1.5 ns Rise/2.0 ns Fall Times
Output Current: 180 mA @ 3 V, 200 mA @ 2.5 V
Bias Current: 90 mA @ 3 V
Modulation Current: 60 mA @ 3 V
Offset Current: 30 mA @ 3 V
Single +5 V Power Supply
Switching Rate: 200 MHz
Onboard Light Power Control Loops
APPLICATIONS
Laser Printers and Copiers
Optical Disk Drives
FO Datacomm
GENERAL DESCRIPTION
The AD9660 is a highly integrated driver for laser diode applications such as optical disk drives, printers, and copiers. The
AD9660 gets feedback from an external photo detector and includes two analog feedback loops to allow users to set “bias”
and “write” (for optical disk drives) power levels of the laser,
and switch between the two power levels at up to 200 MHz.
Output rise and fall times are typically 1.5 ns and 2.0 ns to
complement printer applications that use image enhancing techniques such as pulse width modulation to achieve gray scale,
and allow disk drive applications to improve density and take
advantage of pulsed write formats. Control signals are TTL/
CMOS compatible.
with Light Power Control
AD9660
FUNCTIONAL BLOCK DIAGRAM
WRITE
PULSE
WRITE
CALIBRATE
WRITE
LEVEL
BIAS
LEVEL
BIAS
CAL
TRANSIMPEDANCE
BIAS
T/H
V:1T/H
AMPLIFIER
V:1
OUTPUT
DRIVER
OUTPUT
DRIVER
AD9660
The driver output provides up to 180 mA of current @ 3 V,
90 mA of BIAS current, 60 mA of modulation current, and
30 mA of offset current. The onboard disable circuit turns off
the output drivers and returns the light power control loops to a
safe state.
The AD9660 can also be used in closed loop applications in
which the output power level follows an analog WRITE LEVEL
voltage input. By optimizing the external hold capacitor, and
the photo detector, the write loop can achieve bandwidths as
high as 25 MHz.
The AD9660 is offered in a 28-pin plastic SOIC for operation
over the commercial temperature range (0°C to +70°C).
OUTPUT
SENSE
INPUT
PHOTO
DETECTOR
DIODE
LASER
DIODE
REV. 0
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
which may result from its use. No license is granted by implication or
otherwise under any patent or patent rights of Analog Devices.
Maximum Pulse RateIV+25°C200250MHz3 dB Reduction in I
OUT
Output Propagation Delay (tPD), Rising1IVFull1.63.0ns
Output Propagation Delay (t
Output Current Rise Time
Output Current Fall Time
WRITE CAL Aperture Delay
Disable Time
I+25°C1.551.751.90V
Temperature CoefficientV–0.2mV/°C
Output CurrentV+25°C–0.51.0mA
SENSE IN
Current GainV+25°C1.85mA/mA
VoltageI+25°C3.74.04.3VI
MONITOR
= 2 mA
Input ResistanceV+25°C<150Ω
POWER SUPPLY (DISABLE = HIGH)
+V
VoltageI+25°C4.755.005.25VDISABLE = HIGH
S
CurrentI+25°C75110150mA
+V
S
Power DissipationI+25°C550mW
OFFSET CURRENT
OFFSET SET VoltageI+25°C1.11.41.7VI
NOTES
1
Propagation delay measured from the 50% of the rising/falling transition of WRITE PULSE to 50% point of the rising/falling edge of the output modulation current.
2
Rise time measured between the 10% and 90% points of the rising transition of the modulation current.
3
Fall time measured between the 10% and 90% points of the falling transition of the modulation current.
4
Aperture Delay is measured from the 50% point of the rising edge of WRITE PULSE to the time when the output modulation begins to recalibrate, WRITE CAL is
held during this test.
5
Disable Time is measured from the 50% point of the rising edge of DISABLE to the 50% point of the falling transition of the output current. Fall time during disable
is similar to fall time during normal operation.
