The OPT211 is a monolithic photodiode with on-chip
FET-input transpedance amplifier, that provides wide
bandwidth at very high gains. Uncommitted input and
feedback nodes allow a variety of feedback options for
maximum versatility. Trade-offs in responsivity (gain),
bandwidth and SNR can easily be made.
The monolithic combination of photodiode and
transimpedance amplifier on a single chip eliminates
the problems commonly encountered in discrete designs such as leakage current errors, noise pickup and
gain peaking due to stray capacitance. The 0.09 x 0.09
inch photodiode is operated at zero bias for excellent
linearity and low dark current. Direct access to the
detector’s anode allows photodiode bootstrapping,
which increases speed performance.
The OPT211 operates over a wide supply range (±2.25V
to ±18V) and supply current is only 400µA. It is
packaged in a transparent plastic 8-pin DIP specified
for the 0°C to 70°C temperature range.
SPECTRAL RESPONSIVITY
Ultraviolet
0.5
0.4
0.3
0.2
0.1
Photodiode Responsivity (A/W)
0
Using External
1MΩ Resistor
100 200 300 400 500 600 700 800 900 1000 1100
Blue
Wavelength (nm)
Green
Yellow
Red
Infrared
International Airport Industrial Park • Mailing Address: PO Box 11400, Tucson, AZ 85734 • Street Address: 6730 S. Tucson Blvd., Tucson, AZ 85706 • Tel: (520) 746-1111 • Twx: 910-952-1111
Photodiode Current650nm0.45A/W
Unit-to-Unit Variation650nm±5%
Voltage Outputλ = 650nm, R
Nonlinearity0.01% of FS
Photodiode Area(0.090 x 0.090 inches)0.008in
(2.29 x 2.29mm)5.2mm
DARK ERRORS, RTO
(1)
Offset Voltage, Output±0.5±2mV
vs Temperature±10µV/°C
vs Power SupplyV
Voltage Noise, DarkDark, f
= ±2.25V to ±18V10100µV/V
S
B
FREQUENCY RESPONSE
BandwidthAnode Grounded
Anode Bootstrapped
Rise Time, 10% to 90%, R
= 1MΩAnode Grounded
F
Anode Bootstrapped
Settling Time, FS to DarkAnode Grounded
1%10µs
0.1%25µs
0.01%30µs
100% Overload Recovery TimeFS to Dark (to 1%)44µs
OUTPUT
Voltage OutputR
Capacitive Load, Stable Operation
(4)
Short-Circuit Current±18mA
POWER SUPPLY
Operating Voltage Range±2.25± 15±18V
Quiescent CurrentV
NOTES: (1) Referred to Output. Includes all error sources. (2) See Figure 1. (3) See Figure 3. (4) See Figure 2.
= 1MΩ0.45V/µW
F
= 0.1Hz to 100kHz1mVrms
(2)
(3)
(2)
(3)
(2)
V
= ±5V100µs
S
V
= ±2.25V240µs
S
= 10kΩ(V+) – 1.25(V+) – 1V
L
R
= 5kΩ(V+) – 2(V+) – 1.5V
L
= 0V±400±500µA
OUT
50kHz
150kHz
5µs
2µs
250pF
100°C/W
2
2
PHOTODIODE SPECIFICATIONS
At TA = +25°C, λ = 650nm, unless otherwise noted.
Photodiode of OPT211
PARAMETERCONDITIONSMINTYPMAXUNITS
Photodiode Area(0.090 x 0.090 inches)0.008in
(2.29 x 2.29mm)5.2mm
Current Responsivityλ = 650nm0.45A/W
865µA/W/cm
Dark CurrentVD = 0V500fA
vs Temperaturedoubles every 10°C
CapacitanceV
= 0V600pF
D
The information provided herein is believed to be reliable; however, BURR-BROWN assumes no responsibility for inaccuracies or omissions. BURR-BROWN assumes
no responsibility for the use of this information, and all use of such information shall be entirely at the user’s own risk. Prices and specifications are subject to change
without notice. No patent rights or licenses to any of the circuits described herein are implied or granted to any third party. BURR-BROWN does not authorize or warrant
any BURR-BROWN product for use in life support devices and/or systems.
