OPA843IDBVT [TI]
Wideband, Low Distortion, Medium Gain Voltage-Feedback OPERATIONAL AMPLIFIER;
| 型号： | OPA843IDBVT |
| 厂家： | 
TEXAS INSTRUMENTS |
| 描述： | Wideband, Low Distortion, Medium Gain Voltage-Feedback OPERATIONAL AMPLIFIER 放大器 光电二极管 |
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OPA843
O
P
A
8
4
3
www.ti.com
SBOS268C – DECEMBER 2002 – DECEMBER 2008
Wideband, Low Distortion, Medium Gain,
Voltage-Feedback OPERATIONAL AMPLIFIER
DESCRIPTION
FEATURES
The OPA843 provides a level of speed and dynamic range
previously unattainable in a monolithic op amp. Using a high
Gain Bandwidth (GBW), two gain-stage design, the OPA843
gives a medium gain range device with exceptional dynamic
range. The “classic” differential input complements this high
dynamic range with DC precision beyond most high-speed
amplifier products. Very low input offset voltage and current,
high Common-Mode Rejection Ratio (CMRR) and Power-
Supply Rejection Ratio (PSRR), and high open-loop gain
combine to give a high DC precision amplifier along with low
noise and high 3rd-order intercept.
● HIGH BANDWIDTH: 260MHz (G = +5)
● GAIN BANDWIDTH PRODUCT: 800MHz
● LOW INPUT VOLTAGE NOISE: 2.0nV/√Hz
● VERY LOW DISTORTION: –96dBc (5MHz)
● HIGH OPEN-LOOP GAIN: 110dB
● FAST 12-BIT SETTLING: 10.5ns (0.01%)
● LOW INPUT OFFSET VOLTAGE: 300µV
● OUTPUT CURRENT: ±100mA
12- to 16-bit converter interfaces will benefit from this combi-
nation of features. High-speed transimpedance applications
can be implemented with exceptional DC precision as well.
Differential configurations using two OPA843s can deliver
very low distortion to high output voltages, as shown below.
APPLICATIONS
● ADC/DAC BUFFER AMPLIFIER
● LOW DISTORTION “IF” AMPLIFIER
● ACTIVE FILTERS
● LOW-NOISE RECEIVER
OPA843 RELATED PRODUCTS
● WIDEBAND TRANSIMPEDANCE
● TEST INSTRUMENTATION
● PROFESSIONAL AUDIO
INPUT NOISE
GAIN-BANDWIDTH
PRODUCT (MHz)
√Hz
SINGLES
VOLTAGE (nV/
)
OPA842
OPA846
OPA847
2.6
1.2
200
1750
3900
0.85
● OPA643 UPGRADE
+5V
DIFFERENTIAL DISTORTION vs OUTPUT VOLTAGE
OPA843
–85
–90
GD = 10
RL = 400Ω
F = 5MHz
–5V
40.2Ω
40.2Ω
402Ω
1:1
VI
–95
RL
132Ω
VO = 10VI
50Ω
2nd-Harmonic
402Ω
400Ω
–100
–105
–110
3rd-Harmonic
+5V
OPA843
1
10
–5V
Output Voltage Swing (Vp-p)
Very Low Distortion Differential Driver
Please be aware that an important notice concerning availability, standard warranty, and use in critical applications of
Texas Instruments semiconductor products and disclaimers thereto appears at the end of this data sheet.
All trademarks are the property of their respective owners.
PRODUCTION DATA information is current as of publication date.
Products conform to specifications per the terms of Texas Instruments
standard warranty. Production processing does not necessarily include
testing of all parameters.
Copyright © 2002-2008, Texas Instruments Incorporated
www.ti.com
ABSOLUTE MAXIMUM RATINGS(1)
Power Supply ............................................................................... ±6.5VDC
ELECTROSTATIC
Internal Power Dissipation...................................... See Thermal Analysis
DISCHARGE SENSITIVITY
Differential Input Voltage .................................................................. ±1.2V
Input Voltage Range............................................................................ ±VS
Storage Voltage Range: D, DBV ...................................–65°C to +125°C
Lead Temperature (soldering, 10s)............................................... +300°C
Junction Temperature (TJ) ............................................................ +150°C
ESD Rating (Human Body Model) .................................................. 2000V
(Charge Device Model) ............................................... 1500V
This integrated circuit can be damaged by ESD. Texas Instru-
ments 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 degrada-
tion 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.
(Machine Model) ........................................................... 200V
NOTE: (1) Stresses above these ratings may cause permanent damage.
Exposure to absolute maximum conditions for extended periods may degrade
device reliability. These are stress ratings only, and functional operation of the
device at these or any other conditions beyond those specified is not implied.
(1)
PACKAGE/ORDERING INFORMATION
SPECIFIED
PACKAGE
DESIGNATOR
TEMPERATURE
RANGE
PACKAGE
MARKING
ORDERING
NUMBER
TRANSPORT
MEDIA, QUANTITY
PRODUCT
PACKAGE-LEAD
OPA843
SO-8
D
"
–40°C to +85°C
OPA843
OPA843ID
OPA843IDR
Rails, 100
"
OPA843
"
"
"
"
OARI
"
Tape and Reel, 2500
Tape and Reel, 250
Tape and Reel, 3000
SOT23-5
DBV
–40°C to +85°C
OPA843IDBVT
OPA843IDBVR
"
"
"
NOTE: (1) For the most current package and ordering information, see the Package Option Addendum at the end of this document, or see the TI website at www.ti.com.
PIN CONFIGURATIONS
Top View
SOT
Top View
SO
Output
1
5
4
+VS
–VS
2
3
Noninverting Input
Inverting Input
NC
1
8
NC
Inverting Input
2
3
4
7
6
5
+VS
Noninverting Input
Output
NC
–VS
NC = No Connection
OARI
Pin Orientation/Package Marking
OPA843
2
SBOS268C
www.ti.com
ELECTRICAL CHARACTERISTICS: VS = ±5V
Boldface limits are tested at +25°C.
At TA = +25°C, VS = ±5V, RF = 402Ω, RL = 100Ω, and G = +5, unless otherwise noted. See Figure 1 for AC performance.
