Fully differential
Extremely low power with power-down feature
2.6 mA quiescent supply current @ 5 V
450 µA in power-down mode @ 5 V
High speed
110 MHz large signal 3 dB bandwidth @ G = 1
450 V/µs slew rate
12-bit SFDR performance @ 500 kHz
Fast settling time: 100 ns to 0.02%
Low input offset voltage: ±2.6 mV max
Low input offset current: 0.45 µA max
Differential input and output
Differential-to-differential or single-ended-to-differential
operation
Rail-to-rail output
Adjustable output common-mode voltage
Externally adjustable gain
Wide supply voltage range: 2.7 V to 12 V
Available in small SOIC package
Qualified for automotive applications
Low Cost, Low Power,
FUNCTIONAL BLOCK DIAGRAM
Figure 1.
APPLICATIONS
ADC drivers
Automotive vision and safety systems
Automotive infotainment systems
Portable instrumentation
Battery-powered applications
Single-ended-to-differential converters
Differential active filters
Video amplifiers
Level shifters
GENERAL DESCRIPTON
The AD8137 is a low cost differential driver with a rail-to-rail
output that is ideal for driving ADCs in systems that are sensitive
to power and cost. The AD8137 is easy to apply, and its internal
common-mode feedback architecture allows its output commonmode voltage to be controlled by the voltage applied to one pin.
The internal feedback loop also provides inherently balanced
outputs as well as suppression of even-order harmonic distortion
products. Fully differential and single-ended-to-differential gain
configurations are easily realized by the AD8137. External
feedback networks consisting of four resistors determine the
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
license is granted by implication or otherwise under any patent or patent rights of Analog Devices.
closed-loop gain of the amplifier. The power-down feature is
beneficial in critical low power applications.
The AD8137 is manufactured on Analog Devices, Inc.,
proprietary second-generation XFCB process, enabling it to
achieve high levels of performance with very low power
consumption.
The AD8137 is available in the small 8-lead SOIC package and
3 mm × 3 mm LFCSP package. It is rated to operate over the
extended industrial temperature range of −40°C to +125°C.
One Technology Way, P.O. Box 9106, Norwood, MA 02062-9106, U.S.A.
Tel: 781.329.4700 www.analog.com
Figure 2. Small Signal Response for Various Gains
AD8137 Data Sheet
TABLE OF CONTENTS
Features .............................................................................................. 1
VS+ to VS−
Power Dissipation See Figure 3
Input Common-Mode Voltage VS+ to VS−
Storage Temperature Range −65°C to +125°C
Operating Temperature Range −40°C to +125°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.
THERMAL RESISTANCE
θJA is specified for the worst-case conditions, that is, θJA is
specified for the device soldered in a circuit board in still air.
The power dissipated in the package (P
quiescent power dissipation and the power dissipated in the
package due to the load drive for all outputs. The quiescent
power is the voltage between the supply pins (V
quiescent current (I
). The load current consists of differential
S
and common-mode currents flowing to the load, as well as
currents flowing through the external feedback networks and
the internal common-mode feedback loop. The internal resistor
tap used in the common-mode feedback loop places a 1 kΩ
differential load on the output. RMS output voltages should be
considered when dealing with ac signals.
Airflow reduces θ
. In addition, more metal directly in contact
JA
with the package leads from metal traces, through holes, ground,
and power planes reduces the θ
JA
Figure 3 shows the maximum safe power dissipation in the
package vs. the ambient temperature for the 8-lead SOIC
(125°C/W) and 8-lead LFCSP (θ
standard 4-layer board. θ
The maximum safe power dissipation in the AD8137 package
is limited by the associated rise in junction temperature (T
the die. At approximately 150°C, which is the glass transition
temperature, the plastic changes its properties. Even temporarily
exceeding this temperature limit may change the stresses that
the package exerts on the die, permanently shifting the parametric
performance of the AD8137. Exceeding a junction temperature
of 175°C for an extended period can result in changes in the
silicon devices, potentially causing failure.
) on
J
Figure 3. Maximum Power Dissipation vs.
Ambient Temperature for a 4-Layer Board
ESD CAUTION
Rev. E | Page 9 of 32
AD8137 Data Sheet
04771-0-001
–IN
1
V
OCM
2
V
S+
3
+OUT
4
+IN
8
PD
7
V
S–
6
–OUT
5
AD8137
1
−IN
Inverting Input.
PIN CONFIGURATION AND FUNCTION DESCRIPTIONS
Figure 4. Pin Configuration
Table 6. Pin Function Descriptions
Pin No. Mnemonic Description
2 V
OCM
An internal feedback loop drives the output common-mode voltage to be equal to the voltage applied to
the V
pin, provided the operation of the amplifier remains linear.
OCM
3 VS+ Positive Power Supply Voltage.
4 +OUT Positive Side of the Differential Output.
5 −OUT Negative Side of the Differential Output.
6 VS− Negative Power Supply Voltage.
7
PD
Power Down.
8 +IN Noninverting Input.
EPAD Exposed paddle may be connected to either ground plane or power plane.
Rev. E | Page 10 of 32
Data Sheet AD8137
R
G
= 1kΩ
V
O, dm
= 0.1V p-p
FREQUENCY (MHz)
NORMALIZED CLOSED-LOOP GAIN (dB)
3
2
1
0
–12
–11
–10
–9
–8
–7
–6
–5
–4
–3
–2
–1
0.11101001000
04771-0-002
G = 5
G = 10
G = 1
G = 2
FREQUENCY (MHz)
CLOSED-LOOP GAIN (dB)
–12
1101001000
04771-0-003
VS = ±5
VS = +5
VS = +3
3
2
1
0
–11
–10
–9
–8
–7
–6
–5
–4
–3
–2
–1
V
O, dm
= 0.1V p-p
FREQUENCY (MHz)
CLOSED-LOOP GAIN (dB)
3
2
1
0
–12
–11
–10
–9
–8
–7
–6
–5
–4
–3
–2
–1
1101001000
04771-0-006
V
O, dm
= 0.1V p-p
T = –40°C
T = +125°C
T = +85°C
T = +25°C
FREQUENCY (MHz)
NORMALIZED CLOSED-LOOP GAIN (dB)
3
2
1
0
–12
–11
–10
–9
–
8
–7
–6
–5
–4
–3
–2
–1
0.11101001000
04771-0-004
G = 10
G = 1
G = 2
G = 5
RG= 1kΩ
V
O, dm
= 2.0V p-p
FREQUENCY (MHz)
CLOSED-LOOP GAIN (dB)
4
3
2
1
0
–11
–
10
–9
–8
–7
–6
–5
–4
–3
–2
–1
1101001000
04771-0-005
V
O, dm
= 2.0V p-p
VS = ±5
VS = +5
V
S
= +3
FREQUENCY (MHz)
CLOSED-LOOP GAIN (dB)
4
3
2
1
–11
–10
–9
–8
–7
–6
–5
–4
–3
–2
–1
0
1101001000
04771-0-007
T = +85°C
T = +125°C
T = –40°C
T = +25°C
V
O, dm
= 2.0V p-p
TYPICAL PERFORMANCE CHARACTERISTICS
Unless otherwise noted, differential gain = 1, RG = RF = R
Figure 60 for the definition of terms.
