Patented clock recovery architecture
Loss of signal detect range: 3 mV to 15 mV
Single reference clock frequency for both native SONET and
15/14 (7%) wrapper rate
Choice of 19.44 MHz, 38.88 MHz, 77.76 MHz, or 155.52 MHz
REFCLK
LVPECL/LVDS/LVCMOS/LVTTL compatible inputs
(LVPECL/LVDS only at 155.52 MHz)
19.44 MHz on-chip oscillator to be used with external crystal
Loss of lock indicator
Loopback mode for high speed test data
Output squelch and bypass features
Single-supply operation: 3.3 V
Low power: 540 mW typical
7 mm × 7 mm, 48-lead LFCSP
APPLICATIONS
SONET OC-48, SDH STM-16, and 15/14 FEC
WDM transponders
Regenerators/repeaters
Test equipment
Backplane applications
FUNCTIONAL BLOCK DIAGRAM
SLICEP/NVCCVEE
IC with Integrated Limiting Amp
ADN2811
PRODUCT DESCRIPTION
The ADN2811 provides the receiver functions of quantization,
signal level detect, and clock and data recovery at OC-48 and
OC-48 FEC rates. All SONET jitter requirements are met,
including jitter transfer, jitter generation, and jitter tolerance. All
specifications are quoted for −40°C to +85°C ambient
temperature, unless otherwise noted.
The device is intended for WDM system applications and can
be used with either an external reference clock or an on-chip
oscillator with external crystal. Both the 2.48 Gb/s and
2.66 Gb/s digital wrapper rates are supported by the ADN2811,
without any change of reference clock.
This device, together with a PIN diode and a TIA preamplifier,
can implement a highly integrated, low cost, low power, fiber
optic receiver.
The receiver front end signal detect circuit indicates when the
input signal level has fallen below a user-adjustable threshold.
The signal detect circuit has hysteresis to prevent chatter at the
output.
The ADN2811 is available in a compact, 7 mm × 7 mm, 48-lead
chip scale package.
CF1CF2
LOL
ADN2811
2
PIN
QUANTIZER
NIN
VREF
Rev. B
Information furnished by Analog Devices is believed to be accurate and reliable.
However, no responsibility is assumed by Analog Devices for its use, nor for any
infringements of patents or other rights of third parties that may result from its use.
Specifications subject to change without notice. No license is granted by implication
or otherwise under any patent or patent rights of Analog Devices. Trademarks and
registered trademarks are the property of their respective owners.
Setup Time TS (See Figure 3) OC-48 140 ps
Hold Time TH (See Figure 3) OC-48 150 ps
REFCLK DC INPUT CHARACTERISTICS
Input Voltage Range @ REFCLKP or REFCLKN 0 VCC V
Peak-to-Peak Differential Input 100 mV
Common-Mode Level DC-Coupled, Single-Ended VCC/2 V
TEST DATA DC INPUT CHARACTERISTICS4 (TDINP/N) CML Inputs
Peak-to-Peak Differential Input Voltage 0.8 V
LVTTL DC INPUT CHARACTERISTICS
Input High Voltage V
Input Low Voltage V
IH
IL
Input Current VIN = 0.4 V or VIN = 2.4 V −5 +5 µA
LVTTL DC OUTPUT CHARACTERISTICS
Output High Voltage VOH, IOH = −2.0 mA 2.4 V
Output Low Voltage VOL, IOL = +2.0 mA 0.4 V
1
PIN and NIN should be differentially driven, ac-coupled for optimum sensitivity.
2
PWD measurement made on quantizer outputs in Bypass mode.
3
Measurement is equipment limited.
4
TDINP/N are CML inputs. If the drivers to the TDINP/N inputs are anything other than CML, they must be ac-coupled.
2.0 V
0.8 V
Rev. B | Page 4 of 20
ADN2811
ABSOLUTE MAXIMUM RATINGS
Table 2.
Parameter Ratings
Supply Voltage (VCC) 5.5 V
Minimum Input Voltage (All Inputs) VEE − 0.4 V
Maximum Input Voltage (All Inputs) VCC + 0.4 V
Maximum Junction Temperature 165°C
Storage Temperature −65°C to +150°C
Lead Temperature (Soldering 10 Sec) 300°C
Stresses above those listed under Absolute Maximum Ratings
may cause permanent damage to the device. This is a stress
rating only; functional operation of the device at these or any
other conditions above those indicated in the operational
section of this specification is not implied. Exposure to absolute
maximum rating conditions for extended periods may affect
device reliability.
