frequency synthesizers may be found in U.S. Pat. Nos. 3,217,267 and 5,038,117, which are incorporated herein by reference.
Unfortunately, switching between divisors results in an undesirable phase error or phase jitter near the carrier frequency. Techniques for reducing such phase error are also known and are described in U.S. Pat. No. 4,609,881 and in Steven R. Norsworthy et al. (Ed.) Delta-Sigma Data Converters Theory, Design, and Simulation, IEEE Press (1997), which are incorporated herein by reference, as well as in the above-referenced U.S. Pat. Nos. 3,217,267 and 5,038,117. As shown in
FIG. 3
which is reproduced from FIG. 3.3 of Delta-Sigma Data Converters, a general technique for reducing such phase error is to cascade multiple stages of first or second order Delta-Sigma modulators
310
,
320
,
330
and supply an output of each stage to digital cancellation logic
340
. The general form of each modular stage is shown in
FIG. 4
which is adapted from FIG. 3.1 of Delta-Sigma Data Converters. As shown in
FIG. 4
, the modulator comprises first and second summers
412
,
413
, first and second filters
415
,
419
and a quantizer
417
. Filter
419
connects an output signal, y(n), from quantizer
417
to a negative input of first summer
412
which combines an input signal x(n) with the filtered output and provides the result to an input to filter
415
. An output of filter
415
is provided to an input to quantizer
417
. Second summer
413
calculates the difference between the signals at the input and the output of quantizer
417
to generate a signal, e(n), representing the quantization error of the quantizer. Ideally, for the circuit of
FIG. 3
the noise transfer function is (1−Z
−1
)
m
, where m is the overall order. Such a function has m coincident zeroes at z=1 in the Z-transform plane.
A model of the Delta-Sigma modulator of
FIG. 3
is shown in
FIG. 5
which is reproduced from FIG.
5
(
d
) of the '117 patent. Here, each of three identical stages
510
,
520
,
530
comprises first and second summers
512
,
513
, an integrator
515
, a quantizer
517
and a Z
−1
delay
519
. A digital cancellation logic circuit
540
comprises a first differentiator
542
coupled to the output of the second stage
520
, second and third differentiators
544
,
546
coupled in cascade to the output of the third stage
530
and summer circuitry
550
coupled to the outputs of the first stage
510
, the first differentiator
542
and the third differentiator
546
. A series of error terms arising at different stages of the circuit of
FIG. 5
are canceled when the terms are combined. In particular, following equation
16
of the '117 patent, the combined output of the circuit of
FIG. 5
can be written
O=f
+(1
−Z
−1
)
Q
1
−(1
−Z
−1
)
Q
1
+(1
−Z
−1
)
2
Q
2
−(1
−Z
−1
)
2
Q
2
+(1
−Z
−1
)
3
Q
3
where Q
n
is the quantization error associated with stage n. This equation reduces to
O=f
+(1
−Z
−1
)
3
Q
3
.
As will be recognized by those skilled in the art, this equation has three coincident zeroes at z=1 in the Z-transform plane.
An actual implementation of the Delta-Sigma modulator of
FIG. 5
is shown in FIG.
6
.
Here, each of three identical stages
610
,
620
,
630
comprise an adder
614
and a Z
−1
delay
619
. A digital cancellation logic circuit
640
comprises a first differentiator
642
, coupled to the carry output of adder
614
of the second stage
620
, second and third differentiators
644
,
646
coupled in cascade to the carry output of adder
614
of the third stage
630
and summer circuitry coupled to the carry output of the adder
614
of the first stage
610
, the output of the first differentiator
642
and the output of the third differentiator
646
.
SUMMARY OF THE INVENTION
While prior art circuits of the type shown in
FIGS. 3
,
5
and
6
have better performance than conventional fractional-N synthesizer circuits, there is still a need for even better performance.
We have devised such a circuit. With reference to the Z-transform plane, such better performance is achieved by separating the zeroes in the Z-transform plane. As a result, the spectrum of the noise components of the fractional-N divisor is shifted away from the carrier frequency, thereby reducing the components near the carrier frequency and increasing the components farther away. This is advantageous because it is possible to remove the higher frequency components from the divisor signal by conventional filtering techniques. The model of a circuit for separating the zeroes is similar to that of FIG.
4
and comprises a first summer, first and second filters and a quantizer. The second filter connects an output of the quantizer to the first summer and an output of the summer is connected to an input of the first filter and an output of the first filter is connected to an input to the quantizer. In accordance with the invention, the second filter introduces off-axis zeroes into equations representative of this circuit. In a preferred embodiment, the second filter is realized by first and second delay elements connected in cascade, a multiplier and a second summer. An input to the first delay element is connected to the output of the quantizer and an output of the second delay element is connected to an input to the second summer. An input to the multiplier is connected to a node between the first and second delay elements and an output of the multiplier is connected to an input to the second summer. The second summer subtracts the signal from the second delay element from the signal from the multiplier an

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