= 1 kΩ, VS = 5 V, TA = 25°C, V
L, dm
= 2.5V. Refer to the basic test circuit in
OCM
Figure 5. Small Signal Frequency Response for Various Gains
Figure 6. Small Signal Frequency Response for Various Power Supplies
Figure 8. Large Signal Frequency Response for Various Gains
Figure 9. Large Signal Frequency Response for Various Power Supplies
Figure 7. Small Signal Frequency Response at Various Temperatures
Figure 10. Large Signal Frequency Response at Various Temperatures
Rev. E | Page 11 of 32
AD8137 Data Sheet
FREQUENCY (MHz)
CLOSED-LOOP GAIN (dB)
3
2
1
0
–1
–3
–4
–2
–5
–6
–7
–8
–10
–11
–9
–
12
1101001000
04771-0-041
V
O, dm
= 0.1V p-p
R
L, dm
= 2kΩ
R
L, dm
= 1kΩ
R
L, dm
= 500Ω
1101001000
FREQUENCY (MHz)
CLOSED-LOOP GAIN (dB)
V
O, dm
= 0.1V p-p
3
2
1
0
–12
–11
–10
–9
–8
–7
–6
–5
–4
–3
–2
–1
04771-0-008
C
F
= 2pF
CF= 1pF
C
F
= 0pF
FREQUENCY (MHz)
CLOSED-LOOP GAIN (dB)
2
1
0
–1
–2
–4
–5
–3
–6
–7
–8
–9
–11
–12
–10
–13
1101001000
04771-0-042
V
O, dm
= 0.1V p-p
V
OCM
= 1V
V
OCM
= 4V
V
OCM
= 2.5V
FREQUENCY (MHz)
CLOSED-LOOP GAIN (dB)
3
2
1
0
–1
–3
–4
–2
–5
–6
–7
–8
–10
–11
–9
–12
1101001000
04771-0-043
V
O, dm
= 2V p-p
R
L, dm
= 2kΩ
R
L, dm
= 1kΩ
R
L, dm
= 500Ω
1101001000
FREQUENCY (MHz)
CLOSED-LOOP GAIN (dB)
V
O, dm
= 2.0V p-p
3
2
1
0
–12
–11
–10
–9
–8
–7
–6
–5
–4
–3
–2
–1
04771-0-009
CF= 2pF
CF= 1pF
C
F
= 0pF
FREQUENCY (MHz)
CLOSED-LOOP GAIN (dB)
3
2
1
0
–1
–3
–4
–2
–5
–6
–7
–8
–10
–11
–9
–12
1101001000
04771-0-044
2V p-p
0.5V p-p
0.1V p-p
1V p-p
Figure 11. Small Signal Frequency Response for Various Loads
Figure 12. Small Signal Frequency Response for Various C
F
Figure 14. Large Signal Frequency Response for Various Loads
Figure 15. Large Signal Frequency Response for Various C
F
Figure 13. Small Signal Frequency Response at Various V
OCM
Rev. E | Page 12 of 32
Figure 16. Frequency Response for Various Output Amplitudes
Data Sheet AD8137
FREQUENCY (MHz)
CLOSED-LOOP GAIN (dB)
4
3
2
1
–3
–2
–1
0
–7
–6
–5
–4
–11
–10
–9
–8
110100
1000
04771-0-037
G = 1
V
S
= ±5V
V
O, dm
= 0.1V p-p
R
F
= 500Ω
R
F
= 2kΩ
RF = 1kΩ
FREQUENCY (MHz)
DISTORTION (dBc)
–65
–70
–80
–75
–85
–90
–95
–100
–105
0.1110
04771-0-045
V
S
= ±5V
V
S
= +5V
V
S
= +3V
G = 1
V
O, dm
= 2V p-p
V
O, dm
(V p-p)
DISTORTION (dBc)
–50
–60
–65
–70
–55
–75
–80
–85
–90
–95
–100
0.25 1.25 2.25 3.25 4.25 5.257.25 8.256.259.25
04771-0-027
F
C
= 500kHz
SECOND HARMONIC SOLID LINE
THIRD HARMONIC DASHED LINE
V
S
= +5V
VS = +5V
VS = +3V
V
S
= +3V
FREQUENCY (MHz)
CLOSED-LOOP GAIN (dB)
4
3
2
1
–3
–2
–1
0
–7
–6
–5
–4
–11
–10
–9
–8
1
101001000
04771-0-036
G = 1
V
O, dm
= 2V p-p
R
F
= 500Ω
R
F
= 2kΩ
RF = 1kΩ
FREQUENCY (MHz)
DISTORTION (dBc)
–40
–70
–60
–50
–80
–90
–
100
–110
0.1110
04771-0-063
V
S
= ±5V
V
S
= +5V
V
S
= +3V
G = 1
V
O, dm
= 2V p-p
V
O, dm
(V p-p)
DISTORTION (dBc)
–50
–60
–65
–70
–55
–75
–80
–85
–90
–95
–100
0.25 1.25 2.25 3.25 4.25 5.257.25 8.256.259.25
04771-0-026
V
S
= +5V
V
S
= +5V
VS = +3V
VS = +3V
FC = 2MHz
SECOND HARMONICSOLID
LINE
THIRDHARMONIC DASHED LINE
Figure 17. Small Signal Frequency Response for Various R
F
Figure 18. Second Harmonic Distortion vs. Frequency and Supply Voltage
Figure 20. Large Signal Frequency Response for Various R
F
Figure 21. Third Harmonic Distortion vs. Frequency and Supply Voltage
Figure 19. Harmonic Distortion vs. Output Amplitude and Supply,
F
= 500 kHz
C
= 2 MHz
C
Figure 22. Harmonic Distortion vs. Output Amplitude and Supply, F
Rev. E | Page 13 of 32
AD8137 Data Sheet
FREQUENCY (MHz)
DISTORTION (dBc)
–40
–50
–60
–70
–80
–90
–100
–110
0.1110
04771-0-032
V
O, dm
= 2V p-p
R
L, dm
= 200Ω
R
L, dm
= 1kΩ
R
L, dm
= 500Ω
FREQUENCY (MHz)
DISTORTION (dBc)
–40
–50
–60
–70
–80
–90
–100
–110
0.1110
04771-0-034
G = 2
G = 5
G = 1
V
O, dm
= 2V p-p
R
G
= 1kΩ
FREQUENCY (MHz)
DISTORTION (dBc)
–40
–50
–60
–70
–80
–90
–100
–110
0.1110
04771-0-030
V
O, dm
= 2V p-p
G = 1
R
F
= 500Ω
R
F
= 2kΩ
RF = 1kΩ
FREQUENCY (MHz)
DISTORTION (dBc)