®
OPT211
2
2
2
2
Page 3
OP AMP SPECIFICATIONS
TA = +25°C, VS = ±15V, RL = 10kΩ, unless otherwise noted.
OPT211 Op Amp
PARAMETERCONDITIONSMINTYPMAXUNITS
INPUT
Offset Voltage±0.5mV
vs Temperature±5µV/°C
vs Power SupplyV
Input Bias Current±1pA
= ±2.25V to ±18V10µV/V
S
vs Temperaturedoubles every 10°C
Input Impedance
Differential10
Common-Mode10
Common-Mode Input Voltage RangeLinear Operation±14.4V
Common-Mode Rejection106dB
NOISE
Voltage Noise Densityf = 10Hz30nV/√Hz
f = 100Hz25nV/√Hz
f = 1kHz15nV/√Hz
Current Noise Densityf = 1kHz0.8fA/√Hz
OPEN-LOOP GAIN
Open-Loop Voltage Gain120dB
FREQUENCY RESPONSE
Gain-Bandwidth Product
(2)
Slew Rate6V/µs
Settling Time 0.1%4µs
0.01%5µs
OUTPUT
Voltage OutputR
Short-Circuit Current±18mA
= 10kΩ(V+) – 1.25(V+) – 1V
L
R
= 5kΩ(V+) – 2(V+) – 1.5V
L
POWER SUPPLY
Operating Voltage Range±2.25±15±18V
Quiescent CurrentI
= 0mA±400±500µA
O
NOTES: (1) Op amp specifications provided for information and comparison only. (2) Stable in gains ≥ 20V/V.
Operating Temperature..................................................... –25°C to +85°C
Storage Temperature........................................................ –25°C to +85°C
Junction Temperature ...................................................................... +85°C
Lead Temperature (soldering, 10s)................................................ +300°C
(Vapor-Phase Soldering Not Recommended)
PACKAGE INFORMATION
PRODUCTPACKAGENUMBER
PACKAGE DRAWING
OPT211P8-Pin DIP006-1
NOTE: (1) For detailed drawing and dimension table, please see end of data
sheet, or Appendix C of Burr-Brown IC Data Book.
(1)
ELECTROSTATIC
DISCHARGE SENSITIVITY
This integrated circuit can be damaged by ESD. Burr-Brown
recommends that all integrated circuits be handled with appropriate precautions. Failure to observe proper handling and
installation procedures can cause damage.
ESD damage can range from subtle performance degradation
to complete device failure. Precision integrated circuits may
be more susceptible to damage because very small parametric
changes could cause the device not to meet its published
specifications.
S
MOISTURE SENSITIVITY
AND SOLDERING
Clear plastic does not contain the structural-enhancing fillers
used in black plastic molding compound. As a result, clear
plastic is more sensitive to environmental stress than black
plastic. This can cause difficulties if devices have been stored
in high humidity prior to soldering. The rapid heating during
soldering can stress wire bonds and cause failures. Prior to
soldering, it is recommended that plastic devices be baked-out
at +85°C for 24 hours.
The fire-retardant fillers used in black plastic are not compatible with clear molding compound. The OPT211 plastic
packages cannot meet flammability test, UL-94.
®
OPT211
4
Page 5
RESPONSE vs INCIDENT ANGLE
Relative Response
Incident Angle (°)
0
1.0
0.8
0.6
0.4
0.2
0
±20±40±60±80
θ
Y
θ
X
1.0
0.8
0.6
0.4
0.2
0
θ
Y
θ
X
Plastic
DIP Package
TYPICAL PERFORMANCE CURVES
At TA = +25°C, VS = ±15V, λ = 650nm, external 1MΩ feedback resistor, circuit shown in Figure 1, unless otherwise noted.
