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MAX3676 データシートの表示(PDF) - Maxim Integrated

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MAX3676 Datasheet PDF : 15 Pages
First Prev 11 12 13 14 15
622Mbps, 3.3V Clock-Recovery and
Data-Retiming IC with Limiting Amplifier
Reduced Power Consumption
Without the Limiting Amplifier
The limiting amplifier is biased independently from the
clock recovery circuitry. Grounding INSEL turns off the
limiting amplifier and selects the PECL DDI inputs.
Converting Average Optical Power
to Signal Amplitude
Many of the MAX3676’s specifications relate to input-
signal amplitude. When working with fiber optic
receivers, the input is usually expressed in terms of
average optical power and extinction ratio. The rela-
tions given in Table 2 and Figure 6 are helpful for con-
verting optical power to input signal when designing
with the MAX3676.
In an optical receiver, the input voltage to the limiting
amplifier can be found by multiplying the relationship in
Table 2 by the photodiode responsivity and transim-
pedance amplifier gain.
Optical Hysteresis
Power and hysteresis are often expressed in decibels.
By definition, decibels are always 10log (power). At the
inputs to the MAX3676 limiting amplifier, the power is
VIN2/R. If a receiver’s optical input power (x) increases
by a factor of two, and the preamplifier is linear, then the
voltage at the input to the MAX3676 also increases by a
factor of two.
The optical power increase is:
10log(2x/x) = 10log(2) = +3dB
At the MAX3676, the voltage increase is:
( ) 10log
2VIN 2/ R
VIN2/ R
= 10log(2 2) = 20log(2) = +6dB
Table 2. Optical-Power Relations*
PARAMETER SYMBOL
RELATION
Average
Power
PAVG
( ) PAVG = P0 + P1 / 2
Extinction
Ratio
re
re = P1 / P0
Optical Power
of a “1”
P1
P1
=
2PAVG
re
re + 1
Optical Power
of a “0”
P0
( ) P0 = 2PAVG / re +1
Signal
Amplitude
PIN
( ) PIN = P1P0 = 2PAVG
re 1
re + 1
*Assuming a 50% average input-data duty cycle.
In an optical receiver, the decibel change at the
MAX3676 always equals 2x the optical decibel change.
The MAX3676’s typical voltage hysteresis is 3.0dB. This
provides an optical hysteresis of 1.5dB.
Jitter in Optical Receivers
Timing jitter, edge speeds, aberrations, optical disper-
sion, and attenuation all impact the performance of
high-speed clock recovery for SDH/SONET receivers
(Figure 7). These effects decrease the time available
for error-free data recovery by reducing the received
“eye opening” of nonreturn-to-zero (NRZ) transmitted
signals.
P1
PAVE
P0
TIME
Figure 6. Optical Power Relations
EYE DIAGRAM WITH NO TIMING JITTER
MIDPOINT
TIME
MIDPOINT
EFFECTS OF TIMING JITTER ON EYE DIAGRAM
TIME
Figure 7. Eye Diagram With and Without Timing Jitter
______________________________________________________________________________________ 11

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