–40
–50
–60
–70
–80
–90
–100
–110
0.1110
04771-0-033
V
O, dm
= 2V p-p
R
L, dm
= 200Ω
R
L, dm
= 1kΩ
R
L, dm
= 500Ω
FREQUENCY (MHz)
DISTORTION (dBc)
–40
–50
–60
–70
–80
–90
–100
–110
0.1110
04771-0-035
V
O, dm
= 2V p-p
R
G
= 1kΩ
G = 5
G = 1
G = 2
FREQUENCY (MHz)
DISTORTION (dBc)
–40
–50
–60
–70
–80
–90
–100
–110
0.1110
04771-0-031
V
O, dm
= 2V p-p
G = 1
R
F
= 500Ω
R
F
= 2kΩ
RF = 1kΩ
Figure 23. Second Harmonic Distortion at Various Loads
Figure 24. Second Harmonic Distortion at Various Gains
Figure 26. Third Harmonic Distortion at Various Loads
Figure 27. Third Harmonic Distortion at Various Gains
Figure 25. Second Harmonic Distortion at Various RF
Rev. E | Page 14 of 32
Figure 28. Third Harmonic Distortion at Various RF
Data Sheet AD8137
V
OCM
(V)
DISTORTION (dBc)
–50
–60
–80
–70
–100
–90
–110
0.51.01.52.52.03.54.03.04.5
04771-0-028
FC = 500kHz
V
O, dm
= 2V p-p
SECOND HARMONIC SOLID LINE
THIRD HARMONIC DASHED LINE
FREQUENCY (Hz)
INPUT VOLTAGE NOISE (nV/√Hz)
100
10
1
101001k10k100k1M10M100M
04771-0-046
FREQUENCY (MHz)
CMRR (dB)
20
–20
–10
0
10
–50
–30
–40
–70
–60
–80
110100
04771-0-013
V
IN, cm
= 0.2V p-p
INPUT CMRR = ∆V
O, cm/
∆V
IN, cm
V
OCM
(V)
DISTORTION (dBc)
–50
–60
–70
–80
–90
–100
–110
0.5 0.7 0.91.31.11.5 1.72.32.11.92.5
04771-0-029
F
C
= 500kHz
V
O, dm
= 2V p-p
SECOND HARMONIC SOLID LINE
THIRD HARMONIC DASHED LINE
FREQUENCY (Hz)
V
OCM
NOISE (nV/√Hz)
1000
100
10
1
101001k10k100k1M10M100M
04771-0-047
FREQUENCY (MHz)
V
OCM
CMRR (dB)
–10
–30
–20
–50
–40
–70
–60
–80
110100
04771-0-012
V
O, cm
= 0.2V p-p
V
OCM
CMRR = ∆V
O, dm/∆VOCM
Figure 29. Harmonic Distortion vs. V
, VS = 5 V
OCM
Figure 30. Input Voltage Noise vs. Frequency
Figure 32. Harmonic Distortion vs. V
OCM
, VS = 3 V
Figure 33. V
Voltage Noise vs. Frequency
OCM
Figure 31. CMRR vs. Frequency
Figure 34. V
CMRR vs. Frequency
OCM
Rev. E | Page 15 of 32
AD8137 Data Sheet
TIME (ns)
VOLTAGE (V)
8
2
4
6
0
–4
–2
–6
–8
04771-0-016
250ns/DIV
INPUT
×
2
OUTPUT
G = 2
TIME (ns)
V
O, dm
(mV)
100
50
25
75
0
–25
–50
–75
–100
04771-0-015
10ns/DIV
V
O, dm
= 100mV p-p
CF = 0pF
C
F
= 1pF
TIME (ns)
V
O, dm
(V)
100
50
25
75
0
–50
–25
–75
–100
04771-0-039
20ns/DIV
RS = 111, CL= 5pF
RS = 60.4, C
L
= 15pF
2.0
–2.0
–1.5
–1.0
–0.5
0
0.5
1.5
1.0
04771-0-040
AMPLITUDE (V)
ERROR (V) 1DIV = 0.02%
C
F
= 0pF
V
O, dm
= 3.5V p-p
ERROR = V
O, dm
- INPUT
T
SETTLE
= 110ns
50ns/DIV
V
O, dm
INPUT
TIME (ns)
2V p-p
1V p-p
TIME (ns)
V
O, dm
(V)
1.5
1.0
–0.5
0
0.5
–1.0
–1.5
04771-0-014
C
F
= 0pF
C
F
= 1pF
C
F
= 0pF
C
F
= 1pF
20ns/DIV
TIME (ns)
V
O, dm
(V)
1.5
0.5
1.0
0
–0.5
–1.0
–1.5
04771-0-038
20ns/DIV
R
S
= 111, CL= 5pF
R
S
= 60.4, CL= 15pF
Figure 35. Overdrive Recovery
Figure 36. Small Signal Transient Response for Various Feedback
Capacitances
Figure 38. Settling Time (0.02%)
Figure 39. Large Signal Transient Response for Various Feedback
Capacitances
Figure 37. Small Signal Transient Response for Various Capacitive Loads
Figure 40. Large Signal Transient Response for Various Capacitive Loads
Rev. E | Page 16 of 32
Data Sheet AD8137
FREQUENCY (MHz)
PSRR (dB)
–5
–25
–35
–15
–45
–65
–55
–85
–75
0.1110100
04771-0-011
PSRR = ∆V
O, dm/∆VS
–PSRR
+PSRR
1101001000
FREQUENCY (MHz)
CLOSED-LOOP GAIN (dB)
V
O, dm
= 0.1V p-p
1
0
–1
–2
–14
–13
–12
–11
–10
–9
–8
–7
–6
–5
–4
–3
04771-0-010
VS = +3
V
S
= +5
V
S
= ±5
700
–700
–600
–500
–400
–300
–200
–100
0
100
200
300
400
500
600
2001k10k
04771-0-049
RESISTIVE LOAD (Ω)
SINGLE-ENDED OUTPUT SWING FROM RAIL (mV)
VS+– V
OP
VON– V
S–
VS = +3V
V
S
= +5V
FREQUENCY (MHz)
OUTPUT IMPEDANCE (Ω)
1000
100
10
1
0.1
0.01
0.011001010.1
04771-0-061
TIME (ns)
V
O, cm
(V)
4.0
3.0
3.5
2.5
1.5
2.0
1.0
04771-0-050
20ns/DIV
2V p-p
1V p-p
320
350
–330
–325
–320
–315
–310
–305
–300
345
340
335
330
325
–40–20020406080100120
04771-0-065
TEMPERATURE (°C)
V
OP
SWING FROM RAIL (mV)
V
ON
SWING FROM RAIL (mV)
VON– VS–
VS+ – V
OP
Figure 42. V