Absolute maximum ratings are limiting values, to be applied individually, and
beyond which the serviceability of the circuit may be impaired. Functional
operability under any of these conditions is not necessarily implied. Exposure of
absolute maximum rating conditions for extended periods of time may affect
device reliability.
2
Typical thermal impedance is θJA = 45°C/W, θJC = 41°C/W.
ORDERING GUIDE
ModelTemperature RangePackage Option
AD9660KR0°C to +70°CR-28
AD9660KR-REEL 0°C to +70°CR-28 (1000/reel)
PIN ASSIGNMENTS
EXPLANATION OF TEST LEVELS
Test Level
I.100% Production Tested.
II. 100% production tested at +25°C, and sample tested at
specified temperatures. AC testing done on sample basis.
III. Sample Tested Only.
IV. Parameter is guaranteed by design and characterization
testing.
V. Parameter is a typical value only.
VI. All devices are 100% production tested at +25°C, sample
tested at temperature extremes.
WRITE CAL
WRITE PULSE
WRITE LEVEL
V
REF
WRITE HOLD
GROUND
+V
SENSE IN
GAIN
POWER MONITOR
+V
GROUND
BIAS HOLD
BIAS LEVEL
S
S
1
2
3
4
5
6
7
8
9
10
11
12
13
14
AD9660KR
TOP VIEW
(Not to Scale)
28
OFFSET PULSE
27
OFFSET SET
26
GROUND
25
+V
S
24
OUTPUT
23
+V
S
22
OUTPUT
21
+V
S
20
OUTPUT
+V
19
S
OUTPUT
18
17
GROUND
DISABLE
16
15
BIAS CAL
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 the AD9660 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.
Equivalent Circuits
REV. 0
–3–
Page 4
AD9660
PIN DESCRIPTIONS
PinFunction
OUTPUTAnalog laser diode current output. Connect to anode of laser diode, cathode connected to GROUND externally.
BIAS LEVELAnalog voltage input, V
tion as follows:
BIAS CALTTL/CMOS compatible, Bias loop T/H control signal. Logic HIGH enables calibration mode, and the bias loop
T/H immediately goes into track mode. Logic LOW disables the bias loop T/H and immediately places it in hold
mode. WRITE PULSE should be held logic LOW while calibrating. Floats logic HIGH.
BIAS HOLDExternal hold capacitor for the bias loop T/H. Approximate droop in the bias current while BIAS CAL is logic
LOW is:
±∆I
BIAS
=
WRITE PULSETTL/CMOS compatible, current control signal. Logic HIGH supplies I
LOW turns I
MODULATION
WRITE CALTTL/CMOS compatible, write loop T/H control signal. Logic HIGH enables calibration mode; before enabling
calibration the bias loop should be calibrated and OFFSET PULSE driven to an appropriate state. In calibration
mode, 13 ns after the WRITE PULSE goes logic HIGH, the write loop T/H goes into track mode (there is no delay if WRITE PULSE is HIGH before WRITE CAL transitions to a HIGH level). The write loop T/H immediately goes into hold mode when the WRITE PULSE goes Logic LOW. WRITE CAL LOW disables the write
loop T/H and places it in hold mode. Floats logic HIGH.
WRITE LEVELAnalog voltage input, V
I
tion as follows:
MONITOR
REF
18 ×10
C
to V
+ 1.6 V. Bias current is set proportional to the BIAS LEVEL during calibra-
REF
I
MONITOR
–9
t
BIAS HOLD
BIAS HOLD
off. Floats logic HIGH.