ESD CAUTION
ESD (electrostatic discharge) sensitive device. Electrostatic charges as high as 4000 V readily accumulate on
the human body and test equipment and can discharge without detection. Although this product features
proprietary ESD protection circuitry, permanent damage may occur on devices subjected to high energy
electrostatic discharges. Therefore, proper ESD precautions are recommended to avoid performance
degradation or loss of functionality.
THERMAL CHARACTERISTICS
Thermal Resistance
48-lead LFCSP, 4-layer board with exposed paddle soldered
to VCC
1 THRADJ AI LOS Threshold Setting Resistor.
2, 26, 28, Pad VCC P Analog Supply.
3, 9, 16, 19, 22, 27,
VEE P Ground.
29, 33, 34, 42, 43, 46
4 VREF AO Internal VREF Voltage. Decouple to GND with a 0.1 µF capacitor.
5 PIN AI Differential Data Input. CML.
6 NIN AI Differential Data Input. CML.
7 SLICEP AI Differential Slice Level Adjust Input.
8 SLICEN AI Differential Slice Level Adjust Input.
10 LOL DO Loss of Lock Indicator. LVTTL active high.
11 XO1 AO Crystal Oscillator.
12 XO2 AO Crystal Oscillator.
13 REFCLKN DI Differential REFCLK Input. LVTTL, LVCMOS, LVPECL, LVDS (LVPECL, LVDS only at 155.52 MHz).
14 REFCLKP DI Differential REFCLK Input. LVTTL, LVCMOS, LVPECL, LVDS (LVPECL, LVDS only at 155.52 MHz).
15 REFSEL DI Reference Source Select. 0 = on-chip oscillator with external crystal; 1 = external clock source, LVTTL.
17 TDINP AI Differential Test Data Input.
18 TDINN AI Differential Test Data Input.
20, 47 VCC P Digital Supply.
21 CF1 AO Frequency Loop Capacitor.
23 REFSEL1 DI Reference Frequency Select (See Table 5) LVTTL.
24 REFSEL0 DI Reference Frequency Select (See Table 5) LVTTL.
25 CF2 AO Frequency Loop Capacitor.
30 RATE DI Data Rate Select (See Table 4) LVTTL.
31, 32 NC DI No Connect.
35, 36 VCC P Output Driver Supply.
37 DATAOUTN DO Differential Retimed Data Output. CML.
38 DATAOUTP DO Differential Retimed Data Output. CML.
39 SQUELCH DI Disable Clock and Data Outputs. Active high. LVTTL.
40 CLKOUTN DO Differential Recovered Clock Output. CML.
41 CLKOUTP DO Differential Recovered Clock Output. CML.
44 BYPASS DI Bypass CDR Mode. Active high. LVTTL.
45 SDOUT DO Loss of Signal Detect Output. Active high. LVTTL.
48 LOOPEN DI Enable Test Data Inputs. Active high. LVTTL.
1
Type: P = Power, AI = Analog Input, AO = Analog Output, DI = Digital Input, DO = Digital Output
Rev. B | Page 6 of 20
ADN2811
CLKOUTP
T
S
T
H
DATAOUTP/N
OUTP
OUTN
OUTP–OUTN
0V
03019-B-003
Figure 3. Output Timing
18
16
14
12
10
mV
8
6
4
2
0
0100
THRADJ RESISTOR VS. LOSTRIP POINT
1020 30405060708090
RESISTANCE (kΩ)
03019-B-004
Figure 4. LOS Comparator Trip Point Programming
V
CML
V
SE
V
DIFF
V
SE
03019-B-005
Figure 5. Single-Ended vs. Differential Output Specs
Rev. B | Page 7 of 20
ADN2811
S
DEFINITION OF TERMS
MAXIMUM, MINIMUM, AND TYPICAL
SPECIFICATIONS
Specifications for every parameter are derived from statistical
analyses of data taken on multiple devices from multiple wafer
lots. Typical specifications are the mean of the distribution of
the data for that parameter. If a parameter has a maximum (or a
minimum), that value is calculated by adding to (or subtracting
from) the mean six times the standard deviation of the
distribution. This procedure is intended to tolerate production
variations. If the mean shifts by 1.5 standard deviations, the
remaining 4.5 standard deviations still provide a failure rate of
only 3.4 parts per million. For all tested parameters, the test
limits are guardbanded to account for tester variation and
therefore guarantee that no device is shipped outside of data
sheet specifications.