OPA843ID, OPA843IDBV
MIN/MAX OVER TEMPERATURE
TYP
0
°
C to
–40
°
C to
MIN/
MAX
TEST
LEVEL(3 )
PARAMETER
CONDITIONS
+25°C
+25°C(1)
70°C
+85°C(2)
UNITS
AC PERFORMANCE (see Figure 1)
Small-Signal Bandwidth (VO = 200mVPP
)
G = +3
G = +5
G = +10
G = +20
500
260
85
40
800
65
MHz
MHz
MHz
MHz
MHz
MHz
dB
typ
min
min
min
min
min
typ
C
B
B
B
B
B
C
185
66
30
562
34
180
65
30
560
33
175
64
30
558
32
Gain-Bandwidth Product
Bandwidth for 0.1dB Gain Flatness
Peaking at a Gain of +3
Harmonic Distortion
G = +5, RL = 100Ω, VO = 200mVPP
3.5
G = +5, f = 5MHz, VO = 2VPP
RL = 100Ω
2nd-Harmonic
–76
–96
–102
–110
40
2.0
2.8
1.2
1000
10.5
7.5
3.2
0.001
0.012
–74
–94
–100
–105
–72
–92
–98
–70
–90
–95
dBc
dBc
dBc
dBc
dBm
max
max
max
max
typ
max
max
max
min
typ
B
B
B
B
C
B
B
B
B
C
B
B
C
C
RL = 500Ω
RL = 100Ω
L = 500Ω
G = +5, f = 25MHz
f > 1MHz
3rd-Harmonic
R
–102
–100
2-Tone, 3rd-Order Intercept
Input Voltage Noise
Input Current Noise
Rise-and-Fall Time
Slew Rate
Settling Time to 0.01%
0.1%
1.0%
Differential Gain
Differential Phase
√Hz
√Hz
2.2
3.35
1.95
650
2.31
3.4
2.0
2.36
3.45
2.1
nV/
pA/
f > 1MHz
0.2V Step
2V Step
2V Step
ns
V/µs
ns
ns
ns
600
525
2V Step
2V Step
G = +4, NTSC, RL = 150Ω
G = +4, NTSC, RL = 150Ω
10
5.4
10.3
5.8
10.6
6.4
max
max
typ
%
deg
typ
DC PERFORMANCE(4)
Open-Loop Voltage Gain (AOL
Input Offset Voltage
Average Offset Voltage Drift
Input Bias Current
Input Bias Current Drift
Input Offset Current
)
VO = 0V
110
±0.30
100
±1.20
96
±1.4
±4
–36
25
92
±1.5
±4
–37
25
dB
mV
µV/°C
µA
nA/°C
µA
nA/°C
min
max
max
max
max
max
max
A
A
B
A
B
A
B
V
CM = 0V
VCM = 0V
V
V
CM = 0V
CM = 0V
–20
–35
VCM = 0V
CM = 0V
±0.25
±1.0
±1.15
±2
±1.17
±2
Input Offset Current Drift
V
INPUT
Common-Mode Input Range (CMIR)(5)
Common-Mode Rejection (CMRR)
Input Impedance
±3.2
95
±3.0
85
±2.9
84
±2.8
82
V
dB
min
min
A
A
VCM = ±1V, Input Referred
Differential-Mode
Common-Mode
VCM = 0V
12 || 1
3.2 || 1.2
kΩ || pF
MΩ || pF
typ
typ
C
C
V
CM = 0V
OUTPUT
Output Voltage Swing
R
L > 1kΩ, Positive Output
3.2
–3.7
3.0
–3.5
±100
0.0001
3.0
–3.5
2.8
–3.3
±90
2.9
–3.4
2.7
–3.2
±85
2.8
–3.3
2.6
–3.1
±80
V
V
V
V
mA
Ω
min
min
min
min
min
typ
A
A
A
A
A
C
RL > 1kΩ, Negative Output
RL = 100Ω, Positive Output
RL = 100Ω, Negative Output
VO = 0V
Current Output
Closed-Loop Output Impedance
G = +5, f = 1kHz
POWER SUPPLY
Specified Operating Voltage
Maximum Operating Voltage
Minimum Operating Voltage
Max Quiescent Current
Min Quiescent Current
Power-Supply Rejection Ratio
(+PSRR, –PSRR)
±5
V
V
V
mA
mA
typ
max
min
max
min
C
A
A
A
A
±6
±4
20.8
±6
±4
22.2
19.1
±6
±4
22.5
18.3
V
V
S = ±5V
S = ±5V
20.2
20.2
19.6
|VS| = 4.5V to 5.5V, Input Referred
100
90
88
85
dB
min
typ
A
C
THERMAL CHARACTERISTICS
Specified Operating Range: D, DBV
Thermal Resistance, θJA
–40 to +85
°C
Junction-to-Ambient
D
SO-8
125
150
°C
°C
typ
typ
C
C
DBV SOT23-5
NOTES: (1) Junction temperature = ambient temperature for 25°C min/max specifications. (2) Junction temperature = ambient at low temperature limit: junction
temperature = ambient +23°C at high temperature limit for over temperature min/max specifications. (3) Test Levels: (A) 100% tested at 25°C over-temperature
limits by characterization and simulation. (B) Limits set by characterization and simulation. (C) Typical value only for information. (4) Current is considered positive out-
of-node. VCM is the input common-mode voltage. (5) Tested < 3dB below minimum specified CMRR at ±CMIR limits.
OPA843
SBOS268C
3
www.ti.com
TYPICAL CHARACTERISTICS: VS = ±5V
TA = +25°C, G = +5, RF = 402Ω, RG = 100Ω, and RL = 100Ω, unless otherwise noted.
NONINVERTING SMALL-SIGNAL
FREQUENCY RESPONSE
INVERTING SMALL-SIGNAL
FREQUENCY RESPONSE
6
3
3
0
G = –4
VO = 0.2Vp-p
G = +3
G = +5
G = –8
RG = RS = 50Ω
VO = 0.2Vp-p
0
–3
–3
G = +10
G = +20
–6
–6
–9
–9
G = –16
G = –32
–12
–15
–18
–12
–15
–18
See Figure 1
106
See Figure 2
107
109
106
107
10
109
8
10
8
Frequency (Hz)
Frequency (Hz)
INVERTING LARGE-SIGNAL
FREQUENCY RESPONSE
NONINVERTING LARGE-SIGNAL
FREQUENCY RESPONSE
21
18
15
12
9
17
14
11
8
0.2Vp-p
1Vp-p
2Vp-p
RL = 100Ω
G = +5V/V
RL = 100Ω
G = –8V/V
200mVp-p
to 1Vp-p
5Vp-p
5Vp-p
6
2Vp-p
3
5
0
2
–3
–6
See Figure 2
107
See Figure 1
107
–1
108
109
108
Frequency (Hz)
109
Frequency (Hz)
NONINVERTING PULSE RESPONSE
INVERTING PULSE RESPONSE
G = +5
G = –8
Large Signal ± 1V
Large Signal ± 1V
1.2
0.8
0.4
0
1.2
0.8
0.4
0
200
100
0
200
100
0
Right Scale
Right Scale
Small Signal ± 100mV
Small Signal ± 100mV
–100
–200
–100
–200
–0.4
–0.8
–1.2
–0.4
–0.8
–1.2
Left Scale
Left Scale
See Figure 2
See Figure 1
Time (2ns/div)
Time (2ns/div)
OPA843
4
SBOS268C
www.ti.com
TYPICAL CHARACTERISTICS: VS = ±5V (Cont.)
TA = +25°C, G = +5, RF = 402Ω, RG = 100Ω, and RL = 100Ω, unless otherwise noted.