REF
to V
=
+1.6 V. Write current is set proportional to the input voltage during calibra-
REF
V
WRITE LEVEL−VREF
1. 85 ×(R
GAIN
V
BIAS LEVEL−VREF
=
1. 85 × R
+50 Ω
()
GAIN
. Bandwidth of the loop is:
+ 50 Ω)
BW =
2π (550 Ω)C
MODULATION
1
BIAS HOLD
to the laser diode. Logic
WRITE HOLDExternal hold capacitor for the write loop T/H. Approximate droop in I
−9
±∆I
logic LOW is:
MODULATED
BW =
2π (550 Ω) C
1
BIAS HOLD
SENSE INAnalog current input, I
MONITOR
18 ×10
=
, from PIN photo detector diode. SENSE IN should be connected to the cathode
t
WRITE HOLD
C
WRITE HOLD
. Bandwidth of the loop is:
MODULATION
current while WRITE CAL is
of the PIN diode, with the PIN anode connected to GROUND or a negative voltage. Voltage at SENSE IN varies slightly with temperature and current, but is typically 4.0 V.
GAINExternal connection for the feedback network of the transimpedance amplifier. External feedback network, R
and C
, should be connected between GAIN and POWER MONITOR. See text for choosing values.
GAIN
GAIN
POWEROutput voltage monitor of the internal feedback loop. Voltage is proportional to feedback current from photo
MONITORdiode.
OFFSETSet resistor connection for the offset current source. Resistor between OFFSET CURRENT SET and +V
S
CURRENT SET determines offset current level. The input voltage at this node varies slightly with temperature and current, but is
typically 1.4 V. See curves. Can also be driven with a current out DAC.
OFFSETTTL/CMOS compatible, OFFSET current control signal. Logic HIGH adds I
PULSEturns off I
. Floats logic HIGH.
OFFSET
OFFSET
to I
. Logic LOW
OUT
DISABLETTL/CMOS compatible, current output disable circuit. Logic LOW for normal operation; logic HIGH disables
the current outputs to the laser diode, and drives the voltage on the hold capacitors close to V
(minimizes the
REF
output current when the device is re-enabled). DISABLE floats logic HIGH.
V
+V
REF
S
Analog Voltage Output, internal bandgap voltage reference, ~1.75 V, provided to user for power level offset.
Positive Power Supply. Nominally +5 V, pin connections should be tied together externally.
GROUNDGround Reference. All grounds should be tied together externally.
–4–
REV. 0
Page 5
6.25mV
–193.8mV
OUTPUT
AD9660
20mV
ML64116R
PHOTO DETECTOR
–120V
ANTEL
ARS1
50Ω
2ns
TEK 11802
O'SCOPE
50Ω
Figure 1. Driving ML64116R Laser @ 30 mW
Typical Performance Characteristics–AD9660
35
30
25
20
OFFSET
I
15
10
5
0
0255101520
Figure 2. I
R
OFFSET
OFFSET
– kΩ
vs. R
OFFSET
THEORY OF OPERATION
The AD9660 combines a very fast output current switch with
onboard analog light power control loops to provide the user
with a complete laser diode driver solution. The block diagram
illustrates the key internal functions. The control loops of the
AD9660, the bias loop and the write loop, adjust the output
current level, I
I
MONITOR
, out of SENSE IN is proportional to the analog input
, so that the photo diode feedback current,
OUT
voltage at BIAS LEVEL or WRITE LEVEL. Since the monitor
WRITE HOLD
5pF
5pF
V
V
REF
REF
AD9660
V:1
TZA
V:1
C
GAIN
DISABLE
WRITE PULSE
WRITE CAL
WRITE LEVEL
GAIN
R
GAIN
POWER
MONITOR
BIAS LEVEL
BIAS CAL
BIAS HOLD
OFFSET PULSE
TTL
TTL
TTL
ANALOG
ANALOG
ANALOG
TTL
TTL
DISABLE
CIRCUIT
*
DELAY
50
Figure 3. Functional Block Diagram
current is proportional to the laser diode light power, the loops
effectively control laser power to a level proportional to the analog inputs. The control loops should be periodically calibrated
independently (see Choosing C
BIAS HOLD
and C
WRITE HOLD
).