1.0
NORMALIZED SPECTRAL RESPONSIVITY
0.8
650nm
(0.45A/W)
0.6
0.4
0.2
Normalized Current or Voltage Output
0
100 200 300 400 500 600 700 800 900 1000 1100
Wavelength (nm)
TRANSIMPEDANCE vs FREQUENCY
100M
RF = 100MΩ
Dotted Line:
Bandwidth with
Bootstrap Buffer—
10M
RF = 10MΩ, CF = 1pF
1M
RF = 1MΩ, CF = 3pF
Transimpedance (V/A)
See Text.
(0.48A/W)
VOLTAGE RESPONSIVITY vs RADIANT POWER
10
1
= 100MΩ
F
R
0.1
Output Voltage (V)
0.01
= 10MΩ
F
R
R
= 1MΩ
F
λ = 650nm
100k
1k10k100k1M
Frequency (Hz)
VOLTAGE RESPONSIVITY vs IRRADIANCE
10
1
= 100MΩ
F
0.1
Output Voltage (V)
0.01
R
= 10MΩ
F
R
= 1MΩ
F
R
0.001
-4
10
-3
10
10
Irradiance (W/m
0.001
-3
10
-2
10
-1
10
10
1
10
2
10
Radiant Power (µW)
QUIESCENT CURRENT vs TEMPERATURE
0.6
0.5
VS = ±15V
0.4
0.3
VS = ±2.25V
0.2
λ = 650nm
Quiescent Current (mA)
0.1
0
10
-1
2
)
1010
-2
1
–50–250255075100125
–75
Temperature (°C)
5
OPT211
®
Page 6
TYPICAL PERFORMANCE CURVES (CONT)
At TA = +25°C, VS = ±15V, λ = 650nm, external 1MΩ feedback resistor, circuit shown in Figure 1, unless otherwise noted.
–2
10
Total Noise
0.1 Hz to
–3
10
Indicated BW
–4
10
RF = 100MΩ
–5
10
Noise Voltage (Vrms)
–6
10
RF = 10MΩ
–7
10
1101k10k100k100
OUTPUT NOISE VOLTAGE
vs MEASUREMENT BANDWIDTH
OPT211 Anode
RF = 1MΩ
Grounded
OPT211 with Anode
Bootstrap Drive
Frequency (Hz)
STEP RESPONSE
= 1MΩ, Anode Grounded
R
F
1M
NOISE EFFECTIVE POWER
–8
10
–9
10
vs MEASUREMENT BANDWIDTH
λ = 650nm
Total Noise
0.1 Hz to
–10
10
10
Noise Effective Power (W)
10
10
10
Indicated BW
–11
–12
–13
–14
1101k10k100k100
Frequency (Hz)
STEP RESPONSE
= 1MΩ, Bootstrap Buffer
R
F
1MΩ
10MΩ
100MΩ
OPT211 Anode
Grounded
OPT211 with Anode
Bootstrap Drive
1M
®
OPT211
6
Page 7
APPLICATIONS INFORMATION
Figure 1 shows the basic connections required to operate the
OPT211. Applications with high impedance power supplies
may require decoupling capacitors located close to the
device pins as shown in Figure 1.
C
F
RF ≥ 330kΩ
2
I
D
λ
78
R
F
(Ω)(pF)(kHz)
330k5.686
1M350
10M1
100M0.3
NOTE: (1) Feedback resistor has approximately 1pF stray
capacitance. C
resistors. See text.
0.1µF0.1µF
<1pF requires series-connected feedback
F
OPT211
13
V+
+15V
C
F
(1)
(1)
V–
–15V
5
Bandwidth
16
5
V
OUT
FIGURE 1. Basic Circuit Connections.
Output is zero volts with no light and increases with increasing illumination. Photodiode current is proportional to the
radiant power (watts) falling in the photodiode. At 650nm
wavelength (visible red) the photodiode responsivity is approximately 0.45A/W. Responsivity at other wavelengths is
shown in the typical performance curve “Responsivity vs
Wavelength.”
The OPT211’s output voltage is the product of the photodiode current and feedback resistor, (I
). The feedback
DRF
resistor must be greater than 330kΩ for proper stability. A
feedback capacitor, CF, must be connected as shown. Recommended values are shown in Figure 1. Capacitor values
for other feedback resistances can be interpolated.