SINGLE-ENDED VS. DIFFERENTIAL
AC-coupling is typically used to drive the inputs to the
quantizer. The inputs are internally dc biased to a commonmode potential of ~0.6 V. Driving the ADN2811 single-ended
and observing the quantizer input with an oscilloscope probe at
the point indicated in Figure 7 shows a binary signal with an
average value equal to the common-mode potential and
instantaneous values both above and below the average value. It
is convenient to measure the peak-to-peak amplitude of this
signal and call the minimum required value the quantizer
sensitivity. Referring to Figure 6, since both positive and
negative offsets need to be accommodated, the sensitivity is
twice the overdrive.
10mV p-p
VREF
INPUT SENSITIVITY AND INPUT OVERDRIVE
Sensitivity and overdrive specifications for the quantizer involve
offset voltage, gain, and noise. The relationship between the
logic output of the quantizer and the analog voltage input is
shown in Figure 6. For a sufficiently large positive input voltage,
the output is always Logic 1; similarly for negative inputs, the
output is always Logic 0. However, the transitions between
output Logic Levels 1 and 0 are not at precisely defined input
voltage levels but occur over a range of input voltages. Within
this zone of confusion, the output may be either 1 or 0, or it may
even fail to attain a valid logic state. The width of this zone is
determined by the input voltage noise of the quantizer. The
center of the zone of confusion is the quantizer input offset
voltage. Input overdrive is the magnitude of signal required to
guarantee the correct logic level with 1 × 10
OUTPUT
1
0
OFFSET
OVERDRIVE
SENSITIVITY
(2× OVERDRIVE)
Figure 6. Input Sensitivity and Input Overdrive
NOISE
−10
confidence level.
INPUT (V p-p)
03019-B-006
SCOPE
PROBE
Figure 7. Single-Ended Sensitivity Measurement
COPE
PROBE
Figure 8. Differential Sensitivity Measurement
PIN
VREF
VREF
5mV p-p
PIN
NIN
ADN2811
50Ω 50Ω
ADN2811
50Ω 50Ω
+
QUANTIZER
+
QUANTIZER
VREF
03019-B-007
03019-B-008
Driving the ADN2811 differentially (see Figure 8), sensitivity
seems to improve by observing the quantizer input with an
oscilloscope probe. This is an illusion caused by the use of a
single-ended probe. A 5 mV p-p signal appears to drive the
ADN2811 quantizer. However, the single-ended probe measures
only half the signal. The true quantizer input signal is twice this
value since the other quantizer input is complementary to the
signal being observed.
Rev. B | Page 8 of 20
ADN2811
LOS RESPONSE TIME
The LOS response time is the delay between the removal of the
input signal and the indication of loss of signal (LOS) at
SDOUT. The LOS response time of the ADN2811 is 300 ns typ
when the inputs are dc-coupled. In practice, the time constant
of the ac-coupling at the quantizer input determines the LOS
response time.
Jitter Tolerance
Jitter tolerance is defined as the peak-to-peak amplitude of the
sinusoidal jitter applied on the input signal that causes a 1 dB
power penalty. This is a stress test that is intended to ensure no
additional penalty is incurred under the operating conditions
(see Figure 10). Figure 11 shows the typical OC-48 jitter
tolerance performance of the ADN2811.
JITTER SPECIFICATIONS
The ADN2811 CDR is designed to achieve the best bit-errorrate (BER) performance, and has exceeded the jitter generation,
transfer, and tolerance specifications proposed for SONET/SDH
equipment defined in the Telcordia Technologies specification.
Jitter is the dynamic displacement of digital signal edges from
their long-term average positions measured in UI (unit
intervals), where 1 UI = 1 bit period. Jitter on the input data
can cause dynamic phase errors on the recovered clock
sampling edge. Jitter on the recovered clock causes jitter on the
retimed data.
The following sections briefly summarize the specifications of
jitter generation, transfer, and tolerance in accordance with the
Telcordia document (GR-253-CORE, Issue 3, September 2000)
for the optical interface at the equipment level and the
ADN2811 performance with respect to those specifications.
Jitter Generation
Jitter generation specification limits the amount of jitter that
can be generated by the device with no jitter and wander
applied at the input. For OC-48 devices, the band-pass filter has
a 12 kHz high-pass cutoff frequency with a roll-off of
20 dB/decade and a low-pass cutoff frequency of at least
20 MHz. The jitter generated should be less than 0.01 UI rms
and 0.1 UI p-p.
Jitter Transfer
Jitter transfer function is the ratio of the jitter on the output
signal to the jitter applied on the input signal versus the
frequency. This parameter measures the limited amount of jitter
on an input signal that can be transferred to the output signal
(see Figure 9).