The offset current generator produces an open loop output current, I
a current out DAC (see Figure 2). While I
. Its level is controlled by an external set resistor or
OFFSET
OFFSET
is not calibrated as the currents from the bias and write loops are, it can
be very versatile (see Offset Current below).
2* I
V
REF
MONITOR
VOLT
I
MODULATION
1:10
1.85:1
1:10
1:10
REF
I
BIAS
I
OFFSET
V
REF
OUTPUT
SENSE IN
4.0V
I
MONITOR
OFFSET CURRENT
1.4V
I
OUT
OUT
WRITE LOOP
PHOTO
DETECTOR
SET
*
10ns DELAY ON RISING
EDGE; 0ns ON FALLING
LASER
DIODE
BIAS LOOP
+V
S
REV. 0–5–
Page 6
AD9660
LASER
POWER-UP
OR LASER
NOT IN USE
CALIBRATED WRITE
CALIBRATED BIAS
BIAS
CAL
TIME
WRITE
LOOP
CAL
TIME
WRITE LOOP
HOLD TIME
LASER POWER
MODULATED
BETWEEN
BIAS AND WRITE LEVELS
RECALIBRATE THE BIAS LOOP
RECALIBRATE WRITE LOOP
DISABLE
BIAS CAL
WRITE CAL
WRITE PULSE
OUTPUT POWER
Figure 4. Normal Operating Mode
The disable circuit turns off I
and returns the hold capacitor
OUT
voltages to their minimum levels (minimum output current)
when DISABLE = logic HIGH. It is used during initial powerup of the AD9660 or during time periods when the laser is inactive. When the AD9660 is re-enabled the control loops must be
recalibrated.
Normal operation of the AD9660 involves (in order, see figure):
1. The AD9660 is enabled (DISABLE = logic LOW).
2. The input voltages (BIAS LEVEL and WRITE LEVEL) are
driven to the appropriate levels to set the calibrated laser diode output power levels.
3. The bias loop is closed for calibration (BIAS CAL = logic
HIGH), and then opened (BIAS CAL = logic LOW).
4. The write loop is closed for calibration (WRITE PULSE and
WRITE CAL = logic HIGH) and then opened.
5. While both loops are open, the laser is pulsed between the
two calibrated levels by WRITE PULSE.
6. The bias and write loops are periodically recalibrated as
needed.
7. The AD9660 is disabled when the laser will not be pulsed for
an indefinite period of time.
Control Loop Transfer Functions
The relationship between I
V
I
MONITOR
BIAS LEVEL−VREF
=
1. 85 ×(R
MONITOR
GAIN
and V
+50 Ω)
BIAS LEVEL
is
once the bias loop is calibrated. When the bias loop is open
(BIAS CAL = logic LOW), its output current, I
, is propor-
BIAS
tional to the held voltage at BIAS HOLD; the external hold capacitor on this pin determines the droop error in the output bias
current between calibrations.
The relationship between I
V
I
MONITOR
WRITE LEVEL−VREF
=
1. 85 ×(R
MONITOR
GAIN
and V
+50 Ω)
WRITE LEVEL
is
once the write loop is calibrated. The current supplied by the write
loop output is referred to as the modulation current, I
MODULATION
.
When the write loop is open (WRITE CAL logic LOW),
I
MODULATION
is proportional to the held voltage at WRITE HOLD.
The external hold capacitor (WRITE HOLD) determines the
droop error between calibrations. I
MODULATION
may be switched
on and off by WRITE PULSE when the write loop is open.
4
0°C CASE
3
2
OPTICAL OUTPUT – mW
1
0
CONSTANT WRITE POWER
BIAS CALIBRATION POWER
012020406080100
FORWARD CURRENT – mA
BIAS
MOD
25°C
CASE
50°C CASE
Figure 5. Typical Laser Diode Current-to-Optical
Power Curve
The sections below discuss choosing the external components in
the feedback loops for a particular application.
Choosing R
The gain resistor, R
GAIN
, allows the user to match the feedback
GAIN
loop’s transfer function to the laser diode/photo diode
combination.