The OPT211 provides excellent performance with very high
feedback resistor values. To achieve maximum bandwidth
with R
≥ 10MΩ, good circuit layout is required. With
F
careful circuit board layout and a 10MΩ feedback resistor,
stray capacitance will provide approximately the correct
parallel capacitance for stable operation and widest bandwidth. For larger feedback resistor values, two resistors
connected in series and laid-out end-to-end will reduce the
stray capacitance to a few tenths of a picofarad. With
experimentation, circuit board traces can be used to produce
the necessary stray capacitance for proper compensation and
widest possible bandwidth.
The circuit in Figure 1 can drive capacitive loads up to
250pF. To drive load capacitance up to 1nF, connect R
and
1
the feedback components as shown in Figure 2.
DARK ERRORS
Dark error specifications include all error sources and are
tested with the circuit shown in Figure 1 using R
=1MΩ.
F
The dominate dark error source is the input offset voltage of
the internal op amp. The combination of photodiode dark
current and op amp input bias current is approximately
1.5pA at 25°C. Even with very large feedback resistors, this
contributes virtually no offset error. Dark current and input
bias current increase with temperature, doubling (approximately) for each 10°C increase. At 70°C, dark current is
approximately 35pA. This would produce 3.5mV offset with
a 100MΩ feedback resistor.
Circuit board leakage currents can increase dark error. Use
clean assembly procedures to avoid contamination, particularly around the sensitive inverting input node (pin 2). Errors
due to leakage current from the V+ supply (pin 1) can be
eliminated by encircling the trace connecting to pin 2 with
a guard trace connected to ground.
IMPROVING BANDWIDTH
Bandwidth of the OPT211 can be increased with the feedback buffer circuits shown in Figure 3. Driving the anode of
the photodiode (pin 7) in this manner reduces the effect of
the photodiode’s capacitance on signal bandwidth. This
“bootstrap drive” circuit boosts bandwidth by approximately
3x. Bandwidth achieved with various R
Figure 2. When using a bootstrap buffer, R
values is shown in
F
must be greater
F
or equal to 1MΩ for stable operation.
R
F
C
F
2
OPT211
R
1
175Ω
λ
78
0.1µF0.1µF
13
V+
V–
5
V
CL≤1nF
OUT
FIGURE 2. Increasing C-Load Drive.
®
7
OPT211
Page 8
To Pin 7
+15V
S
D
–15V
+15V
–15V
7.5kΩ
λ
R
6.8kΩ
R
1
Q
1
2N5116
78
Q
1
2N6427
1
(b)
Bootstrap
Buffer
2
(a)
From
Pin 2
RF ≥ 1MΩ
1
To Pin 7
C
F
OPT211
3
–15V+15V
OPA131
5
(c)
V
OUT
From
Pin 2
AC COUPLING
Some applications are concerned only with sensing variation
in light intensity. Simple capacitive coupling at the OPT211’s
output may be adequate. With large feedback resistors or
bright ambient light, however, the OPT211’s output may
saturate. The circuit in Figure 4 can reject very bright
ambient light, yet provide high AC gain for best signal-tonoise ratio. The output voltage is integrated and fed back to
the inverting input through R
. This drives the average (dc)
3
voltage at the output to zero. Application Bulletin AB-061
provides more details on this technique.
C
= C
1
R1 = R
f
–3dB
2
2
=
R3(2πR2C2)
=16Hz
λ
R
F
2
R
1MΩ
6
3
C
2
0.1µF
OPA177
RF = 10MΩ
OPT211
2
3
R
1MΩ
1
5
R
2
1MΩ
C
1
0.1µF
V
OUT
R
F
(Ω)(pF)(kHz)
330kNot Recommended
1M1
10M<0.2
100M<0.2
NOTE: (1) Most resistors have approximately 1pF stray
capacitance. C
resistors. See text.
<1pF requires series-connected feedback
F
C
F
(1)
(1)
(1)
Bandwidth
150
42
13
FIGURE 3. Increasing Bandwidth with Bootstrap Buffer.
