August 11, 2015
7 Revision 2.0
hbwhelp@micrel.com or (408) 955-1690
On the other hand, the smaller the value of Rd, the
higher is the overshoot/undershoot on the optical signal
from the laser. In the circuit shown in Figure 4, the RC
compensation network across the driver outputs (MOD+
and MOD-) allows the user Rd = 10Ω. The optical eye
diagrams at data rates of 1.25Gbps, shown in
“Function al Charac ter istics” section, are a ll obtaine d w ith
the same circuit using Rd = 10Ω, RComp = 100Ω, and
CComp = 3pF. The compensation network may change
from one board to another and from one type of laser to
another. An additional compensation network (RC) can
be added at the laser cathode for further compensation
and eye smoothing.
AC-Coupling
When trying to AC-couple the laser to the driver, the
headroom of the driver is no longer a problem since it is
DC isolated f r om the laser with t he c ou pl ing capacitor. At
the output, the headroom of the driver is determined by
the pull-up network. In Figure 4, the modulation current
out of the dr iver is split bet ween the pull -up network and
the laser. If, for example, the total pull-up resistor is
twice the sum of the damping resistor and laser
equivale nt series resis tance, then o nly two thirds (2/3) of
the modulation current will be used by the laser.
Therefore, to keep most of the modulation current going
through the laser, the total pull-up resistor must be kept
as high as possible. One solution involves using an
inductor alone as pull-up, presenting a high impedance
path for the modulation current and zero ohm (0Ω) path
for the DC current offering headroom of the driver equal
to VCC and almost all the modulation current goes into
the laser. The inductor alone will cause signal distortion,
and, to improve this phenomenon, a combination of
resistors and inductors c an be us ed (as s ho wn on Fi gu r e
4). In this case, the headroom of the driver is VCC-R1 x
αIMOD, where αIMOD is the portion of the modulation
current that goes through the pull-up net wor k .
W hen the laser is AC-coup led to the dr iver, the co upling
capacitor creates a low-frequency cutoff in the circuit,
and its va lue must be c hosen to be as lar ge as poss ible.
If the value of the cap is too high, it will slow down the
fast signals edges, and conversely, if its value is too
small, it won’t be able to hold a constant change
between the first bit and the last bit of a long string of
identica l bits in a lo w data r ate applicatio n. This leads to
higher pattern-dependent jitter in the transmitter signal.
0.1µF is found to be good for all applications from
155Mbps to 1.25Gbps.
AC-coupling the laser to the driver brings a solution to
the driver headroom problem at the expense of extra
components, loss of part of the modulation current
wasted in the pull-up network, and additional power
consumption.