The user should define the maximum laser diode output power
for the intended application, P
photo diode monitor current, I
ode transfer function is illustrated in Figure 5. R
1. 6 V
MONITOR MAX
chosen as:
R
GAIN
=
1. 85 × I
The laser diode’s output power will then vary from 0 to P
for an input range of V
REF
to V
, and the corresponding
LD MAX
MONITOR MAX
+1.6 V @ the BIAS LEVEL
REF
. A typical laser di-
should be
GAIN
−50 Ω
.
LD MAX
and WRITE LEVEL inputs.
–6–
REV. 0
Page 7
AD9660
Minimum specifications for I
choosing R
. Users are cautioned that laser diode/photo di-
GAIN
MONITOR MAX
should be used when
ode combinations that produce monitor currents that are less
than I
MONITOR MAX
in the equation above will produce higher laser output power than predicted, which may damage the laser
diode. Such a condition is possible if R
is calculated using
GAIN
typical instead of minimum monitor current specifications. In
that case the input range to the AD9660 BIAS LEVEL and
WRITE LEVEL inputs should be limited to avoid damaging
laser diodes.
Although not recommended, another approach would be to
use a potentiometer for R
the value of R
for each laser diode/photo diode combina-
GAIN
. This allows users to optimize
GAIN
tion’s monitor current. The drawback to this approach is that
potentiometer’s stray inductance and capacitance may cause the
transimpedance amplifier to overshoot and degrade its settling,
and the value of C
may not be optimized for the entire
GAIN
potentiometer’s range.
C
optimizes the response of the transimpedance amplifier
GAIN
and should be chosen as from the table below. Choosing C
GAIN
larger than the recommended value will slow the response of the
amplifier. Lower values improve TZA bandwidth but may cause
the amplifier to oscillate.
Table I.
Recommended
R
GAIN
C
GAIN
≥2.5 kΩ2 pF
1.5 kΩ3 pF
1 kΩ4 pF
500 Ω8 pF
The circuit in Figure 6 allows an adjustable gain with low variance in bandwidth, but requires several external components.
R
INTERNAL
50Ω
C
EQ
R
EQ
V
I
MONITOR
SENSE
IN
1:2
AD9660
2I PIN
V
REF
R
INTERNAL
50Ω
MONITOR
EQUIVALENT
CIRCUIT
GAIN
POWER
V
REF
REF
R1
R2
REQ + 50Ω = (RF + 50Ω)
C1
R
F
R3
1.7kΩ
C
F
R2R1R1
(1+ + )
R
F
Choosing C
BIAS HOLD
Choosing values for the hold capacitors, C
and C
WRITE HOLD
WRITE
and C
HOLD
, is a
tradeoff between output current droop when the control loops
are open, and the time it takes to calibrate and recalibrate the
laser power when the loops are closed.
The amount of output current droop is determined by the value
of the hold capacitor and the leakage current at that node.
When either of the two control loops are open (WRITE CAL or
BIAS CAL logic LOW), the pin connections for the hold
capacitors (WRITE HOLD and BIAS HOLD) are high imped-
ance inputs. Leakage currents will range from ±200 nA; this
low current minimizes the droop in the output power level. As-
suming the worst case current of ±200 nA, the output current
will change as follows:
−9
±∆I
BIAS
±∆I
MODULATED
18 ×10
=
t
C
BIAS HOLD
18 ×10
=
BIAS HOLD
−9
t
WRITE HOLD
C
WRITE HOLD
To choose a value, the user will need to determine the amount
of time the loop will be in hold mode, t
WRITE HOLD
or t
BIAS HOLD
,
the maximum change in laser output power the application can
tolerate, and the laser efficiency (defined as the change in laser
output power to the change in laser diode current). As an ex-
ample, if an application requires 5 mW of laser power ±5%, and
the laser diode efficiency is 0.25 mW/mA, then
∆I
= 5 mW ×(5%) / 0.25
MAX
mW
mA
=1. 0 mA
If the same application had a hold time requirement of 250 µs,
then the minimum value of the hold capacitor would be:
−9
C
HOLD
18 ×10
=
×250 µs
1. 0 mA
= 4.5 nF
When determining the calibration time, the T/H and the external hold capacitor can be modeled using the simple RC circuit
illustrated in Figure 7.