Gate or base current of the buffer transistor flows through
the feedback resistor, increasing the dark offset voltage. If
dark errors are important, use a FET transistor with picoamp
gate current. A P-channel FET is used to assure that the
anode is at ground potential or slightly negative.
If dark errors are not critical, an NPN Darlington transistor
can be used for a buffer as shown in Figure 3b. A FET-input
op amp connected as a buffer can be used as shown in Figure
3c, but its noise may degrade circuit performance slightly.
Bandwidth of the buffer should be 4MHz, minimum.
1
78
3
See Application Bulletin
V–V+
AB-061 for details.
FIGURE 4. Rejecting Ambient Light.
This circuit also corrects output offset produced by input
bias current of a buffer used to extend bandwidth. A
Darlington transistor can be used for a bandwidth-enhancing
bootstrap buffer in this circuit without creating offset error.
NOISE PERFORMANCE
Noise performance of the OPT211 is shown in typical
curves for various feedback resistor values. This curve
specifies the total noise measured from 0.1Hz to the indicated bandwidth. High frequency noise is reduced with the
bootstrap transistor buffer circuits shown in Figure 1. This
effect is shown on the typical curve.
Output noise of the OPT211 extends beyond the signal
bandwidth, especially for high feedback resistor values.
Signal-to-noise ratio can be improved by filtering the
OPT211’s output to a bandwidth equal to the signal bandwidth—see Figure 5.
®
OPT211
8
Page 9
Best signal-to-noise ratio is achieved by using the highest
practical feedback resistor. This comes with the trade-off of
decreased bandwidth.
The noise performance of a photodetector is sometimes
characterized by its noise effective power (NEP). This is the
radiant power which would produce an output signal equal
to the output noise level. NEP has the units of radiant
power (W). A NEP curve is provided.
LIGHT SOURCE POSITIONING
The OPT211 is 100% tested with a light source that uniformly
illuminates the full area of the integrated circuit, including
the op amp. Although all IC amplifiers are light-sensitive to
some degree, the OPT211 op amp circuitry is designed to
minimize this effect. Sensitive junctions are shielded with
metal, and differential stages are cross-coupled. Furthermore,
the photodiode area is very large relative to the op amp input
circuitry making these effects negligible.
If your light source is focused to a small area, be sure that
it is properly aimed to fall on the photodiode. If a narrowly
focused light source were to miss the photodiode area and
fall only on the op amp circuitry, the OPT211 would not
perform properly. The large (0.090 inch x 0.090 inch)
photodiode area allows easy positioning of narrowly focused
light sources. The photodiode area is easily visible as it
appears very dark compared to the surrounding active
circuitry.
The incident angle of the light source also affects the
apparent sensitivity in uniform irradiance. For small incident
angles, the loss in sensitivity is simply due to the smaller
effective light gathering area of the photodiode (proportional
to the cosine of the angle). At a greater incident angle, light
is diffracted and scattered by the side of the package. These
effects are shown in the typical performance curve
“Responsivity vs Incident Angle.”
LINEARITY PERFORMANCE
The photodiode inside the OPT211 is designed to be operated
in the photoconductive mode (V
= 0V) for very linear
DIODE
operation with radiant power throughout a wide range.
Nonlinearity remains below approximately 0.05% up to
100µA photodiode current.
This very linear performance at high radiant power assumes
that the full photodiode area is uniformly illuminated. If the
light source is focused to a small area of the photodiode,
nonlinearity will occur at lower radiant power.
Using Burr-Brown’s Application Bulletin No. AB-034
RF = 10MΩ
2
OPT211
5
2.94kΩ
λ
Sallen-Key
1
78
3
V–V+
FIGURE 5. Low Pass Filter for Improved Signal-to-Noise Ratio.
2-Pole Butterworth
f
= 20kHz
–3dB
Sallen-Key Low Pass Filter Designed
2.2nF
2
21kΩ
OPA131
3
470pF
6
V
O
®
9
OPT211
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