0.1
15
SLOPE = –20dB/DECADE
1.5
0.15
INPUT JITTER AMPLITUDE (UI)
100
AMPLITUDE (UI p- p)
0.1
ٛ
f
0
Figure 10. SONET Jitter Tolerance Mask
10
1
101k100k10M
Figure 11. OC-48 Jitter Tolerance Curve
f
1
JITTER FREQUENCY (Hz)
OC-48 SONET MASK
10010k1M1
MODULATION FREQUENCY (Hz)
f2f
3
ADN2811
f
4
03019-B-010
03019-B-011
JITTER GAIN (dB)
ACCEPTABLE
RANGE
f
C
JITTER FREQUENCY (kHz)
Figure 9. Jitter Transfer Curve
SLOPE = –20dB/DECADE
03019-B-009
Rev. B | Page 9 of 20
ADN2811
T
A
A
THEORY OF OPERATION
The ADN2811 is a delay-locked 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 that 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 the
input jitter. A separate phase control loop, comprised of the
VCO, tracks the low frequency components of the input jitter.
The initial frequency of the VCO is set by yet a third loop,
which compares the VCO frequency with the reference
frequency and sets the coarse tuning voltage. The jitter tracking
phase-locked loop controls the VCO by the fine tuning control.
The delay-locked and phase-locked 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 also 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. Since the loop filter is an integrator,
the static phase error is driven to zero.
psh
INPUT
DAT A
RECOVERED
d = PHASE DETEC
o = VCO GAIN
c = LOOP INTEGR
psh = PHASE SHIFTER GAIN
n = DIVIDE R
OR GAIN
TOR
TIO
Figure 12. PLL/DLL Architecture
CLOCK
e(s)X(s)
d/sc
Z(s)
JITTERTRANSFER FUNCTION
Z(s)
X(s)
TRACKING ERRORTRANSFER FUNCTION
e(s)
X(s)
o/s
=
cn
2
s
+ s +1
do
=
d psh
s2 + s+
1
s
c
n psh
o
2
do
cn
03019-B-012
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
since the jitter transfer function, Z(s)/X(s), provides the narrowband jitter filtering.
Another view of the circuit is that the phase shifter implements
the zero required for the frequency compensation of a secondorder phase-locked loop, and this zero is placed in the feedback
path and therefore does not appear in the closed-loop transfer
function. Jitter peaking in a conventional second-order phaselocked loop is caused by the presence of this zero in the closedloop transfer function. Since this circuit has no zero in the
closed-loop transfer, jitter peaking is minimized.
The delay- and phase-locked loops together simultaneously
provide wideband jitter accommodation and narrow-band jitter
filtering. The linearized block diagram in Figure 12 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 the main PLL loop has low jitter peaking (see Figure 13),
which makes this circuit ideal for signal regenerator
applications where jitter peaking in a cascade of regenerators
can contribute to hazardous jitter accumulation.
The delay- and phase-locked loops contribute to overall jitter
accommodation. 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, so the phase shifter remains close to the
center of its range, and therefore contributes little to the low
frequency jitter accommodation.
At medium jitter frequencies, the gain and tuning range of the
VCO are not large enough to track the input jitter. In this case,
the VCO control voltage becomes large and saturates, and the
VCO frequency dwells at one or the other extreme of its tuning
range. The size of the VCO tuning range therefore has only a
small effect on the jitter accommodation. The delay-locked loop
control voltage is now larger; thus the phase shifter takes on the
burden of tracking input jitter. The phase shifter range, in UI,
can be seen as a broad plateau on the jitter tolerance curve. The
phase shifter has a minimum range of 2 UI at all data rates.
Rev. B | Page 10 of 20
ADN2811
The gain of the loop integrator is small for high jitter
frequencies, so larger phase differences are needed to make the
loop control voltage big enough to tune the range of the phase
shifter. Large phase errors at high jitter frequencies cannot be
tolerated. In this region, the gain of the integrator determines
the jitter accommodation. Since the gain of the loop integrator
declines linearly with frequency, jitter accommodation is lower
with higher jitter frequency. At the highest frequencies, the loop
gain is very small and little tuning of the phase shifter can be
expected. In this case, jitter acc ommodation is determined by
the eye opening of the input data, the static phase error, and the
residual loop jitter generation. Jitter accommodation is roughly
0.5 UI in this region. The corner frequency between the
declining slope and the flat region is the closed-loop bandwidth
of the delay-locked loop, which is roughly 5 MHz.