5MHz HARMONIC DISTORTION vs LOAD RESISTANCE
1MHz HARMONIC DISTORTION vs LOAD RESISTANCE
–75
–80
–75
–80
VO = 2Vp-p
G = +5
VO = 5Vp-p
G = +5
–85
–85
2nd-Harmonic
–90
–90
2nd-Harmonic
–95
–95
–100
–105
–110
–100
–105
–110
3rd-Harmonic
3rd-Harmonic
See Figure 1
400 450 500
See Figure 1
400 450 500
100
150
200
250
300
350
100
150
200
250
300
350
Resistance (Ω)
Resistance (Ω)
HARMONIC DISTORTION vs OUTPUT VOLTAGE
RL = 200Ω
F = 5MHz
G = +5
HARMONIC DISTORTION vs FREQUENCY
VO = 2Vp-p
–70
–75
–60
–70
G = +5
RL = 200Ω
–80
2nd-Harmonic
–85
–80
2nd-Harmonic
–90
–90
–95
3rd-Harmonic
–100
–105
–110
–100
–110
3rd-Harmonic
See Figure 1
See Figure 1
0.1
1
10
0.1
1
10
100
Output Voltage Swing (Vp-p)
Frequency (MHz)
HARMONIC DISTORTION vs INVERTING GAIN
2nd-Harmonic
HARMONIC DISTORTION vs NONINVERTING GAIN
2nd-Harmonic
–75
–85
–70
–80
VO = 2Vp-p
RL = 200Ω
F = 5MHz
VO = 2Vp-p
–95
–90
RG = 50Ω, RF Adjusted
RL = 200Ω
F = 5MHz
RF = 402Ω, RG Adjusted
–105
–115
–100
–110
3rd-Harmonic
3rd-Harmonic
See Figure 2
30 35 40
See Figure 1
20
5
10
15
20
25
5
10
15
Gain (–V/V)
Gain (V/V)
OPA843
SBOS268C
5
www.ti.com
TYPICAL CHARACTERISTICS: VS = ±5V (Cont.)
TA = +25°C, G = +5, RF = 402Ω, RG = 100Ω, and RL = 100Ω, unless otherwise noted.
2-TONE, 3RD-ORDER
INPUT VOLTAGE AND CURRENT NOISE DENSITY
INTERMODULATION INTERCEPT
10
55
50
45
40
35
30
25
PI
G = +5
50Ω
PO
OPA843
50Ω
50Ω
402Ω
100Ω
Current Noise
2.8pA/√Hz
Voltage Noise
2.0nV/√Hz
1
102
103
104
105
106
107
10 15 20 25 30 35 40 45 50 55 60 65 70
Frequency (MHz)
Frequency (Hz)
NONINVERTING GAIN FLATNESS TUNE
VO = 200mVp-p
LOW GAIN INVERTING BANDWIDTH
VO = 200mVp-p
0.40
0.30
0.20
0.10
0
3
2
AV = +4
NG = 4
1
External Compensation
See Figure 10
G = –1
0
–1
–2
–3
–4
–5
–6
NG = 4.5
G = –2
–0.10
–0.20
–0.30
–0.40
NG = 5
NG = 5.5
G = –3
External Compensation
See Figure 11
1
10
100
1k
1
10
100
1k
Frequency (MHz)
Frequency (MHz)
FREQUENCY RESPONSE vs CAPACITIVE LOAD
RS adjusted to cap load.
RECOMMENDED RS vs CAPACITIVE LOAD
G = +5
17
14
11
8
100
10
1
C = 10pF
C = 100pF
C = 22pF
VI
RS
VO
OPA843
402Ω
50Ω
CL
1kΩ
C = 47pF
5
100Ω
1kΩ is optional.
2
106
107
108
109
1
10
100
1k
Frequency (Hz)
Capacitive Load (pF)
OPA843
6
SBOS268C
www.ti.com
TYPICAL CHARACTERISTICS: VS = ±5V (Cont.)
TA = +25°C, G = +5, RF = 402Ω, RG = 100Ω, and RL = 100Ω, unless otherwise noted.
OPEN-LOOP GAIN AND PHASE
CMRR AND PSRR vs FREQUENCY
+PSRR
120
100
80
0
120
100
80
60
40
20
0
–30
–60
–90
–120
–150
–180
–210
20log (AOL
)
CMRR
AOL
60
–PSRR
40
20
0
–20
101
102
103
104
105
106
107
108
109
101
102
103
104
105
106
107
108
Frequency (Hz)
Frequency (Hz)
CLOSED-LOOP OUTPUT IMPEDANCE
vs FREQUENCY
OUTPUT VOLTAGE AND CURRENT LIMITATIONS
10
1
4
3
OPA843
RL = 100
ZO
2
1W Internal
Power Limit
0.1
402Ω
100Ω
1
RL = 50
0.01
0
RL = 25
–1
–2
–3
–4
0.001
0.0001
0.00001
1W Internal
Power Limit
102
103
104
105
106
107
108
–0.15
–0.1
–0.05
0
0.05
0.1
0.15
Frequency (Hz)
IO (mA)
NONINVERTING OVERDRIVE RECOVERY
Input
INVERTING OVERDRIVE RECOVERY
5
1
5
4
1
RL = 100Ω
G = –8
See Figure 2
Input
RL = 100Ω
G = 5
See Figure 1
4
3
0.8
0.6
0.4
0.2
0
0.8
0.6
0.4
0.2
0
Right Scale
3
Output
Left Scale
2
2
Right Scale
1
1
0
0
Output
Left Scale
–1
–2
–3
–4
–5
–0.2
–0.4
–0.6
–0.8
–1
–1
–2
–3
–4
–5
–0.2
–0.4
–0.6
–0.8
–1
Time (40ns/div)
Time (40ns/div)
OPA843
SBOS268C
7
www.ti.com
TYPICAL CHARACTERISTICS: VS = ±5V (Cont.)
TA = +25°C, G = +5, RF = 402Ω, RG = 100Ω, and RL = 100Ω, unless otherwise noted.
SETTLING TIME
VIDEO DIFFERENTIAL GAIN/DIFFERENTIAL PHASE
G = +4
0.25
0.20
0.15
0.10
0.05
0
0.02
0.015
0.01
0.005
0
0.1
RL = 100Ω
VO = 2V step
G = +5
dG, Negative Video
0.075
0.05
0.025
0
dP, Negative Video
–0.05
–0.10
–0.15
–0.20
–0.25
dP, Positive Video
dG, Positive Video
See Figure 1
0
5
10
Time (ns)
15
20
25
1
2
3
4
5
Video Loads (150Ω each)
TYPICAL DC DRIFT OVER TEMPERATURE
SUPPLY AND OUTPUT CURRENT vs TEMPERATURE
1
0.5
0
25
110
106
102
98
22
21
20
19
18
17
12.5
0
Supply Current
VIO
Sourcing Output Current
100 x IOS
Sinking Output Current
–0.5
–1
–12.5
–25
94
IB
90
–50
–25
0
25
50
75
100
125
–50
–25
0
25
50
75
100
125
Ambient Temperature (°C)
Ambient Temperature (°C)
COMMON-MODE INPUT RANGE AND OUTPUT SWING
vs SUPPLY VOLTAGE
COMMON-MODE AND DIFFERENTIAL
INPUT IMPEDANCE
107
106
105
104
103
102
6
4
Positive Input
Common-Mode
2
Positive Output
0
Differential
–2
–4
–6
Negative Output
Negative Input
103
104
105
106
107
108
3
4
5
6
Frequency (Hz)
Supply Voltage (±V)
OPA843
8
SBOS268C
www.ti.com
TYPICAL CHARACTERISTICS: VS = ±5V (Cont.)
TA = +25°C, GD = 10, RF = 1kΩ, RG = 100Ω, and RL = 100Ω, unless otherwise noted.