Figure 41. PSRR vs. Frequency
Small Signal Frequency Response for Various Supply Voltages
OCM
Figure 44. Single-Ended Output Impedance vs. Frequency
Figure 45. V
Large Signal Transient Response
OCM
Figure 43. Output Saturation Voltage vs. Output Load
Figure 46. Output Saturation Voltage vs. Temperature
Rev. E | Page 17 of 32
AD8137 Data Sheet
–0.3
0.3
–15
10
5
0
5
10
15
0.2
0.1
0
–0.1
–0.2
–40–20020406080100120
04771-0-052
TEMPERATURE (°
C)
V
OS, dm
(mV)
V
OS, cm
(mV)
V
OS, cm
V
OS, dm
V
ACM
(V)
INPUT BIAS CURRENT (µA)
1.2
1.0
0.6
0.8
0.4
0.2
–0.2
0
–0.4
0.501.502.503.504.50
04771-0-059
0.10
0.40
–3
–2
–1
0
1
2
3
0.35
0.30
0.25
0.20
0.15
–40–20020406080100120
04771-0-053
TEMPERATURE (°C)
I
BIAS
(µA)
I
OS
(nA)
I
BIAS
I
OS
TEMPERATURE (°C)
SUPPLY CURRENT (mA)
2.60
2.55
2.45
2.40
2.50
2.35
2.30
–40020–20408010060120
04771-0-051
V
OCM
(V)
I
V
OCM
(µA)
70�
50
30
10
–10
–30
–50
–70
00.5 1.01.5 2.02.5 3.0 3.5
4.0 4.55.0
04771-0-056
–0.5
–0.1
–0.2
–0.3
–0.4
–40–20020406080100120
04771-0-054
TEMPERATURE (°C)
V
OCM
CURRENT (µA)
Figure 47. Offset Voltage vs. Temperature
Figure 48. Input Bias Current vs. Input Common-Mode Voltage, V
ACM
Figure 50. Supply Current vs. Temperature
Figure 51. V
Bias Current vs. V
OCM
Input Voltage
OCM
Figure 49. Input Bias and Offset Current vs. Temperature
Rev. E | Page 18 of 32
Figure 52. V
Bias Current vs. Temperature
OCM
Data Sheet AD8137
V
OCM
V
O, cm
5
4
2
3
0
1
–1
–4
–3
–2
–5
–5 –4–3–2–1432105
04771-0-060
VS = +3V
V
S
= +5V
VS = ±5V
PD VOLTAGE (V)
PD CURRENT (µA)
40�
20
0
–20
–40
–60
–80
–100
–120
00.5 1.01.5 2.02.5 3.0 3.5 4.0 4.5
5.0
04771-0-057
PD VOLTAGE (V)
SUPPLY CURRENT (mA)
3
2
1
0
–1
–2
–3
00.5 1.01.5 2.02.5 3.0 3.5 4.0 4.5 5.0
04771-0-058
IS+
I
S
–
PD
–2.0V
–0.5V
V
O, dm
2µs/DIV
VS = ±
2.5V
G = 1 (R
F
= RG = 1kΩ)
R
L, dm
= 1kΩ
INPUT = 1Vp-p @ 1MHz
TIME (µs)
SUPPLY CURRENT (mA)
1.5
1.0
0.5
–0.5
0
–1.0
–1.5
04771-0-066
TIME (ns)
SUPPLY CURRENT (mA)
3.6
3.2
2.8
2.0
2.4
0.8
1.2
1.6
0.4
0
04771-0-024
100ns/DIV
PD (0.8V TO 1.5V)
TIME (ns)
SUPPLY CURRENT (mA)
3.4
3.0
2.6
2.2
1.8
1.4
1.0
0.6
0.2
04771-0-025
40ns/DIV
PD (1.5V TO 0.8V)
Figure 53. V
O, cm
vs. V
Input Voltage
OCM
Figure 56. Power-Down Transient Response
Figure 54. PD Current vs. PD Voltage
Figure 55. Supply Current vs. PD Voltage
Figure 57. Power-Down Turn-On Time
Figure 58. Power-Down Turn-Off Time
Rev. E | Page 19 of 32
AD8137 Data Sheet
04771-071
0
5
10
15
20
25
–5–4–3–2–1012345
SUPPLY CURRENT (mA)
POWER-DOWN VOLTAGE (V)
VS = ±5V
V
OCM
= 0V
G = +1
Figure 59. Supply Current vs. Power-Down Voltage
Rev. E | Page 20 of 32
Data Sheet AD8137
AD8137
+
–
52.3Ω
52.3Ω
R
L, dm
1kΩ V
O, dm
+
–
V
OCM
R
F
C
F
R
F
V
TEST
TEST
SIGNAL
SOURCE
50Ω
50Ω
04771-0-023
R
G
= 1kΩ
R
G
= 1kΩ
C
F
MIDSUPPLY
AD8137
+
–
52.3Ω
52.3Ω
R
L, dm
V
O, dm
+
–
R
F
= 1kΩ
R
F
= 1kΩ
R
S
R
S
V
TEST
TEST
SIGNAL
SOURCE
50Ω
50Ω
04771-0-062
C
L, dm
RG= 1kΩ
RG= 1kΩ
V
OCM
MIDSUPPLY
TEST CIRCUITS
Figure 60. Basic Test Circuit
Figure 61. Capacitive Load Test Circuit, G = 1
Rev. E | Page 21 of 32
AD8137 Data Sheet
–OUT+IN
A
CM
V
OCM
C
C
C
C
CP+OUT–IN CN
04771-0-017
C
m
C
g
BW×π=
2
FREQUENCY (MHz)
100
80
–60
–40
–20
0
20
40
60
–120
–100
–80
–200
–180
–160
–140
0.00010.010.0010.1110100
04771-0-021
OPEN-LOOP GAIN (dB)
PHASE (DEGREES)
THEORY OF OPERATION
The AD8137 is a low power, low cost, fully differential voltage
feedback amplifier that features a rail-to-rail output stage,
common-mode circuitry with an internally derived commonmode reference voltage, and bias shutdown circuitry. The amplifier
uses two feedback loops to separately control differential and
common-mode feedback. The differential gain is set with external
resistors as in a traditional amplifier, and the output commonmode voltage is set by an internal feedback loop, controlled by
an external V
arbitrarily the output common-mode voltage level without
affecting the differential gain of the amplifier.