JITTER PEAKING
IN ORDINARY PLL
JITTER
GAIN
(dB)
d psh
o
n psh
Figure 13. Jitter Response vs. Conventional PLL
c
ADN2811
Z(s)
X(s)
f
(kHz)
03019-B-013
Rev. B | Page 11 of 20
ADN2811
FUNCTIONAL DESCRIPTION
CLOCK AND DATA RECOVERY
The ADN2811 recovers clock and data from serial bit streams at
OC-48 as well as the 15/14 FEC rates. The data rate is selected
by the RATE input (see Table 4).
Table 4. Data Rate Selection
RATE Data Rate Frequency (MHz)
0 OC-48 2488.32
1 OC-48 FEC 2666.06
LIMITING AMPLIFIER
The limiting amplifier has differential inputs (PIN/NIN) that
are internally terminated with 50 Ω to an on-chip voltage reference (VREF = 0.6 V typically). These inputs are normally
ac-coupled, although dc coupling is possible as long as the input
common-mode voltage remains above 0.4 V (see Figure 22,
Figure 23, and Figure 24). Input offset is factory trimmed to
achieve better than 4 mV typical sensitivity with minimal drift.
The limiting amplifier can be driven differentially or singleended.
SLICE ADJUST
The quantizer slicing level can be offset by ±100 mV to mitigate
the effect of amplified spontaneous emission (ASE) noise by
applying a differential voltage input of ±0.8 V to SLICEP/N
inputs. If no adjustment of the slice level is needed, SLICEP/N
should be tied to VCC.
LOSS OF SIGNAL (LOS) DETECTOR
The receiver front end level signal detect circuit indicates when
the input signal level has fallen below a user adjustable
threshold. The threshold is set with a single external resistor
from Pin 1, THRADJ, to GND. The LOS comparator trip point
versus the resistor value is illustrated in Figure 4 (this is only
valid for SLICEP = SLICEN = VCC). If the input level to the
ADN2811 drops below the programmed LOS threshold,
SDOUT (Pin 45) indicates the loss of signal condition with a
Logic 1. The LOS response time is ~300 ns by design, but is
dominated by the RC time constant in ac-coupled applications.
If the LOS detector is used, the quantizer slice adjust pins must
both be tied to VCC. This is to avoid interaction with the LOS
threshold level.
Note that it is not expected to use both LOS and slice adjust at
the same time; systems with optical amplifiers need the slice
adjust to evade ASE. However, a loss of signal in an optical link
that uses optical amplifiers causes the optical amplifier output
to be full-scale noise. Under this condition, the LOS would not
detect the failure. In this case, the loss of lock signal indicates
the failure because the CDR circuitry is unable to lock onto a
signal that is full-scale noise.
REFERENCE CLOCK
There are three options for providing the reference frequency to
the ADN2811: differential clock, single-ended clock, or crystal
oscillator. See Figure 14, Figure 15, and Figure 16 for example
configurations.
ADN2811
REFCLKP
BUFFER
REFCLKN
VCC
VCC
VCC
Figure 14. Differential REFCLK Configuration
VCC
CLK
OSC
19.44MHz
REFCLKP
OUT
REFCLKN
NC
VCC
VCC
VCC
Figure 15. Single-Ended REFCLK Configuration
VCC
REFCLKP
NC
REFCLKN
XO1
XO2
Figure 16. Crystal Oscillator Configuration
XO1
XO2
XO1
XO2
REFSEL
100kΩ 100kΩ
CRYSTAL
OSCILLATOR
REFSEL
ADN2811
100kΩ 100kΩ
CRYSTAL
OSCILLATOR
REFSEL
ADN2811
100kΩ 100kΩ
CRYSTAL
OSCILLATOR
BUFFER
BUFFER
VCC/2
VCC/2
VCC/2
03019-B-014
03019-B-015
003019-B-016
Rev. B | Page 12 of 20
ADN2811
The ADN2811 can accept any of the following reference clock
frequencies: 19.44 MHz, 38.88 MHz, 77.76 MHz at LVTTL/
LVCMOS/LVPECL/LVDS levels, or 155.52 MHz at LVPECL/
LVDS levels via the REFCLKN/P inputs, independent of data
rate. The input buffer accepts any differential signal with a
peak-to-peak differential amplitude of greater than 100 mV
(e.g., LVPECL or LVDS) or a standard single-ended low voltage
TTL input, providing maximum system flexibility. The
appropriate division ratio can be selected using the REFSEL0/1
pins, according to Table 5. Phase noise and duty cycle of the
reference clock are not critical, and 100 ppm accuracy is
sufficient.