WRITE LEVEL
OR BIAS LEVEL
POWER MONITOR
AD9660
T/H
TZA
R
WRITE HOLD
OR BIAS HOLD
C
HOLD
EXTERNAL HOLD
CAPACITOR
Figure 7. Circuit Model for Determining Calibration Times
REV. 0
Figure 6. Adjustable Gain Configuration
–7–
Page 8
AD9660
100
Using this model, the voltage at the hold capacitor is
−t
V
C
HOLD
= V
t = 0
+(V
t =∞
− V
t = 0
)1−e
τ
where t0 is when the calibration begins (WRITE CAL or BIAS
CAL goes logic HIGH), V
t = 0, V
is the steady state voltage at the hold cap with the
Initial calibration is required after power-up or any other time
the laser has been disabled. Disabling the AD9660 drives the
hold capacitors back down to V
. In this case, or in any case
REF
where the output current is more than 10% out of calibration, R
will range from 300 Ω to 550 Ω for the model above; the higher
value should be used for calculating the worst case calibration
time. Following the example above, if C
were chosen as
HOLD
4.5 nF, then τ = RC = 550 Ω × 4.5 nF would be 2.5 µs. For an
initial calibration error <1%, the initial calibration time should
be >5τ = 12.4 µs.
Initial calibration time will actually be better than this calculation indicates, as a significant portion of the calibration time will
be within 10% of the final value, and the output resistance in
the AD9660’s T/H decreases as the hold voltage approaches its
final value.
Recalibration is functionally identical to initial calibration, but
the loop need only correct for droop. Because droop is assumed
to be a small percentage of the initial calibration (<10%), the
resistance for the model above will be in the range of 75 Ω to
140 Ω. Again, the higher value should be used to estimate the
worst case time needed for recalibration.
Continuing with the example above, since the error during hold
time was chosen as 5%, we meet the criteria for recalibration
and τ = RC = 140 Ω × 4.5 nF = 0.63 µs. To get a final error of
1% after recalibration, the 5% droop must be corrected to
within a 20% error (20% × 5% = 1%). A 2τ recalibration time
of 1.26 µs is sufficient.
Continuous Recalibration
In applications where the hold capacitor is small (<500 pF) and
the WRITE PULSE signals always have a pulse width >25 ns,
the user may continuously calibrate the write loop. In such an
application, the WRITE CAL signal should be held logic
HIGH, and the WRITE PULSE signal will control write loop
calibration via the internal AND gate.
The bias loop may be continuously recalibrated whenever
WRITE PULSE is logic LOW.
Figure 8. Calibration Time Curve
–8–
REV. 0
Page 9
AD9660
DAC1
DAC2
V
DAC1
V
DAC2
OP291
OP291
+5V
V
REF + VDAC1
= V
BIAS LEVEL
R2
R1
V
REF + VDAC2
= V
WRITE LEVEL
R4
R3
BIAS LEVEL
V
REF
WRITE LEVEL
AD9660
R1
R2
R3
R4
R3
R4
R1
R2
Example Calculations
The example below (in addition to the one included in the sections above) should guide users in choosing R
GAIN
, C
GAIN
, the
hold capacitor values, and worst case calibration times.