input. This architecture makes it easy to set
OCM
Figure 62. Block Diagram
From Figure 62, the input transconductance stage is an H-bridge
whose output current is mirrored to high impedance nodes CP
and CN. The output section is traditional H-bridge driven circuitry
with common emitter devices driving nodes +OUT and −OUT.
The 3 dB point of the amplifier is defined as
where:
gm is the transconductance of the input stage.
C
is the total capacitance on node CP/CN (capacitances CP
C
and CN are well matched).
For the AD8137, the input stage g
capacitance C
is 3.5 pF, setting the crossover frequency of the
C
is ~1 mA/V and the
m
amplifier at 41 MHz. This frequency generally establishes an
amplifier’s unity gain bandwidth, but with the AD8137, the
closed-loop bandwidth depends upon the feedback resistor
value as well (see Figure 17). The open-loop gain and phase
simulations are shown in Figure 63.
Rev. E | Page 22 of 32
Figure 63. Open-Loop Gain and Phase
In Figure 62, the common-mode feedback amplifier ACM
samples the output common-mode voltage, and by negative
feedback forces the output common-mode voltage to be equal
to the voltage applied to the V
input. In other words, the
OCM
feedback loop servos the output common-mode voltage to the
voltage applied to the V
sets the V
level to approximately midsupply; therefore, the
OCM
input. An internal bias generator
OCM
output common-mode voltage is set to approximately midsupply
when the V
input is left floating. The source resistance of the
OCM
internal bias generator is large and can be overridden easily by an
external voltage supplied by a source with a relatively small output
resistance. The V
input can be driven to within approximately
OCM
1 V of the supply rails while maintaining linear operation in the
common-mode feedback loop.
The common-mode feedback loop inside the AD8137 produces
outputs that are highly balanced over a wide frequency range
without the requirement of tightly matched external components,
because it forces the signal component of the output commonmode voltage to be zeroed. The result is nearly perfectly balanced
differential outputs of identical amplitude and exactly 180°
apart in phase.
Data Sheet AD8137
04771-0-055
+
–
V
AP
V
AN
V
ON
V
OP
–
+
V
O, dm
R
L, dm
AD8137
C
F
R
F
R
G
R
G
C
F
R
F
V
IP
V
OCM
V
IN
2
,
ONOP
cmO
VVV+
=
dmO
cmO
V
V
BalanceOutput
,
,
∆
∆
=
2
, dmO
OCMOP
V
VV+=
2
, dmO
OCMON
V
VV−=
APPLICATIONS INFORMATION
ANALYZING A TYPICAL APPLICATION WITH
MATCHED R
Typical Connection and Definition of Terms
Figure 64 shows a typical connection for the AD8137, using
matched external R
terminals of the AD8137, V
junctions. An external reference voltage applied to the V
terminal sets the output common-mode voltage. The two
output terminals, V
in a balanced fashion in response to an input signal.
The differential output voltage is defined as
V
O, dm
Common-mode voltage is the average of two voltages. The
output common-mode voltage is defined as
Output Balance
Output balance is a measure of how well VOP and VON are
matched in amplitude and how precisely they are 180° out of
phase with each other. It is the internal common-mode feedback
loop that forces the signal component of the output commonmode toward zero, resulting in the near perfectly balanced
differential outputs of identical amplitude and are exactly 180°
out of phase. The output balance performance does not require
tightly matched external components, nor does it require that
the feedback factors of each loop be equal to each other. Low
frequency output balance is ultimately limited by the mismatch
of an on-chip voltage divider.
AND RG NETWORKS
F
networks. The differential input
F/RG
and VAN, are used as summing
AP
OCM
and VON, move in opposite directions
OP
Figure 64. Typical Connection
= VOP − VON (1)
(2)
Output balance is measured by placing a well-matched resistor
divider across the differential voltage outputs and comparing
the signal at the divider’s midpoint with the magnitude of the
differential output. By this definition, output balance is equal to
the magnitude of the change in output common-mode voltage
divided by the magnitude of the change in output differential
mode voltage:
(3)
The differential negative feedback drives the voltages at the summing
junctions V
V
and VAP to be essentially equal to each other.
AN
= VAP (4)
AN
The common-mode feedback loop drives the output commonmode voltage, sampled at the midpoint of the two internal
common-mode tap resistors in Figure 62, to equal the voltage
set at the V
terminal. This ensures that
OCM
(5)
and
(6)
ESTIMATING NOISE, GAIN, AND BANDWITH WITH
MATCHED FEEDBACK NETWORKS
Estimating Output Noise Voltage and Bandwidth
The total output noise is the root-sum-squared total of several
statistically independent sources. Because the sources are
statistically independent, the contributions of each must be
individually included in the root-sum-square calculation. Tab le 7
lists recommended resistor values and estimates of bandwidth
and output differential voltage noise for various closed-loop
gains. For most applications, 1% resistors are sufficient.
Table 7. Recommended Values of Gain-Setting Resistors and
Voltage Gain for Various Closed-Loop Gains
3 dB Bandwidth
Gain RG (Ω) RF (Ω)
(MHz)
1 1 k 1 k 72 18.6
2 1 k 2 k 40 28.9
5 1 k 5 k 12 60.1
10 1 k 10 k 6 112.0
Total Output
Noise (nV/√Hz)
Rev. E | Page 23 of 32
AD8137 Data Sheet
+=
G
F
n
R
R
vVo_n11
()
F
n
RiVo_n =2
=
G
F
G
R
R
TRVo_nk43
F
TRVo_nk44 =
F
ONAP
G
AP
IP
R
VV
R
VV−
=
−
+
==
G
F
G
OPAPAN
RR
R
VVV
i
G
F
dmO,
ONOP
V
R
R
VVV==−
G
F
G
RRR+
≡β
()
×
+
+
+
×
+
OCM
G
F
GINIP
G
F
F
V
RR
R
VV
RR
R
2
2
INIP
ICM
VVV+
≡
)(2
1
F
G
F
G
IN
RR
R
R
R
+
−
=
The differential output voltage noise contains contributions
from the AD8137’s input voltage noise and input current noise
as well as those from the external feedback networks.