Table 5. Reference Frequency Selection
Applied Reference
REFSEL REFSEL[1..0]
Frequency (MHz)
1 00 19.44
1 01 38.88
1 10 77.76
1 11 155.52
0 XX
REFCLKP/N Inactive. Use 19.44 MHz
XTAL oscillator on Pins XO1, XO2 (Pull
REFCLKP to VCC).
An on-chip oscillator to be used with an external crystal is also
provided as an alternative to using the REFCLKN/P inputs.
Details of the recommended crystal are given in Table 6.
Table 6. Required Crystal Specifications
Parameter Value
Mode Series Resonant
Frequency/Overall Stability 19.44 MHz ±100 ppm
Frequency Accuracy ±100 ppm
Temperature Stability ±100 ppm
Aging ±100 ppm
ESR 50 Ω max
REFSEL must be tied to VCC when the REFCLKN/P inputs are
active, or tied to VEE when the oscillator is used. No connection
between the XO pin and REFCLK input is necessary (see
Figure 14, Figure 15, and Figure 16). Note that the crystal should
operate in series resonant mode, which renders it insensitive to
external parasitics. No trimming capacitors are required.
LOCK DETECTOR OPERATION
The lock detector monitors the frequency difference between
the VCO and the reference clock and deasserts the loss of lock
signal when the VCO is within 500 ppm of center frequency
(see Figure 17). This enables the phase loop, which pulls the
VCO frequency in the remaining amount and also acquires
phase lock. Once locked, if the input frequency error exceeds
1000 ppm (0.1%), the loss of lock signal is reasserted and
control returns to the frequency loop, which reacquires and
maintains a stable clock signal at the output.
The frequency loop requires a single external capacitor between
CF1 and CF2. The capacitor specification is given in Table 7.
Table 7. Recommended C
Parameter Value
Temperature Range −40°C to +85°C
Capacitance >3.0 µF
Leakage <80 nA
Rating >6.3 V
Capacitor Specification
F
LOL
1
100050005001000f
Figure 17. Transfer Function of LOL
Rev. B | Page 13 of 20
VCO
(ppm)
ERROR
03019-B-017
ADN2811
ADN2811
PIN
NIN
VREF
+
QUANTIZER
50Ω 50Ω
50Ω 50Ω
VCC
TDINP/NLOOPEN BYPASS
Figure 18. Test Modes
SQUELCH MODE
When the squelch input is driven to a TTL high state, both the
clock and data outputs are set to the zero state to suppress
downstream processing. If desired, this pin can be directly
driven by the LOS detector output, SDOUT. If the squelch
function is not required, the pin should be tied to VEE.
TEST MODES: BYPASS AND LOOPBACK
When the bypass input is driven to a TTL high state, the
quantizer output is connected directly to the buffers driving the
data out pins, thus bypassing the clock recovery circuit (see
Figure 18). This feature can help the system deal with
nonstandard bit rates.
0
CDR
FROM
QUANTIZER
1
OUTPUT
RETIMED
DATACLK
10
DATAOUTP/NCLKOUTP/N SQUELCH
03019-B-018
The loopback mode can be invoked by driving the LOOPEN
pin to a TTL high state, which facilitates system diagnostic
testing. This connects the test inputs (TDINP/N) to the clock
and data recovery circuit (per Figure 18). The test inputs have
internal 50 Ω terminations and can be left floating when not in
use. TDINP/N are CML inputs and can only be dc-coupled
when being driven by CML outputs. The TDINP/N inputs must
be ac-coupled if being driven by anything other than CML
outputs. Bypass and loopback modes are mutually exclusive.
Only one of these modes can be used at any given time. The
ADN2811 is put into an indeterminate state if the BYPASS and
LOOPEN pins are set to Logic 1 at the same time.
Rev. B | Page 14 of 20
ADN2811
APPLICATIONS INFORMATION
PCB DESIGN GUIDELINES
Proper RF PCB design techniques must be used for optimal
performance.
Power Supply Connections and Ground Planes
Use of one low impedance ground plane to both analog and
digital grounds is recommended. The VEE pins should be
soldered directly to the ground plane to reduce series
inductance. If the ground plane is an internal plane and
connections to the ground plane are made through vias,
multiple vias may be used in parallel to reduce the series
inductance, especially on Pins 33 and 34, which are the ground
returns for the output buffers.
Use of a 10 µF electrolytic capacitor between VCC and GND is
recommended at the location where the 3.3 V supply enters the
PCB. 0.1 µF and 1 nF ceramic chip capacitors should be placed
between IC power supply VCC and GND as close as possible to
the ADN2811’s VCC pins. Again, if connections to the supply
and ground are made through vias, the use of multiple vias in
parallel helps to reduce series inductance, especially on Pins 35
and 36, which supply power to the high speed CLKOUTP/N
and DATAOUTP/N output buffers. Refer to the schematic in
Figure 19 for recommended connections.