DIFFERENTIAL PERFORMANCE
TEST CIRCUIT
DIFFERENTIAL SMALL-SIGNAL
FREQUENCY RESPONSE
3
0
VO = 400mVp-p
+5V
GD = 5
OPA843
GD = 10
GD = 16
RF
GD
=
–3
100Ω
–5V
RF
RG
100Ω
–6
GD = 32
–9
RG
100Ω
RL
VI
VO
RF
–12
–15
–18
+5V
OPA843
1
10
100
1k
Frequency (MHz)
–5V
DIFFERENTIAL LARGE-SIGNAL
FREQUENCY RESPONSE
DIFFERENTIAL DISTORTION vs LOAD RESISTANCE
VO = 4Vp-p
–70
23
20
17
14
11
8
GD = 10V/V
VO = 400mVp-p to 5Vp-p
–75 GD = 10
F = 5MHz
–80
–85
–90
2nd-Harmonic
VO = 8Vp-p
–95
–100
–105
3rd-Harmonic
–110
10
100
Load Resistance (Ω)
1k
10
100
200
Frequency (MHz)
DIFFERENTIAL DISTORTION vs FREQUENCY
VO = 4Vp-p
DIFFERENTIAL DISTORTION vs OUTPUT VOLTAGE
–60
–70
–80
–85
GD = 10
RL = 400Ω
F = 5MHz
GD = 10
RL = 400Ω
–90
–80
–95
2nd-Harmonic
2nd-Harmonic
–100
–105
–110
–115
–90
3rd-Harmonic
–100
–110
3rd-Harmonic
1
10
20
1
10
Frequency (Hz)
Output Voltage Swing (Vp-p)
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APPLICATIONS INFORMATION
+5V
WIDEBAND NONINVERTING OPERATION
The OPA843’s combination of speed and dynamic range is
useful in a wide variety of application circuits, as long as
simple guidelines common to all high-speed amplifiers are
observed. For example, good power-supply decoupling, as
shown in Figure 1, is essential to achieve the lowest possible
harmonic distortion and smooth frequency response. Careful
PC board layout and component selection will maximize the
performance of the OPA843 in all applications, as discussed
in the following sections of this data sheet. Figure 1 shows
the gain of +5 configuration used as the basis for most of the
Typical Characteristics. Most of the curves were character-
ized using signal sources with 50Ω driving impedance and
with measurement equipment presenting 50Ω load imped-
ance. In Figure 1, the 50Ω shunt resistor at the input terminal
matches the source impedance of the test generator, while
the 50Ω series resistor at the VO terminal provides a match-
ing resistor for the measurement equipment load. Generally,
data sheet specifications refer to the voltage swing at the
output pin (VO in Figure 1) while those referring to load power
are at the 50Ω load. The total 100Ω load from the series and
shunt matching resistors, combined with the 502Ω total
feedback network load, presents the OPA843 with an effec-
tive output load of approximately 83Ω.
+
0.1µF
2.2µF
50Ω Load
RS
50Ω
VO
RT
OPA843
RG
50Ω
RF
402Ω
50Ω Source
VI
RM
(optional)
0.1µF
2.2µF
+
–5V
FIGURE 2. Inverting G = –8 Specification and Test Circuit.
both the input termination resistor and the gain setting
resistor for the circuit. Although the signal gain for the circuit
of Figure 2 is equal to –8V/V (versus the +5V/V for Figure 1),
their noise gains are equal when the 50Ω source resistor is
included. This has the interesting effect of nearly doubling
the equivalent Gain Bandwidth Product (GBP) for the ampli-
fier. This can be seen in comparing the G = +5 and G = –8
small-signal frequency response curves. Both show approxi-
mately 260MHz bandwidth, but the inverting configuration of
Figure 2 is giving 4dB higher signal gain. If the signal source
is actually the low impedance output of another amplifier, RG
is increased to the minimum value allowed at the output of
that amplifier and RF is adjusted to get the desired gain. It is
critical for stable operation of the OPA843 that this driving
amplifier show a very low output impedance through frequen-
cies exceeding the expected closed-loop bandwidth for the
OPA843.
+5V
+VS
+
0.1µF
2.2µF
50Ω Source
50Ω Load
RS
50Ω
VIN
VO
50Ω
OPA843
RF
402Ω
An optional input termination resistor is also shown in Figure 2.
This RM resistor may be used to adjust the input impedance to
lower values when RG needs to be adjusted higher. This might
be desirable at lower gains where increasing RF will reduce the
output loading improving harmonic distortion performance. For
instance, at a gain of –4 an RG set to 50Ω will require a 200Ω
feedback resistor. In this case, adjusting RF to 400Ω, setting RG
to 100Ω, and then adding a 100Ω RM resistor will deliver a gain
of –4 with a 50Ω input match.
RG
100Ω
0.1µF
2.2µF
+
–VS
–5V
FIGURE 1. Gain of +5, High-Frequency Application and
Characterization Circuit.
BUFFERING HIGH-PERFORMANCE ADCs
WIDEBAND, INVERTING GAIN OPERATION
A single-channel interface using the OPA843 can provide a low
noise/distortion interface to emerging 14-bit Analog-to-Digital
Converters (ADCs) through approximately 5MHz for medium
gain applications. Since the dominant distortion mechanism is
2nd-harmonic distortion, differential circuits using the OPA843
can extend this frequency range and/or power level to much
higher levels. The example on the front page of this data sheet,
for instance, shows better than 93dB SFDR at 5MHz for up to
8VPP signals. This is still being limited by the 2nd-harmonic with
There can be significant benefits to operating the OPA843 as
an inverting amplifier. This is particularly true when a matched
input impedance is required. Figure 2 shows the inverting
gain circuit used as a starting point for the typical character-
istics showing inverting mode performance.
Driving this circuit from a 50Ω source, and constraining the
gain resistor, RG, to equal 50Ω will give both a signal
bandwidth and noise advantage. RG in this case is acting as
OPA843
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the 3rd-harmonic much lower. 2-tone 3rd-order intermodulation
terms will be much lower than most other solutions using the
circuit shown on the front page. The differential typical charac-
teristic curves also show that a 4VPP output will have
> 80dBc SFDR through 20MHz using this differential approach.
1dB through 50MHz. For narrowband IF’s in the 44MHz
region, this configuration of the OPA843 will show a 3rd-order
intercept of 33dBm while dissipating only 200mW (23dBm)
power from ±5V supplies.
PHOTODIODE TRANSIMPEDANCE AMPLIFIER
WIDE DYNAMIC RANGE “IF” AMPLIFIER
High Gain Bandwidth Product (GBP) and low input voltage
and current noise make the OPA843 an ideal wideband
transimpedance amplifier for low to moderate gains. Note
that unity-gain stability is not required for transimpedance
applications. Figure 4 shows an example photodiode ampli-
fier circuit. The key parameters of this design are the esti-
mated diode capacitance (CD) at the applied DC reverse bias
voltage (–VB), the desired transimpedance gain (RF), and the
GBP for the OPA843 (800MHz). With these three variables
set (and adding the OPA843’s parasitic input capacitance to
the value of CD to get CS), the feedback capacitor value (CF)
is selected to provide stability for the transimpedance fre-
quency response.
The OPA843 offers an attractive alternative to standard fixed-
gain IF amplifier stages. Narrowband systems will benefit from
the exceptionally high 2-tone 3rd-order intermodulation inter-
cept, as shown in the Typical Characteristics. Op amps with
high open-loop gain, like the OPA843, provide an intercept
that decreases with frequency along with the loop gain. The
OPA843’s 3rd-order intercept shows a decreasing intercept
with frequency. The OPA843’s intercept is > 30dBm up to
50MHz but improves to > 50dBm as the operating frequency
is reduced below 10MHz. Broadband systems will also benefit
from the very low even-order harmonics and intermodulation
components produced by the OPA843. Compared to standard
fixed-gain IF amplifiers, the OPA843 operating at IF’s below
50MHz provides much higher intercepts for its quiescent
power dissipation (200mW), superior gain accuracy, higher
reverse isolation, and lower I/O return loss. The noise figure
for the OPA843 will be higher than alternative fixed-gain
stages. If the application comes late in the amplifier chain with
significant gain in prior stages, this higher noise figure may be
acceptable. Figure 3 shows an example of a noninverting
configuration for the OPA843 used as an IF amplifier.