The contribution from the input voltage noise spectral density
is computed as
Feedback Factor Notation
When working with differential drivers, it is convenient to
introduce the feedback factor β, which is defined as
(14)
, or equivalently, vn/β (7)
where v
is defined as the input-referred differential voltage
n
noise. This equation is the same as that of traditional op amps.
The contribution from the input current noise of each input is
computed as
(8)
where i
is defined as the input noise current of one input. Each
n
input needs to be treated separately because the two input currents
are statistically independent processes.
The contribution from each R
is computed as
G
(9)
This result can be intuitively viewed as the thermal noise of
each R
multiplied by the magnitude of the differential gain.
G
The contribution from each R
is computed as
F
(10)
Voltage Gain
The behavior of the node voltages of the single-ended-todifferential output topology can be deduced from the signal
definitions and Figure 64. Referring to Figure 64, C
setting V
= 0, one can write:
IN
= 0 and
F
(11)
(12)
Solving the previous two equations and setting V
the gain relationship for V
O, dm/Vi
.
to Vi gives
IP
(13)
An inverting configuration with the same gain magnitude can
be implemented by simply applying the input signal to V
setting V
V
IN, dm
= 0. For a balanced differential input, the gain from
IP
to V
is also equal to RF/RG, where V
O, dm
= VIP − VIN.
IN, dm
IN
and
This notation is consistent with conventional feedback analysis
and is very useful, particularly when the two feedback loops are
not matched.
Input Common-Mode Voltage
The linear range of the VAN and VAP terminals extends to within
approximately 1 V of either supply rail. Because V
and VAP are
AN
essentially equal to each other, they are both equal to the amplifier’s
input common-mode voltage. Their range is indicated in the
specifications tables as input common-mode range. The voltage
at V
and VAP for the connection diagram in Figure 64 can be
AN
expressed as
V
= VAP = V
AN
ACM
=
(15)
where V
is the common-mode voltage present at the amplifier
ACM
input terminals.
Using the β notation, Equation (15) can be written as
= βV
V
ACM
+ (1 − β)V
OCM
(16)
ICM
or equivalently,
= V
V
where V
ACM
ICM
+ β(V
ICM
is the common-mode voltage of the input signal,
OCM
− V
) (17)
ICM
that is
For proper operation, the voltages at V
and VAP must stay
AN
within their respective linear ranges.
Calculating Input Impedance
The input impedance of the circuit in Figure 64 depends on
whether the amplifier is being driven by a single-ended or a
differential signal source. For balanced differential input
signals, the differential input impedance (R
= 2RG (18)
R
IN, dm
For a single-ended signal (for example, when V
and the input signal drives V
), the input impedance becomes
IP
) is simply
IN, dm
IN
is grounded
(19)
Rev. E | Page 24 of 32
Data Sheet AD8137
04771-0-018
GND
V
REF
V
REFA
ADR525A
2.5V SHUNT
REFERENCE
AD7450A
VIN+
V
IN
–
VDD
AD8137
+
–
8
V
REFB
2.5V
2
1
6
3
4
5
V
OCM
1kΩ
1kΩ1kΩ
2.5kΩ
1kΩ
5V
50Ω
50Ω
V
IN
1.0nF
1.0nF
0.1µF
0.1µF
+1.88V
+1.25VV
ACM WITH
V
REFB
= 0
+0.63V
+2.5V
GND
–2.5V
04771-0-019
V
IN
0V TO 5V
AD8137
+
–
8
2
1
6
3
4
5
V
OCM
1kΩ
1kΩ
5V
1kΩ1kΩ
10kΩ
0.1µF
0.1µF
0.1µF
10µF
+
AD8031
+
–
0.1µF
5V
ADR525A
2.5V SHUNT
REFERENCE
TO
AD7450A
V
REF
)MHz72(,
3
×
+
=
−
F
G
G
dmO,dB
RR
R
Vf
Figure 65. AD8137 Driving AD7450A, 12-Bit ADC
The input impedance of a conventional inverting op amp
configuration is simply R
; however, it is higher in Equation 19
G
because a fraction of the differential output voltage appears at
the summing junctions, V
bootstraps the voltage across the input resistor R
and VAP. This voltage partially
AN
, leading to
G
the increased input resistance.
Input Common-Mode Swing Considerations
In some single-ended-to-differential applications, when using a
single-supply voltage, attention must be paid to the swing of the
input common-mode voltage, V
Consider the case in Figure 65, where V
about a baseline at ground and V
.
ACM
is 5 V p-p swinging
IN
is connected to ground.
REFB
The input signal to the AD8137 is originating from a source
with a very low output resistance.
The circuit has a differential gain of 1.0 and β = 0.5. V
amplitude of 2.5 V p-p and is swinging about ground. Using the
results in Equation 16, the common-mode voltage at the inputs of
the AD8137, V
, is a 1.25 V p-p signal swinging about a baseline
ACM
of 1.25 V. The maximum negative excursion of V
0.63 V, which exceeds the lower input common-mode voltage limit.
One way to avoid the input common-mode swing limitation is
to bias V
swinging about a baseline at 2.5 V, and V
low-Z 2.5 V source. V
and V
IN
at midsupply. In this case, VIN is 5 V p-p
REF
is connected to a
REF
now has an amplitude of 2.5 V p-p and
ICM
is swinging about 2.5 V. Using the results in Equation 17, V
is calculated to be equal to V
V
ICM
common-mode voltage limits of the AD8137. Another benefit
seen by this example is that because V
wasted common-mode current flows. Figure 66 illustrates a way
to provide the low-Z bias voltage. For situations that do not
require a precise reference, a simple voltage divider suffices to
develop the input voltage to the buffer.
swings from 1.25 V to 3.75 V, which is well within the input
because V
ICM
OCM
OCM
= V
ICM
in this case is
ACM
= V
. Therefore,
ICM
= V
ACM
has an
ACM
, no
ICM
Rev. E | Page 25 of 32
Figure 66. Low-Z Bias Source
Another way to avoid the input common-mode swing limitation
is to use dual power supplies on the AD8137. In this case, the
biasing circuitry is not required.
Bandwidth vs. Closed-Loop Gain
The 3 dB bandwidth of the AD8137 decreases proportionally
to increasing closed-loop gain in the same way as a traditional
voltage feedback operational amplifier. For closed-loop gains
greater than 4, the bandwidth obtained for a specific gain can
be estimated as
(20)
or equivalently, β(72 MHz).