Transmission Lines
Use of 50 Ω transmission lines is required for all high frequency
input and output signals to minimize reflections, including PIN,
NIN, CLKOUTP, CLKOUTN, DATAOUTP, and DATAOUTN
(also REFCLKP, REFCLKN for a 155.2 MHz REFCLK). It is also
recommended that the PIN/NIN input traces are matched in
length and that the CLKOUTP/N and DATAOUTP/N output
traces are matched in length. All high speed CML outputs,
CLKOUTP/N and DATAOUTP/N, also require 100 Ω back
termination chip resistors connected between the output pin
and VCC. These resistors should be placed as close as possible
to the output pins. These 100 Ω resistors are in parallel with
on-chip 100 Ω termination resistors to create a 50 Ω back
termination (see Figure 20).
The high speed inputs, PIN and NIN, are internally terminated
with 50 Ω to an internal reference voltage (see Figure 21). A
0.1 µF capacitor is recommended between VREF, Pin 4, and
GND to provide an ac ground for the inputs.
As with any high speed mixed-signal design, care should be
taken to keep all high speed digital traces away from sensitive
analog nodes.
Soldering Guidelines for Chip-Scale Package
The lands on the 48-lead LFCSP are rectangular. The printed
circuit board pad for these should be 0.1 mm longer than the
package land length and 0.05 mm wider than the package land
width. The land should be centered on the pad. This ensures
that the solder joint size is maximized. The bottom of the chip
scale package has a central exposed pad. The pad on the printed
circuit board should be at least as large as this exposed pad. The
user must connect the exposed pad to analog VCC.
If vias are used, they should be incorporated into the pad at
1.2 mm pitch grid. The via diameter should be between 0.3 mm
and 0.33 mm, and the via barrel should be plated with 1 oz.
copper to plug the via.
Rev. B | Page 15 of 20
ADN2811
VCC
TRANSMISSION
LINES
VCC
36
VCC
35
VEE
34
VEE
33
NC
32
NC
31
RATE
30
VEE
29
VCC
28
VEE
27
VCC
26
CF2
25
µC
50Ω
CLKOUTP
CLKOUTN
DATAOUTP
DATAOUTN
1nF
µC
1nF
4.7µF
(SEETABLE 7 FOR SPECS)
VCC
0.1µF
0.1µF
VCC
VCC
VCC
TIA
0.1µF
50Ω
50Ω
10µF
C
IN
VCC
µC
19.44MHz
R
1nF
0.1µF
TH
THRADJ
VCC
VEE
VREF
PIN
NIN
SLICEP
SLICEN
VEE
LOL
XO1
XO2
4 × 100Ω
µC
1nF0.1µF
LOOPEN
VCC
VEE
SDOUT
BYPASS
VEE
VEE
CLKOUTP
CLKOUTN
48 47 46 45 44 43 42 41 40 39 38 37
1
2
3
4
5
6
7
8
9
10
11
ADN2811
12
13 14 15 16 17 18 19
REFCLKN
NC
REFSEL
REFCLKP
VCC
EXPOSED PAD
TIED OFFTO
VCC PLANE
WITH VIAS
1nF
VEE
TDINP
TDINN
NC
NC
0.1µF
20 21 22 23 24
CF1
VEE
VCC
DATAOUTP
SQUELCH
VEE
REFSEL1
µC
DATAOUTN
REFSEL0
VCC
1nF
0.1µF
03019-B-019
Figure 19. Typical Application Circuit
VCC
C
0.1µ F
IN
C
IN
TIA
50Ω
50Ω
Figure 21. AC-Coupled Input Configuration
ADN2811
PIN
NIN
50Ω50Ω
VREF
03019-B-021
100Ω
VCC
100Ω
VCC
100Ω 100Ω
0.1µ F
0.1µ F
50Ω
50Ω
ADN2811
Figure 20. AC-Coupled Output Configuration
V
V
TERM
TERM
50Ω
50Ω
03019-B-020
Rev. B | Page 16 of 20
ADN2811
CHOOSING AC-COUPLING CAPACITORS
The choice of ac-coupling capacitors at the input (PIN, NIN)
and output (DATAOUTP, DATAOUTN) of the ADN2811 must
be chosen carefully. When choosing the capacitors, the time
constant formed with the two 50 Ω resistors in the signal path
must be considered. When a large number of consecutive
identical digits (CIDs) are applied, the capacitor voltage can
drop due to baseline wander (see Figure 22), causing pattern
dependent jitter (PDJ).
