Phase locked loop having DC bias circuitry

Miscellaneous active electrical nonlinear devices – circuits – and – Signal converting – shaping – or generating – Synchronizing

Reexamination Certificate

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C327S159000

Reexamination Certificate

active

06466068

ABSTRACT:

BACKGROUND OF THE INVENTION
1. Technical Field
The present invention is directed to the field of phase locked loops. More specifically, the invention provides an improved phase locked loop (“PLL”) that includes a DC bias circuit. The DC bias circuit enables the PLL to operate using a single supply voltage, and also may be used to eliminate the phase discrimination “dead zone” normally associated with the phase detector element of the PLL.
2. Description of the Related Art
Phase locked loops are well-known elements in analog and digital circuit design. A phase locked loop operates by receiving an external reference clock signal and generating a localized oscillator signal that is synchronized with the external reference clock signal. The local oscillator signal may operate at the same frequency as the reference clock signal or at some integer multiple of that frequency. A general description of the theory and operational characteristics of a PLL is contained in Couch,
Digital and Analog Communication Systems,
Fourth Edition, pp. 289-296.
FIG. 1
is a circuit diagram of a known PLL circuit
10
. This circuit
10
includes four primary elements—a phase detector
14
, an operational amplifier
26
, a voltage controlled oscillator (VCXO)
32
, and a counter
36
. This circuit
10
generates a local oscillator signal (PLL clock)
34
that is synchronized with an external reference clock signal
12
, but which operates at a higher frequency than the external reference clock
12
. This is accomplished by feeding back a divided down version
38
of the local oscillator signal
34
to the phase detector
14
, which then compares the phases of the reference clock signal
12
with the feedback signal
38
.
The phase detector
14
is preferably a phase frequency detector, and has two inputs and two outputs. The two inputs of the phase detector
14
are coupled to the external reference clock signal
12
and the PLL feedback signal
38
, and the two outputs
16
A,
16
B are coupled to the operational amplifier
26
. If the PLL feedback signal
38
leads in phase with respect to the reference clock signal
12
, then the phase detector
14
outputs a pulse on the negative phase output (ph−)
16
A. Similarly, if the reference clock signal
12
leads in phase with respect to the PLL feedback signal
38
, then the phase detector
14
outputs a pulse on the positive phase output (ph+)
16
B. These output pulses on the positive and negative phase outputs
16
A,
16
B from the phase detector
14
are characterized by a pulse width that is equivalent to the phase difference between the two inputs.
When the phase difference between the reference clock signal
12
and the PLL feedback signal
38
is nearly zero degrees (i.e., when the PLL is “locked”), then the phase detector enters an operational region in which it cannot discriminate the phase difference between the two input signals. This operational region is referred to herein as the “dead zone.” As the phase difference of the two inputs approaches zero degrees, the phase detector
14
outputs minimum-width pulses on both the positive and negative phase outputs
16
A,
16
B.
The phase detector outputs
16
A,
16
B are coupled to the operational amplifier
26
through a pair of RC circuits. These RC circuits configure the operational amplifier
26
as an integrator. The negative phase output (ph−)
16
A is coupled to the negative input of the operational amplifier
26
through the RC circuit composed of resistors
18
,
28
and capacitor
30
. And the positive phase output (ph+)
16
B is coupled to the positive input of the operational amplifier
26
through the RC circuit composed of resistors
20
,
22
and capacitor
24
.
This integrator
18
-
30
receives the pulses from the phase detector outputs (ph+, ph−)
16
A,
16
B and generates a voltage level at its output that is proportional to the pulse width of the phase pulses. This phase voltage is then provided as an input to the voltage controlled oscillator (VCXO)
32
. Because these phase pulses are typically very narrow, particularly when the reference clock signal
12
is very nearly in phase with the PLL feedback signal
38
, the voltage output of the operational amplifier is typically near ground. For this reason, the operational amplifier
26
is typically powered using two power supply voltages, such as +/−12 volts or +/−15 volts. This is done because the operational amplifier
26
output becomes non-linear as the output voltage approaches the power supply rails. Thus, it does not operate effectively from a single supply voltage, such as +5V, where the other supply rail is ground, since the phase voltage is typically very close to ground when the PLL is in the locked condition.
The voltage controlled oscillator
32
generates an output clock signal, PLL clock
34
, which is characterized by a frequency that is proportional to the phase voltage from the integrator. This clock signal, PLL clock
34
, is the localized oscillator signal that is synchronized with the external reference clock
12
. The PLL clock signal
34
is then fed back to one of the inputs of the phase detector
14
either directly, or via a counter
36
.
The counter
36
is configured as a divide-by-N counter, and it generates the PLL feedback signal
38
, which is a frequency divided version of the PLL clock signal
34
. By selecting an appropriate value of N, a circuit designer can select the frequency of the PLL clock signal
34
with respect to the external reference clock
12
. For example, if the circuit designer desires to generate a synchronized version of the reference clock signal
12
, but at a frequency 10 times greater than the reference clock signal
12
, then the value of N would be
10
.
FIG. 2
is a timing diagram showing the operation of the PLL set forth in FIG.
1
. This timing diagram sets forth, from top to bottom, the PLL clock signal
34
, the reference clock signal
12
, the PLL feedback signal
38
, and the corresponding phase pulse signals on the positive and negative phase outputs
16
B,
16
A of the phase detector
14
. As seen in this diagram, during normal operation (i.e., when the PLL is locked), the PLL clock signal
34
is in phase with the reference clock
12
, but at a higher frequency. The PLL feedback signal
38
is nearly identical to the external reference clock signal
12
when the circuit is locked, and is in phase with this signal. When locking occurs, the phase difference between the PLL feedback signal
38
and the reference clock signal
12
is very small, and the phase detector
14
enters the “dead zone” region in which it cannot further discriminate between the phase difference of the two input signals
12
,
38
. In this region, the phase detector
14
outputs two extremely narrow pulses at the positive and negative phase outputs
16
B,
16
A, during the rising edge of the input clocks
12
,
38
.
The circuit shown in
FIG. 1
suffers from two problems. The first problem relates to the dead zone. As described above, at some point during the locking of the PLL, the phase difference between the reference clock signal
12
and the feedback signal
38
becomes so small that the phase detector
14
cannot determine which signal is leading or lagging the other signal. This dead zone region thus presents a minimum threshold phase difference below which the PLL cannot properly lock. Although the characteristics of the phase detector circuitry
14
generally determine the extent of the dead zone region, the minimum threshold difference represented by this region may also be affected by component variations and tolerances in the external RC elements
18
-
24
,
28
-
30
of the integrator.
The second problem with the circuit shown in
FIG. 1
relates to the operational amplifier
26
power scheme. As described above, because the positive and negative phase outputs
16
A,
16
B of the phase detector
14
are typically very narrow pulses, particularly as the PLL approaches a locked condition, the output voltage of the int

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