This estimate assumes a minimum 90° phase margin for the
amplifier loop, a condition approached for gains greater than 4.
Lower gains show more bandwidth than predicted by the equation
due to the peaking produced by the lower phase margin.
AD8137 Data Sheet
+
=
G
G
F
IO
R
RR
VVo_e
1
()
F
IO
G
F
F
G
G
G
F
IO
RI
RR
RR
R
RR
IVo_e=
+
+
=2
Estimating DC Errors
Primary differential output offset errors in the AD8137 are due
to three major components: the input offset voltage, the offset
between the V
and VAP input currents interacting with the
AN
feedback network resistances, and the offset produced by the
dc voltage difference between the input and output commonmode voltages in conjunction with matching errors in the
feedback network.
The first output error component is calculated as
, or equivalently as VIO/β (21)
where V
is the input offset voltage.
IO
The second error is calculated as
(22)
where I
is defined as the offset between the two input bias
IO
currents.
The third error voltage is calculated as
− V
Vo_e3 = Δenr × (V
ICM
) (23)
OCM
where Δenr is the fractional mismatch between the two feedback
resistors.
The total differential offset error is the sum of these three error
sources.
Additional Impact of Mismatches in the Feedback Networks
The internal common-mode feedback network still forces the
output voltages to remain balanced, even when the R
F/RG
feedback networks are mismatched. The mismatch, however, causes
a gain error proportional to the feedback network mismatch.
Ratio-matching errors in the external resistors degrade the
ability to reject common-mode signals at the V
and VIN input
AN
terminals, similar to a four resistor, difference amplifier made
from a conventional op amp. Ratio-matching errors also produce a
differential output component that is equal to the V
OCM
input
voltage times the difference between the feedback factors (βs).
In most applications using 1% resistors, this component amounts
to a differential dc offset at the output that is small enough to
be ignored.
Driving a Capacitive Load
A purely capacitive load reacts with the bondwire and pin
inductance of the AD8137, resulting in high frequency ringing
in the transient response and loss of phase margin. One way to
minimize this effect is to place a small resistor in series with
each output to buffer the load capacitance. The resistor and load
capacitance forms a first-order, low-pass filter; therefore, the
resistor value should be as small as possible. In some cases, the
ADCs require small series resistors to be added on their inputs.
Figure 37 and Figure 40 illustrate transient response vs. capacitive
load and were generated using series resistors in each output
and a differential capacitive load.
Layout Considerations
Standard high speed PCB layout practices should be adhered
to when designing with the AD8137. A solid ground plane is
recommended and good wideband power supply decoupling
networks should be placed as close as possible to the supply pins.
To minimize stray capacitance at the summing nodes, the
copper in all layers under all traces and pads that connect to
the summing nodes should be removed. Small amounts of stray
summing-node capacitance cause peaking in the frequency
response, and large amounts can cause instability. If some stray
summing-node capacitance is unavoidable, its effects can be
compensated for by placing small capacitors across the feedback
resistors.
Terminating a Single-Ended Input
Controlled impedance interconnections are used in most high
speed signal applications, and they require at least one line
termination. In analog applications, a matched resistive termination
is generally placed at the load end of the line. This section deals
with how to properly terminate a single-ended input to the AD8137.
The input resistance presented by the AD8137 input circuitry
is seen in parallel with the termination resistor, and its loading
effect must be taken into account. The Thevenin equivalent
circuit of the driver, its source resistance, and the termination
resistance must all be included in the calculation as well. An
exact solution to the problem requires solution of several
simultaneous algebraic equations and is beyond the scope of
this data sheet. An iterative solution is also possible and is easier,
especially considering the fact that standard resistor values are
generally used.
Rev. E | Page 26 of 32
Data Sheet AD8137
AD8137
+
–
8
2
1
6
3
4
0V
2V p-p
R
T
52.3Ω
5
+
–
V
OCM
1kΩ
1.02kΩ
1kΩ
1kΩ
0.1µF
0.1µF
+5V
–5V
V
IN
SIGNAL
SOURCE
50Ω
04771-0-020
50kΩ
5kΩ
150kΩ
REF APD
–V
S
+V
S
+V
S
Q1Q2
04771-072
Figure 67 shows the AD8137 in a unity-gain configuration, and
with the following discussion, provides a good example of how
to provide a proper termination in a 50 Ω environment.
Figure 67. AD8137 with Terminated Input
The 52.3 Ω termination resistor, RT, in parallel with the 1 kΩ
input resistance of the AD8137 circuit, yields an overall input
resistance of 50 Ω that is seen by the signal source. To have
matched feedback loops, each loop must have the same R
has the same R
. In the input (upper) loop, RG is equal to the 1 kΩ
F
if it
G
resistor in series with the (+) input plus the parallel combination
of R
and the source resistance of 50 Ω. In the upper loop, RG is
T
therefore equal to 1.03 kΩ. The closest standard value is 1.02 kΩ
and is used for R
in the lower loop.
G
Things become more complicated when it comes to determining
the feedback resistor values. The amplitude of the signal source
generator V
is two times the amplitude of its output signal when
IN
terminated in 50 Ω. Therefore, a 2 V p-p terminated amplitude
is produced by a 4 V p-p amplitude from V
equivalent circuit of the signal source and R
calculating the closed-loop gain because R
. The Thevenin
S
must be used when
T
in the upper loop is
G
split between the 1 kΩ resistor and the Thevenin resistance
looking back toward the source. The Thevenin voltage of the
signal source is greater than the signal source output voltage
when terminated in 50 Ω because R
than 50 Ω. In this case, R
is 52.3 Ω and the Thevenin voltage
T
must always be greater
T
and resistance are 2.04 V p-p and 25.6 Ω, respectively.
Now the upper input branch can be viewed as a 2.04 V p-p
source in series with 1.03 kΩ. Because this is to be a unity-gain
application, a 2 V p-p differential output is required, and R
F
must therefore be 1.03 kΩ × (2/2.04) = 1.01 kΩ ≈ 1 kΩ.
This example shows that when R
the gain reduction produced by the increase in R
cancelled by the increase in the Thevenin voltage caused by R
and RG are large compared to RT,
F
is essentially
G
T
being greater than the output resistance of the signal source. In
general, as R
R
needs to be increased to compensate for the increase in RG.
