ADN2814 Analog Devices, Inc., ADN2814 Datasheet - Page 14

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ADN2814

Manufacturer Part Number
ADN2814
Description
Continuous Rate 10 Mb/s To 675 Mb/s Clock And Data Recovery Ic With Integrated Limiting Amp
Manufacturer
Analog Devices, Inc.
Datasheet
ADN2814
THEORY OF OPERATION
The ADN2814 is a delay- and phase-locked loop circuit for
clock recovery and data retiming from an NRZ encoded data
stream. The phase of the input data signal is tracked by two
separate feedback loops, which share a common control voltage.
A high speed delay-locked loop path uses a voltage controlled
phase shifter to track the high frequency components of input
jitter. A separate phase control loop, comprised of the VCO,
tracks the low frequency components of input jitter. The initial
frequency of the VCO is set by yet a third loop that compares
the VCO frequency with the input data frequency and sets the
coarse tuning voltage. The jitter tracking phase-locked loop
controls the VCO by the fine-tuning control.
The delay and phase loops together track the phase of the input
data signal. For example, when the clock lags input data, the
phase detector drives the VCO to a higher frequency and
increases the delay through the phase shifter; both of these
actions serve to reduce the phase error between the clock and
data. The faster clock picks up phase, while the delayed data
loses phase. Because the loop filter is an integrator, the static
phase error is driven to zero.
Another view of the circuit is that the phase shifter implements
the zero required for frequency compensation of a second-order
phase-locked loop, and this zero is placed in the feedback path
and, thus, does not appear in the closed-loop transfer function.
Jitter peaking in a conventional second-order phase-locked loop
is caused by the presence of this zero in the closed-loop transfer
function. Because this circuit has no zero in the closed-loop
transfer, jitter peaking is minimized.
The delay and phase loops together simultaneously provide
wideband jitter accommodation and narrow-band jitter
filtering. The linearized block diagram in Figure 17 shows that
the jitter transfer function, Z(s)/X(s), is a second-order low-pass
providing excellent filtering. Note that the jitter transfer has no
zero, unlike an ordinary second-order phase-locked loop. This
means that the main PLL loop has virtually zero jitter peaking
(see Figure 18). This makes this circuit ideal for signal regen-
erator applications, where jitter peaking in a cascade of
regenerators can contribute to hazardous jitter accumulation.
The error transfer, e(s)/X(s), has the same high-pass form as an
ordinary phase-locked loop. This transfer function is free to be
optimized to give excellent wideband jitter accommodation,
because the jitter transfer function, Z(s)/X(s), provides the
narrow-band jitter filtering.
Rev. 0 | Page 14 of 28
INPUT
d = PHASE DETECTOR GAIN
o = VCO GAIN
c = LOOP INTEGRATOR
psh = PHASE SHIFTER GAIN
n = DIVIDE RATIO
The delay and phase loops contribute to overall jitter accom-
modation. At low frequencies of input jitter on the data signal,
the integrator in the loop filter provides high gain to track large
jitter amplitudes with small phase error. In this case, the VCO is
frequency modulated, and jitter is tracked as in an ordinary
phase-locked loop. The amount of low frequency jitter that can
be tracked is a function of the VCO tuning range. A wider
tuning range gives larger accommodation of low frequency
jitter. The internal loop control voltage remains small for small
phase errors; therefore, the phase shifter remains close to the
center of its range and thus contributes little to the low
frequency jitter accommodation.
DATA
X(s)
Figure 18. ADN2814 Jitter Response vs. Conventional PLL
RECOVERED
CLOCK
Figure 17. ADN2814 PLL/DLL Architecture
Z(s)
n psh
o
e(s)
psh
FREQUENCY (kHz)
JITTER TRANSFER FUNCTION
Z(s)
X(s)
TRACKING ERROR TRANSFER FUNCTION
X(s)
e(s)
=
=
d/sc
s
s
d psh
2
2
+
cn
do
c
JITTER PEAKING
IN ORDINARY PLL
s
d psh
1/n
+
s
c
s
2
1
n psh
o
+
o/s
do
cn
+ 1
ADN2814
Z(s)
X(s)

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