System Requirements:
• Bias laser power: 4 mW Bias ± 5%
• Write laser power: 25 mW ± 0.5%
• Bias Hold Time: 1 ms
• Write Hold Time: 1 µs
Laser diode/photo diode characteristics:
• Laser efficiency 0.5 mA/mA
• Monitor current: 5 µA/mA
• From the laser power requirements and efficiency we can
estimate:
∆I
BIAS MAX
= 4 mW ×(5%)/ 0.5
mW
mA
= 400. 0 µA
and
∆I
WRITE MAX
= 25 mW × 0.5%
(
/0.5
)
mW
mA
= 250 µA
• Choosing hold caps based on these:
−9
C
BIAS HOLD
18 ×10
=
×1 ms
400 µA
= 0.045 µF
and
−9
C
WRITE HOLD
18 ×10
=
250 µA
×1 µs
= 72 pF
• The bias loop initial calibration time for a <1% error:5τ = 5 × RC = 5 × 550
Ω
× 0.045
µ
F = 123.75µs
• Bias loop recalibration for a 1% error after 5% droop (need to
correct within 20%):
2τ = 2 ×RC = 2 × 140
Ω
× 0.045
µ
F = 12.6µs
• The write loop initial calibration time for <0.1% error:
7τ = 7 ×RC = 7 × 550
Ω
× 72 pF = 277.2 ns
• Write loop re-calibration for a 0.1% error after 0.5% droop
(need to correct within 20%):
2τ = RC = 2 × 140
Ω
× 72 pF = 20.2 ns
• From the monitor current specification and the max power
specified:
I
MONITOR MAX
= 25 mW
5 µA
mW
=125 µA
and
1. 6 V
MONITOR MAX
−50 Ω=6.9 kΩ
• C
R
=
GAIN
GAIN
1. 85 × I
would be chosen as 2 pF (see Table I).
Driving the Analog Inputs
The BIAS LEVEL and WRITE LEVEL inputs of the AD9660
drive the track and hold amplifiers and allow the user to adjust
the amount of output current as described above. The input
voltage range on both inputs is V
the user to create an offset of V
REF
REF
to V
for a ground based signal.
+ 1.6 V, requiring
REF
The circuit in Figure 9 will perform the level shift and scale the
output of a DAC whose output is from ground to a positive
voltage. This solution is attractive because both the DAC and
the op amp can run off a single +5 V supply, and the op amp
doesn’t have to swing rail to rail.
Figure 9. Driving the Analog Inputs
REV. 0
–9–
Page 10
AD9660
Offset Current Generator
The offset current source allows the user to inject a fixed,
uncalibrated current into the laser diode. The offset current
source is set by an external resistor connected between OFFSET CURRENT SET and +V
, and is controlled by OFFSET
S
PULSE. See Figure 2 for a transfer function of the offset current source.
The offset current may be used to increase the output current
provided by the bias and/or write loops after calibration. Alternatively, the offset current may be added during the calibration
of the bias loop and switched off after calibration to drop the
bias current below the knee of the laser diode power curve.
This is illustrated in Figure 10.
4
0°C CASE
3
2
OPTICAL OUTPUT – mW
1
0
CONSTANT WRITE POWER
BIAS CALIBRATION POWER
OPERATING
BIAS LEVEL
012020
1
WITH OFFSET CURRENT TURNED OFF,
BIAS CURRENT IS BELOW THE KNEE OF THE LASER DIODE
As in all high speed applications, proper layout is critical; it is
particularly important when both analog and digital signals are
involved. Analog signal paths should be kept as short as possible, and isolated from digital signals to avoid coupling in noise.
In particular, digital lines should be isolated from OUTPUT,
PIN SENSE, WRITE LEVEL, and BIAS LEVEL traces. Digital signal paths should also be kept short, and run lengths
matched to avoid propagation delay mismatch.
Layout of the ground and power supply circuits is also critical.
A single, low impedance ground plane will reduce noise on the
circuit ground. Power supplies should be capacitively coupled
to the ground plane to reduce noise in the circuit. 0.1 µF sur-
face mount capacitors, placed as close as possible to the
AD9660 +V
connections meet this requirement. Multilayer
S
circuit boards allow designers to lay out signal traces without
interrupting the ground plane, and provide low impedance
power planes to further reduce noise.