For the ADN2811 to work robustly at OC-48, a minimum
capacitor of 0.1 µF to PIN/NIN and 0.1 µF on DATAOUTP/
DATAOUTN should be used. This is based on the assumption
that 1000 CIDs must be tolerated and that the PDJ should be
limited to 0.01 UI p-p.
C
IN
V2V1
PIN
TIA
1
V1
V1b
V2
V2b
V
DIFF
V
= V2–V2b
DIFF
VTH = ADN2811 QUANTIZERTHRESHOLD
NOTES
1. DURING DATAPATTERNS WITH HIGH TRANSITION DENSITY, DIFFERENTIAL DC VOLTAGEAT V1 AND V2 IS 0.
2. WHENTHE OUTPUT OFTHE TIA GOESTO CID, V1 AND V1b ARE DRIVEN TO DIFFERENT DC LEVELS. V2 AND V2b DISCHARGE TOTHE V
WHICH EFFECTIVELY INTRODUCES A DIFFERENTIAL DC OFFSET ACROSS THE AC COUPLING CAPACITORS.
3. WHENTHE BURST OF DATA STARTS AGAIN,THE DIFFERENTIAL DC OFFSET ACROSSTHE AC COUPLING CAPACITORS IS APPLIEDTOTHE INPUT LEVELS,
CAUSING A DC SHIFT INTHE DIFFERENTIAL INPUT. THIS SHIFT IS LARGE ENOUGH SUCHTHAT ONE OFTHE STATES, EITHER HIGH OR LOW DEPENDING ON
THE LEVELS OF V1 AND V1bWHENTHE TIA WENT TO CID, IS CANCELLED OUT. THE QUANTIZERWILL NOT RECOGNIZETHIS AS AVALID STATE.
4. THE DC OFFSET SLOWLY DISCHARGES UNTILTHE DIFFERENTIAL INPUT VOLTAGE EXCEEDSTHE SENSITIVITY OFTHE ADN2811. THE QUANTIZERWILL BE
ABLETO RECOGNIZE BOTH HIGH AND LOW STATES ATTHIS POINT.
C
V2bV1b
IN
50Ω
50Ω
NIN
ADN2811
+
V
LIMAMPCDR
REF
C
OUT
DATAOUTP
C
OUT
DATAOUTN
432
V
REF
VTH
LEVEL,
REF
Figure 22. Example of Baseline Wander
03019-B-022
Rev. B | Page 17 of 20
ADN2811
DC-COUPLED APPLICATION
The inputs to the ADN2811 can also be dc-coupled. This may
be necessary in burst mode applications where there are long
periods of CIDs and baseline wander cannot be tolerated. If the
inputs to the ADN2811 are dc-coupled, care must be taken not
to violate the input range and common-mode level
requirements of the ADN2811 (see Figure 23, Figure 24, and
Figure 25). If dc-coupling is required and the output levels of
the TIA do not adhere to the levels shown in Figure 24 and
Figure 25, there needs to be level shifting and/or an attenuator
between the TIA outputs and the ADN2811 inputs.
LOL TOGGLING DURING LOSS OF INPUT DATA
If the input data stream is lost due to a break in the optical link
(or for any reason), the clock output from the ADN2811 stays
within 1000 ppm of the VCO center frequency as long as there
is a valid reference clock. The LOL pin toggles at a rate of
several kHz because the LOL pin toggles between a Logic 1 and
a Logic 0 while the frequency loop and phase loop swap control
of the VCO. The chain of events is as follows:
• The ADN2811 is locked to the input data stream; LOL = 0.
• The input data stream is lost due to a break in the link. The
VCO frequency drifts until the frequency error is greater
than 1000 ppm. LOL is asserted to a Logic 1 as control of
the VCO is passed back to the frequency loop.
•The frequency loop pulls the VCO to within 500 ppm of its
center frequency. Control of the VCO is passed back to the
phase loop and LOL is deasserted to a Logic 0.
•The phase loop tries to acquire, but there is no input data
present so the VCO frequency drifts.
•The VCO frequency drifts until the frequency error is
greater than 1000 ppm. LOL is asserted to a Logic 1 as
control of the VCO is passed back to the frequency loop.
This process is repeated until a valid input data stream is
re-established.
V
= 1.2V MAX
SE
NIN
Figure 25. Maximum Allowed DC-Coupled Input Levels