+5V
Power-supply decoupling
not shown.
0.01µF
10kΩ
VO = IDRF
OPA843
RF
10kΩ
–5V
λ
CF
0.75pF
CD
20pF
ID
Power-supply
+5V
decoupling not shown.
50Ω Source
0.01µF
RS
–VB
PI
50Ω Load
50Ω
VO
P0
OPA843
52.3Ω
1kΩ
FIGURE 3. High Dynamic Range IF Amplifier.
To achieve a maximally flat 2nd-order Butterworth frequency
response, the feedback pole should be set to:
RF
1kΩ
+5V
CS = CD + CI
RG
144Ω
1
GBP
=
(1)
2πRFCF
4πRFCS
0.01µF
Adding the OPA843’s common-mode and differential mode
input capacitances CI = (1.0 + 1.2)pF to the 20pF diode
source capacitance of Figure 4, and targeting a 10kΩ tran-
simpedance gain using the 800MHz GBP for the OPA843,
the required feedback pole frequency is 16.9MHz. This will
require a total feedback capacitance of 0.94pF. Typical
surface-mount resistors have a parasitic capacitance of
0.2pF, leaving the required 0.75pF value shown in Figure 4
to get the required feedback pole.
PI
RF
1
2
Gain =
= 20log
1+
dB = 12dB with valuesshown
PO
RG
FIGURE 3. High Dynamic Range IF Amplifier.
The input signal and the gain resistor are AC-coupled through
the 0.01µF blocking capacitors. This holds the DC input and
output operating point at ground independent of source im-
pedance and gain setting. The RG value in Figure 3 (144Ω),
sets the gain to the matched load at 12dB. Using standard 1%
tolerance resistors for RF and RG will hold the gain to a ±0.2dB
tolerance. This example will give a –3dB bandwidth of ap-
proximately 100MHz while maintaining gain flatness within
This will set the –3dB bandwidth according to:
GBP
F−3dB
Hz
(2)
2πRFCS
The example of Figure 4 will give approximately 24MHz
–3dB bandwidth using the 0.75pF feedback compensation.
OPA843
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WIDEBAND INVERTING SUMMING AMPLIFIER
100pF
220pF
One common application for a wideband op amp like the
OPA843 is to sum a number of signal sources together.
Figure 5 shows the inverting summing configuration that is
most often used. This circuit offers the benefit that each input
sees an input impedance set only by its individual input
resistor, since the summing junction (inverting op amp node)
is a virtual ground. Each input is non-interactive with every
other. However, the bandwidth from any input to the summed
output is set by the op amp noise gain (NG), which is equal
to the noninverting voltage gain. Therefore, each inverting
channel may have a low gain to the output (like the –1 shown
in Figure 5); this noise gain will set the frequency response
and the loop stability. The noninverting gain for Figure 5 is
equal to +5, which will give a 260MHz bandwidth at a gain of
–1 for each of the input signals.
61Ω
150Ω
VI
0Ω
Source
VO
OPA843
402Ω
100Ω
FIGURE 6. 10MHz Butterworth Low-Pass Filter.
10MHz Low-Pass Filter
15
12
9
+5V
Power-supply decoupling not shown.
6
3
VO = –(V1 + V2 + V3 + V4)
81.8Ω
OPA843
0.1µF
0
–3
–6
–9
–12
–15
–5V
RF
402Ω
402Ω
V1
V2
V3
V4
100k
1M
10M
100M
402Ω
402Ω
402Ω
Frequency (MHz)
FIGURE 7. Frequency Response for Figure 6.
transition from a unity gain receiver at lower frequencies
(through the R5 path) to a gain of 20dB (10V/V) through the
R1 path at higher frequencies. The component values have
been selected to set the peak gain at approximately 30MHz.
A unique feature for this circuit is an independent tune on the
width of the peaking (Q of the response) by adjusting RG.
See Figure 9 for the effect of adjusting RG over the range of
20Ω to 100Ω.
FIGURE 5. Wideband Inverting Summing Amplifier.
2nd-Order Filter Topology
High-speed amplifiers like the OPA843 are good choices for
2nd-order filter building blocks as part of ADC driver chan-
nels. These can provide noise bandlimiting to improve the
SNR for the amplifier/converter combination. The circuit of
Figure 6 shows an example of a 10MHz Butterworth low-
pass filter where the amplifier provides a low frequency gain
of 5 and a 2nd-order cutoff at 10MHz. The resistor values
have been adjusted slightly to account for the amplifier
bandwidth. Figure 7 shows the small-signal frequency re-
sponse for this filter.
DESIGN-IN TOOLS
DEMONSTRATION FIXTURES
Two printed circuit boards (PCBs) are available to assist in
the initial evaluation of circuit performance using the OPA843
in its two package options. Both of these are offered free of
charge as unpopulated PCBs, delivered with a user's guide.
The summary information for these fixtures is shown in the
table below.
EQUALIZING FILTER APPLICATION
In sensor receiver applications, where the pickup is a sensor
or cable giving a bandlimited frequency response, an equal-
izing filter can sometimes be used to extend the useable
frequency range for the sensor. This is done mathematically
by taking the inverse of the rolloff transfer function and
implementing that as the amplifier frequency response. See
Figure 8 for one example of a wideband equalizer where two
stages of the OPA843 are used. This example is set to
ORDERING
NUMBER
LITERATURE
NUMBER
PRODUCT
PACKAGE
OPA843U
OPA843N
SO-8
SOT23-5
DEM-OPA-SO-1A
DEM-OPA-SOT-1A
SBOU009
SBOU010
The demonstration fixtures can be requested at the Texas
Instruments web site (www.ti.com) through the OPA843
product folder.
OPA843
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+5V
+5V
VCC
VCC
VOUT
OPA843
OPA843
Power-supply
decoupling not shown.
RLOAD
1kΩ
VEE
VEE
–5V
RF
1.2kΩ
–5V
C2
41.125pF
R4
R1
120Ω
R2
600Ω
1.2kΩ
VIN
C1
5.2pF
RG
R5
1.2kΩ
FIGURE 8. Adjustable Equalizer.
value should be between 200Ω and 1kΩ. Below 200Ω, the
feedback network will present additional output loading that
can degrade the harmonic distortion performance of the
OPA843. Above 1kΩ, the typical parasitic capacitance (ap-
proximately 0.2pF) across the feedback resistor may cause
unintentional band limiting in the amplifier response.
40
20
0
A good rule of thumb is to target the parallel combination of
RF and RG (see Figure 1) to be less than about 200Ω. The
combined impedance RF || RG interacts with the inverting
input capacitance, placing an additional pole in the feedback
network, and thus a zero in the forward response. Assuming
a 2pF total parasitic on the inverting node, holding RF || RG
< 200Ω will keep this pole above 400MHz. By itself, this
constraint implies that the feedback resistor RF can increase
to several kΩ at high gains. This is acceptable as long as the
pole formed by RF and any parasitic capacitance appearing
in parallel is kept out of the frequency range of interest.