Minimizing the Impedance of the Output Current Path
Because of the very high current slew that the AD9660 is
capable of producing (70+ mA in 1.5 ns), the inductance of the
output current path to and from the laser diode is critical. A
good layout of the output current path will yield high quality
light pulses with rise times of about 1.5 ns and less than 5%
overshoot. A poor layout can result in significant overshoot and
ringing. The most important guideline for the layout is to minimize the impedance (mostly inductance) of the output current
path to the laser. It is important to recognize that the laser current path is a closed loop. The figure illustrates the path that
current travels: (1) from the output pins of the AD9660 to the
anode of the laser, (2) through the laser to the cathode
(ground), (3) through the return path, (4) through the 0.1 µF
bypass capacitors back to the +V
pins of the AD9660 where (5)
S
the current travels through the output driver circuitry of the
AD9660, and back to the output pins. The inductance of this
loop can be minimized by placing the laser as close to the
AD9660 as possible to keep the loop short, and by placing the
send and return paths on adjacent layers of the PC board to take
advantage of mutual coupling of the path inductances. This
mutual coupling effect is the most important factor in reducing
inductance in the current path.
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AD9660
The trace from the output pins of the AD9660 to the anode of
the laser (send trace) should be several millimeters wide and
should be as direct as possible. The return current will choose
the path of least resistance. If the return path is the ground
plane, it should have an unbroken path, under the output trace,
from the laser cathode back to the AD9660. If the return path is
not the ground plane (such as on a two layer board, or on the
plane), it should still be on the board plane adjacent to the
+V
S
plane of the output trace. If the current cannot return along a
path that follows the output trace, the inductance will be drastically increased and performance will be degraded.
Optimizing the Feedback Layout
In applications where the dynamic performance of the analog
feedback loop is important, it is necessary to optimize the layout
of the gain resistor, R
, as well as the monitor current path to
GAIN
SENSE IN. Such applications include MOD systems which
recalibrate the write loop on pulses as short as 25 ns, and closed
loop applications.
PIN ASSIGNMENTS
PIN CONNECTIONS
+V
S
25
24
23
22
The best possible TZA settling will be achieved by using a
single carbon surface mount resistor (usually 5% tolerance) for
and small surface mount capacitor for C
R
GAIN
. Because the
GAIN
GAIN pin (Pin 9) is essentially connected to the inverting input
of the TZA, it is very sensitive to stray capacitance. R
GAIN
should be placed between Pin 9 and Pin 10, as close as possible
to Pin 9. Small traces should be used, and the ground and +V
S
planes adjacent to the trace should be removed to further minimize stray capacitance.
The trace from SENSE IN to the cathode of the PIN photodetector should be thin and routed away from the laser anode
trace.
MUTUAL COUPLING
REDUCES INDUCTANCE
LASER DIODE CURRENT
PATH SEGMENTS
(SEE TEXT)
1
5
AD9660
OUTPUT PIN CONNECTIONS
CONNECTIONS
21
20
19
4
BYPASS CAPS
GROUND PIN
GROUND PLANE
Figure 11. Laser Diode Current Loop
3
2
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AD9660
0.300 (7.60)
0.292 (7.40)
0.012 (0.30)
0.004 (0.10)
OUTLINE DIMENSIONS
Dimensions shown in inches and (mm).
28-Pin Plastic SOIC
(R-28)
0.712 (18.08)
0.700 (17.78)
2815
PIN 1
(1.27)
BSC
0.019 (0.48)
0.014 (0.36)
0.0500
0.419 (10.64)
141
SEATING
PLANE
0.393 (9.98)
0.104 (2.64)
0.093 (2.36)
0.013 (0.33)
0.009 (0.23)
C2040–6–7/95
0.04 (1.02)
0.024 (0.61)
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PRINTED IN U.S.A.
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