F
When generating the typical performance characteristics data,
the measurements were calibrated to take the effects of the
terminations on closed-loop gain into account.
and RG become smaller in terminated applications,
F
Rev. E | Page 27 of 32
Power-Down
The AD8137 features a PD pin that can be used to minimize the
quiescent current consumed when the device is not being used.
PD
is asserted by applying a low logic level to Pin 7. The threshold
between high and low logic levels is nominally 1.1 V above the
negative supply rail. See
The AD8137
PD
enables the amplifier for normal operation. The AD8137
Tabl e 1 to Table 3 for the threshold limits.
pin features an internal pull-up network that
PD
pin can be left floating (that is, no external connection is
required) and does not require an external pull-up resistor to
ensure normal on operation (see Figure 68).
Do not connect the
PD
pin directly to VS+ in ±5 V applications.
This can cause the amplifier to draw excessive supply current
(see Figure 59) and may induce oscillations and/or stability
issues.
PD
Figure 68.
Pin Circuit
DRIVING AN ADC WITH GREATER THAN 12-BIT
PERFORMANCE
Because the AD8137 is suitable for 12-bit systems, it is desirable
to measure the performance of the amplifier in a system with
greater than 12-bit linearity. In particular, the effective number
of bits (ENOB) is most interesting. The AD7687, 16-bit, 250 KSPS
ADC performance makes it an ideal candidate for showcasing
the 12-bit performance of the AD8137.
For this application, the AD8137 is set in a gain of 2 and driven
single-ended through a 20 kHz band-pass filter, while the output
is taken differentially to the input of the AD7687 (see Figure 69).
This circuit has mismatched R
dc offset at the differential output. It is included as a test circuit to
illustrate the performance of the AD8137. Actual application
circuits should have matched feedback networks.
For an AD7687 input range up to −1.82 dBFS, the AD8137 power
supply is a single 5 V applied to V
increase the AD7687 input range to −0.45 dBFS, the AD8137
supplies are increased to +6 V and −1 V. In both cases, the V
pin is biased with 2.5 V and the
supplies are decoupled with 0.1 µF capacitors. Figure 70 and
Figure 71 show the performance of the −1.82 dBFS setup and the
Figure 70. AD8137 Performance on Single 5 V Supply, −1.82 dBFS
Figure 71. AD8137 Performance on +6 V, −1 V Supplies, −0.45 dBFS
Rev. E | Page 28 of 32
Data Sheet AD8137
CONTROLLING DIMENSIONS ARE IN MILLIMETERS; INCH DIMENSIONS
(IN PARENTHESES) ARE ROUNDED-OFF MILLIMETER EQUIVALENTS FOR
REFERENCE ONLYAND ARE NOT APPROPRIATE FOR USE IN DESIGN.
COMPLIANT TO JEDEC STANDARDS MS-012-AA
012407-A
0.25 (0.0098)
0.17 (0.0067)
1.27 (0.0500)
0.40 (0.0157)
0.50 (0.0196)
0.25 (0.0099)
45°
8°
0°
1.75 (0.0688)
1.35 (0.0532)
SEATING
PLANE
0.25 (0.0098)
0.10 (0.0040)
4
1
85
5.00(0.1968)
4.80(0.1890)
4.00 (0.1574)
3.80 (0.1497)
1.27 (0.0500)
BSC
6.20 (0.2441)
5.80 (0.2284)
0.51 (0.0201)
0.31 (0.0122)
COPLANARITY
0.10
TOP VIEW
8
1
5
4
0.30
0.25
0.20
BOTTOM VIEW
PIN 1 INDEX
AREA
SEATING
PLANE
0.80
0.75
0.70
1.55
1.45
1.35
1.84
1.74
1.64
0.203 REF
0.05 MAX
0.02 NOM
0.50 BSC
EXPOSED
PAD
3.10
3.00 SQ
2.90
FOR PROPER CONNECTION OF
THE EXPOSED PAD, REFER TO
THE PIN CONFIGURATION AND
FUNCTION DESCRIPTIONS
SECTION OF THIS DATA SHEET.
COPLANARITY
0.08
0.50
0.40
0.30
COMPLIANT
TO
JEDEC STANDARDS MO-229-WEED
12-07-2010-A
PIN 1
INDICATOR
(R 0.15)
OUTLINE DIMENSIONS
Figure 72. 8-Lead Standard Small Outline Package [SOIC_N]
Narrow Body
(R-8)
Dimensions shown in millimeters and (inches)
Figure 73. 8-Lead Lead Frame Chip Scale Package [LFCSP_WD]
3 mm × 3 mm Body, Very Very Thin, Dual Lead
(CP-8-13)
Dimensions shown in millimeters
Rev. E | Page 29 of 32
AD8137 Data Sheet
AD8137YCPZ-R2
–40°C to +125°C
8-Lead Lead Frame Chip Scale Package (LFCSP_WD)
CP-8-13
HFB#
ORDERING GUIDE
1, 2
Model
AD8137YR −40°C to +125°C 8-Lead Standard Small Outline Package (SOIC_N) R-8
AD8137YR-REEL7 −40°C to +125°C 8-Lead Standard Small Outline Package (SOIC_N) R-8
AD8137YRZ −40°C to +125°C 8-Lead Standard Small Outline Package (SOIC_N) R-8
AD8137YRZ-REEL −40°C to +125°C 8-Lead Standard Small Outline Package (SOIC_N) R-8
AD8137YRZ-REEL7 −40°C to +125°C 8-Lead Standard Small Outline Package (SOIC_N) R-8
AD8137YCPZ-REEL –40°C to +125°C 8-Lead Lead Frame Chip Scale Package (LFCSP_WD) CP-8-13 HFB#
AD8137YCPZ-REEL7 –40°C to +125°C 8-Lead Lead Frame Chip Scale Package (LFCSP_WD) CP-8-13 HFB#
AD8137WYCPZ-R7 –40°C to +125°C 8-Lead Lead Frame Chip Scale Package (LFCSP_WD) CP-8-13 H2G
AD8137YCP-EBZ LFCSP Evaluation Board
AD8137YR-EBZ SOIC Evaluation Board
1
Z = RoHS Compliant Part; # denotes that RoHS part may be top or bottom marked.
2
W = Qualified for Automotive Applications.
AUTOMOTIVE PRODUCTS
The AD8137W models are available with controlled manufacturing to support the quality and reliability requirements of automotive
applications. Note that these automotive models may have specifications that differ from the commercial models; therefore, designers
should review the Specifications section of this data sheet carefully. Only the automotive grade products shown are available for use in
automotive applications. Contact your local Analog Devices account representative for specific product ordering information and to
obtain the specific Automotive Reliability reports for these models.
Temperature Range Package Description Package Option Branding