–20
–40
100kHz
1MHz
10MHz
100MHz
1GHz
Frequency
FIGURE 9. Equalizer Plot, Multiple Settings.
MACROMODELS AND APPLICATIONS SUPPORT
Computer simulation of circuit performance using SPICE is
often a quick way to analyze the performance of the OPA843
and its circuit designs. This is particularly true for video and
RF amplifier circuits where parasitic capacitance and induc-
tance can play a major role on circuit performance. A SPICE
model for the OPA843 is available through the TI web page
(http://www.ti.com). The applications department is also avail-
able for design assistance. These models predict typical
small-signal AC, transient steps, DC performance, and noise
under a wide variety of operating conditions. The models
include the noise terms found in the electrical specifications
of this data sheet. These models do not attempt to distin-
guish between the package types in their small-signal AC
performance.
In the inverting configuration, an additional design consider-
ation must be noted. RG becomes the input resistor and,
therefore, the load impedance to the driving source. If imped-
ance matching is desired, RG may be set equal to the
required termination value. However, at low inverting gains
the resultant feedback resistor value can present a signifi-
cant load to the amplifier output. For example, an inverting
gain of –4 with a 50Ω input matching resistor (= RG) would
require a 200Ω feedback resistor, which would contribute to
output loading in parallel with the external load. In such a
case, it would be preferable to increase both the RF and RG
values, and then achieve the input matching impedance with
a third resistor to ground; see Figure 2. The total input
impedance becomes the parallel combination of RG and the
additional shunt resistor.
OPERATING SUGGESTIONS
OPTIMIZING RESISTOR VALUES
BANDWIDTH vs GAIN
Voltage-feedback op amps exhibit decreasing closed-loop
bandwidth as the signal gain is increased. In theory, this
relationship is described by the GBP shown in the Electrical
Characteristics. Ideally, dividing GBP by the noninverting
signal gain (also called the Noise Gain, or NG) will predict the
closed-loop bandwidth. In practice, this only holds true when
Since the OPA843 is a voltage-feedback op amp, a wide
range of resistor values may be used for the feedback and
gain setting resistors. The primary limits on these values are
set by dynamic range (noise and distortion) and parasitic
capacitance considerations. Usually, the feedback resistor
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the phase margin approaches 90°, as it does in high-gain
configurations. At low signal gains, most amplifiers will ex-
hibit a more complex response with lower phase margin. The
OPA843 is optimized to give a maximally flat 2nd-order
Butterworth response in a gain of 5. In this configuration, the
OPA843 has approximately 60° of phase margin and will
show a typical –3dB bandwidth of 260MHz. When the phase
margin is 60°, the closed-loop bandwidth is approximately √2
greater than the value predicted by dividing GBP by the noise
gain. Increasing the gain will cause the phase margin to
approach 90° and the bandwidth to more closely approach
the predicted value of (GBP/NG). At a gain of +20, the
40MHz bandwidth shown in the Electrical Characteristics
agrees with that predicted using the simple formula and the
typical GBP of 800MHz.
tune the flatness by adjusting RI. The Typical Characteristics
show a signal gain of +4 with the noise gain adjusted for
flatness using different values for R1.
Where low gain is desired, and inverting operation is accept-
able, a new external compensation technique may be used to
retain the full slew rate and noise benefits of the OPA843 while
maintaining the increased loop gain and the associated im-
provement in distortion offered by the decompensated archi-
tecture. This technique shapes the noise gain for good stability
while giving an easily controlled 2nd-order low-pass frequency
response. Figure 11 shows this circuit. Considering only the
noise gain for the circuit of Figure 11, the low-frequency noise
gain (NG1) will be set by the resistor ratios while the high-
frequency noise gain (NG2) will be set by the capacitor ratios.
The capacitor values set both the transition frequencies and
the high-frequency noise gain. If this noise gain, determined by
NG2 = 1 + CS/CF, is set to a value greater than the recom-
mended minimum stable gain for the op amp and the noise
gain pole (set by 1/RFCF) is placed correctly, a very well
controlled 2nd-order low-pass frequency response will result.
LOW GAIN OPERATION
Decreasing the operating gain for the OPA843 from the
nominal design point of +5 will decrease the phase margin.
This will increase the Q for the closed-loop poles, peak up
the frequency response, and extend the bandwidth. A peaked
frequency response will show overshoot and ringing in the
pulse response as well as a higher integrated output noise.
Operating at a noise gain less than +3 runs the risk of
sustained oscillation (loop instability). However, operation at
low gains would be desirable to take advantage of the much
higher slew rate and lower input noise voltage available in
the OPA843, as compared to the performance offered by
unity-gain stable op amps. Numerous external compensation
techniques have been suggested for operating a high-gain
op amp at low gains. Most of these give zero/pole pairs in the
closed-loop response that cause long term settling tails in the
pulse response and/or phase nonlinearity in the frequency
response. Figure 10 shows an external compensation method
for a noninverting configuration that does not suffer from
these drawbacks.
+5V
Power-supply
decoupling not shown.
VO
280Ω
OPA843
0.1µF
–5V
RF
806Ω
402Ω
V1
RS = 0Ω
CF
1.9pF
CS
12.6pF
FIGURE 10. Noninverting Low Gain Circuit.
+5V
To choose the values for both CS and CF, two parameters
and only three equations need to be solved. The first param-
eter is the target high-frequency noise gain, NG2, which
should be greater than the minimum stable gain for the
OPA843. Here, a target NG2 of 7.5 will be used. The second
parameter is the desired low-frequency signal gain, which
also sets the low-frequency noise gain, NG1. To simplify this
discussion, we will target a maximally flat 2nd-order low-pass
Butterworth frequency response (Q = 0.707). The signal gain
of –2 shown in Figure 11 will set the low-frequency noise gain
to NG1 = 1 + RF/RG (= 3 in this example). Then, using only
these two gains and the GBP for the OPA843 (800MHz), the
key frequency in the compensation is determined by:
50Ω Source
RS
50Ω
VI
VO
R1
133Ω
RT
50Ω
OPA843
50Ω Load
RF
402Ω
+5V
RG
402Ω
FIGURE 10. Noninverting Low Gain Circuit.
GBP
2
NG1
NG1
NG2
NG1
NG2
Z0 =
1−
− 1− 2
(11)
The R1 resistor across the two inputs will increase the noise
gain (i.e., decrease the loop gain) without changing the
signal gain. This approach will retain the full slew rate to the
output but will give up some of the low-noise benefit of the
OPA843. Assuming a low source impedance, set R1 so that
1 + RF/(RG || RI) is ≥ +3. This approach may also be used to
Physically, this Z0 (13.6MHz for the values shown in Figure 11)
is set by 1/(2π • RF (CF + CS)) and is the frequency at which
the rising portion of the noise gain would intersect unity gain
if projected back to 0dB gain. The actual zero in the noise gain
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occurs at NG1 • Z0 and the pole in the noise gain occurs at
NG2 • Z0. Since GBP is expressed in Hz, multiply Z0 by 2π and
use this to get CF by solving:
susceptible to decreased stability and closed-loop response
peaking when a capacitive load is placed directly on the
output pin. In simple terms, the capacitive load reacts with
the open-loop output resistance of the amplifier to introduce
an additional pole into the loop and thereby decrease the
phase margin. This issue has become a popular topic of
application notes and articles, and several external solutions
to this problem have been suggested. When the primary
considerations are frequency-response flatness, pulse re-
sponse fidelity, and/or distortion, the simplest and most
effective solution is to isolate the capacitive load from the
feedback loop by inserting a series isolation resistor between
the amplifier output and the capacitive load. This does not
eliminate the pole from the loop response, but rather shifts it
and adds a zero at a higher frequency. The additional zero
acts to cancel the phase lag from the capacitive load pole,
thus increasing the phase margin and improving stability.
1
CF =
(12)
2πRFZ0NG2
Finally, since CS and CF set the high-frequency noise gain,
determine CS by:
CS = (NG2 – 1)CF
(13)
The resulting closed-loop bandwidth will be approximately
equal to:
(14)
f−3dB
Z0 GBP
For the values shown in Figure 10, the f–3dB will be approxi-
mately 105MHz. This is less than that predicted by simply
dividing the GBP product by NG1. The compensation network
controls the bandwidth to a lower value while providing full
slew rate and exceptional distortion performance due to in-
creased loop gain at frequencies below NG1 • Z0. The capaci-
tor values shown in Figure 10 are calculated for NG1 = 3 and
NG2 = 7.5 with no adjustment for parasitics.
The Typical Characteristics show the recommended RS vs
Capacitive Load and the resulting frequency response at the
load. The criterion for setting the recommended resistor is
maximum bandwidth and flat frequency response at the load.
Since there is now a passive low-pass filter between the
output pin and the load capacitance, the response at the
output pin itself is typically somewhat peaked, and becomes
flat after the roll off action of the RC network. This is not a
concern in most applications, but can cause clipping if the
desired signal swing at the load is very close to the amplifier’s
swing limit.
OUTPUT DRIVE CAPABILITY
The OPA843 has been optimized to drive the demanding load
of a doubly-terminated transmission line. When a 50Ω line is
driven, a series 50Ω into the cable and a terminating 50Ω load
at the end of the cable are used. Under these conditions, the
impedance of the cable appears resistive over a wide fre-
quency range and the total effective load on the OPA843 is
100Ω in parallel with the resistance of the feedback network.
The Electrical Characteristics show a 6.1VPP swing into a
100Ω load—which is then reduced to a 3VPP swing at the
termination resistor. The ±85mA output drive over tempera-
ture provides adequate current drive margin for this load.
Parasitic capacitive loads greater than 2pF can begin to
degrade the performance of the OPA843. Long PC board
traces, unmatched cables, and connections to multiple de-
vices can easily cause this value to be exceeded. Always
consider this effect carefully and add the recommended
series resistor as close as possible to the OPA843 output pin
(see Board Layout section).
A common IF amplifier specification, which describes avail-
able output power is the –1dB compression point. This is
usually defined at a matched 50Ω load to be the sinusoidal
power where the gain has compressed by –1dB vs the gain
seen at very low power levels. This compression level is
frequency dependent for an op amp, due to both bandwidth
and slew rate limitations. For frequencies well within the
bandwidth and slew rate limit of the OPA843, the –1dB
compression at a matched 50Ω load will be > 13dBm based
on the minimum available 3Vp-p swing at the load. One
common use for the –1dB compression is to predict
intermodulation intercept. This is normally 10dB greater than
the –1dB compression power for a standard RF amplifier. This
simple rule of thumb does NOT apply to the OPA843. The high
open-loop gain and Class AB output stage of the OPA843
produce a much higher intercept than the –1dB compression
would predict, as shown in the Typical Characteristics.
DISTORTION PERFORMANCE
The OPA843 is capable of delivering an exceptionally low
distortion signal at high frequencies and medium gains. The
distortion plots in the Typical Characteristics show the typical
distortion under a wide variety of conditions. Most of these
plots are limited to 100dB dynamic range. The OPA843’s
distortion does not rise above –100dBc until either the signal
level exceeds 0.5Vp-p and/or the fundamental frequency
exceeds 500kHz.
Distortion in the audio band is < –120dBc.
Generally, until the fundamental signal reaches very high
frequencies or powers, the 2nd-harmonic will dominate the
distortion with a negligible 3rd-harmonic component. Focus-
ing then on the 2nd-harmonic, increasing the load imped-
ance improves distortion directly. Remember that the total
load includes the feedback network—in the noninverting
configuration this is the sum of RF + RG, whereas in the
inverting configuration this is just RF (see Figure 1). Increas-
ing output voltage swing increases harmonic distortion di-
rectly. A 6dB increase in output swing will generally increase
DRIVING CAPACITIVE LOADS
One of the most demanding, and yet very common, load
conditions for an op amp is capacitive loading. A high-speed,
high open-loop gain amplifier like the OPA843 can be very
OPA843
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the 2nd-harmonic 12dB and the 3rd-harmonic 18dB. Increas-
ing the signal gain will also increase the 2nd-harmonic
distortion. Again, a 6dB increase in gain will increase the
2nd- and 3rd-harmonic by 6dB even with a constant output
power and frequency. Finally, the distortion increases as the
fundamental frequency increases due to the roll off in the
loop gain with frequency. Conversely, the distortion will
improve going to lower frequencies down to the dominant
open-loop pole at approximately 3kHz. Starting from the
–100dBc 2nd-harmonic for 2VPP into 200Ω, G = +5 distortion
at 500kHz (from the Typical Characteristics), the 2nd-har-
monic distortion at 20kHz should be approximately:
shows the general form for this output noise voltage using the
terms presented in Figure 12.
2
EO
=
E2 + IBNRS + 4kTRS NG2 + IBIRF 2 + 4kTRFNG
(
)
(15)
(
)
(
)
NI
ENI
EO
OPA843
RS
IBN
ERS
RF
√4kTRS
√4kTRF
IBI
–100dB – 20log (500kHz/20kHz) = –128dBc.
RG
4kT
RG
4kT = 1.6E – 20J
at 290°K
The OPA843 has an extremely low 3rd-order harmonic distortion.
This also gives an exceptionally good 2-tone, 3rd-order
intermodulation intercept, as shown in the Typical Characteristics.
This intercept curve is defined at the 50Ω load when driven through
a 50Ω-matching resistor to allow direct comparisons to RF MMIC
devices. This network attenuates the voltage swing from the output
pin to the load by 6dB. If the OPA843 drives directly into the input
of a high-impedance device, such as an ADC, this 6dB attenuation
is not taken. Under these conditions, the intercept will increase by
a minimum of 6dBm. The intercept is used to predict the
intermodulation spurious for two closely spaced frequencies. If the
two test frequencies, f1 and f2, are specified in terms of average and
delta frequency, fO = (f1 + f2)/2 and µf = |f2 – f1|/2, the two, 3rd-order,
close-in spurious tones will appear at fO ± (3 • ∆f). The difference
between two equal test-tone power levels and these
intermodulation spurious power levels is given by 2 • (IM3 – PO)
where IM3 is the intercept taken from the typical characteristic
curve and PO is the power level in dBm at the 50Ω load for one of
the two closely spaced test frequencies. For instance, at 10MHz the
OPA843 at a gain of +5 has an intercept of 49dBm at a matched
50Ω load. If the full envelope of the two frequencies needs to be
2Vp-p, this requires each tone to be 4dBm. The 3rd-order
intermodulation spurious tones will then be 2 • (49 – 4) = 90dBc
below the test-tone power level (–86dBm). If this same 2Vp-p 2-
tone envelope were delivered directly into the input of an ADC
without the matching loss or loading of the 50Ω network, the
intercept would increase to at least 55dBm. With the same signal
and gain conditions now driving directly into a light load, the
spurious tones will then be at least 2 • (55 – 4) = 102dBc below the
1VPP test-tone signal levels.
FIGURE 12. Op Amp Noise Analysis Model.
Dividing this expression by the noise gain (NG = 1 + RF/RG)
will give the equivalent input referred spot noise voltage at
the noninverting input, as shown in Equation 16.
2
IBIRF
NG
4kTRF
NG
2
EN = EN2I + IBNRS + 4kTRS
+
+
(16)
(
)
Evaluating these two equations for the OPA843 circuit pre-
sented in Figure 1 will give a total output spot noise voltage
of 12.4nV/√Hz and an equivalent input spot noise voltage of
2.48nV/√Hz
.
DC OFFSET CONTROL
The OPA843 can provide excellent DC signal accuracy due to
its high open-loop gain, high common-mode rejection, high
power supply rejection, and low input offset voltage and bias
current offset errors. To take full advantage of this low input
offset voltage, careful attention to input bias current cancella-
tion is also required. The high-speed input stage for the
OPA843 has a relatively high input bias current (20µA typical
into the pins) but with a very close match between the two
input currents—typically 0.17µA input offset current. Figures
13 and 14 show typical distribution of input offset voltage and
current for the OPA843.
1000
Mean = 0.38mV
Standard Deviation = 0.31mV
900
NOISE PERFORMANCE
Total Count = 5572
800
700
600
500
400
300
200
100
0
The OPA843 complements its ultra low harmonic distortion
with low input noise terms. Both the input-referred voltage
noise, and the two input-referred current noise terms com-
bine to give a low output noise under a wide variety of
operating conditions. Figure 12 shows the op amp noise
analysis model with all the noise terms included. In this
model, all the noise terms are taken to be noise voltage or
current density terms in either nV/√Hz or pA/√Hz
.
The total output spot noise voltage is computed as the square
root of the squared contributing terms to the output noise
voltage. This computation is adding all the contributing noise
powers at the output by superposition, and then taking the
square root to get back to a spot noise voltage. Equation 15
mV
FIGURE 13. Input Offset Voltage Distributing in mV.
OPA843
16
SBOS268C
www.ti.com
+5V
1600
1400
1200
1000
800
600
400
200
0
VCC
Mean = 0.04µA
Standard Deviation = 0.17µA
Total Count = 5572
Power-supply decoupling
not shown.
VO
OPA843
0.1µF
200Ω
VEE
–5V
+5V
RG
250Ω
RF
1kΩ
VIN
5kΩ
5kΩ
±125mV Output Adjustment
20kΩ
10kΩ
0.1µF
VO
RF
mV
= –
= –4
VIN
RG
FIGURE 14.
–5V
The total output offset voltage may be considerably reduced
by matching the source impedances looking out of the two
inputs. For example, one way to add bias current cancellation
to the circuit of Figure 1 would be to insert a 55Ω series resistor
into the noninverting input from the 50Ω terminating resistor.
When the 50Ω source resistor is DC coupled, this will increase
the source impedance for the noninverting input bias current
to 80Ω. Since this is now equal to the impedance looking out
of the inverting input (RF || RG), the circuit will cancel the gains
for the bias currents to the output leaving only the offset
current times the feedback resistor as a residual DC error term
at the output. Using a 402Ω feedback resistor, this output error
will now be less than 1µA • 402Ω = 0.4mV at 25°C.
FIGURE 15. DC-Coupled, Inverting Gain of –4 with Output
Offset Adjustment.
resistor values for setting this offset adjustment are chosen
to be much larger than the signal path resistors. This will
insure that this adjustment has minimal impact on the loop
gain and hence, the frequency response.
THERMAL ANALYSIS
The OPA843 will not require heat sinking or airflow in most
applications. Maximum desired junction temperature would
set the maximum allowed internal power dissipation as
described below. In no case should the maximum junction
temperature be allowed to exceed +150°C.
A fine-scale output offset null, or DC operating point adjust-
ment, is sometimes required. Numerous techniques are
available for introducing a DC offset control into an op amp
circuit. Most of these techniques eventually reduce to setting
up a DC current through the feedback resistor. One key
consideration to selecting a technique is to insure that it has
a minimal impact on the desired signal path frequency
response. If the signal path is intended to be noninverting,
the offset control is best applied as an inverting summing
signal to avoid interaction with the signal source. If the signal
path uses the inverting mode, applying an offset control to
the noninverting input can be considered. For a DC-coupled
inverting input signal, this DC offset signal will set up a DC
current back into the source that must be considered. An
offset adjustment placed on the inverting op amp input can
also change the noise gain and frequency response flatness.
Figure 15 shows one example of an offset adjustment for a
DC-coupled signal path that will have minimum impact on the
signal frequency response. In this case, the input is brought
into an inverting gain resistor with the DC adjustment an
additional current summed into the inverting node. The
Operating junction temperature (TJ ) is given by TA + PD • θJA
.
The total internal power dissipation (PD) is the sum of quiescent
power (PDQ) and additional power dissipated in the output
stage (PDL) to deliver load power. Quiescent power is simply
the specified no-load supply current times the total supply
voltage across the part. PDL will depend on the required output
signal and load but would, for a grounded resistive load, be at
a maximum when the output is fixed at a voltage equal to 1/2
of either supply voltage (for equal bipolar supplies). Under this
worst-case condition, PDL = VS2/(4 • RL), where RL includes
feedback network loading.
Note that it is the power in the output stage and not in the
load that determines internal power dissipation.
As a worst-case example, compute the maximum TJ using an
OPA843IDBV (SOT23-5 package) in the circuit of Figure 1
operating at the maximum specified ambient temperature of
+85°C. PD = 10V(22.5mA) + 52/(4 • (100Ω || 500Ω)) = 300mW.
Maximum TJ = +85°C + (0.30W • 150°C/W) = 130°C.
OPA843
SBOS268C
17
www.ti.com
BOARD LAYOUT
> 1.5kΩ, this parasitic capacitance can add a pole and/or a
zero below 500MHz that can effect circuit operation. Keep
resistor values as low as possible consistent with load driving
considerations.
Achieving optimum performance with a high-frequency am-
plifier such as the OPA843 requires careful attention to board
layout parasitics and external component types. Recommen-
dations that will optimize performance include:
d) Connections to other wideband devices on the board
may be made with short, direct traces or through onboard
transmission lines. For short connections, consider the
trace and the input to the next device as a lumped capacitive
load. Relatively wide traces (50mils to 100mils) should be
used, preferably with ground and power planes opened up
around them. Estimate the total capacitive load and set RS
from the plot of recommended RS vs Capacitive Load. Low
parasitic capacitive loads (< 5pF) may not need an RS since
the OPA843 is nominally compensated to operate with a 2pF
parasitic load. Higher parasitic capacitive loads without an RS
are allowed as the signal gain increases (increasing the
unloaded phase margin). If a long trace is required, and the
6dB signal loss intrinsic to a doubly-terminated transmission
line is acceptable, implement a matched-impedance trans-
mission line using microstrip or stripline techniques (consult
an ECL design handbook for microstrip and stripline layout
techniques). A 50Ω environment is normally not necessary
on board, and in fact a higher impedance environment will
improve distortion as shown in the distortion versus load
plots. With a characteristic board trace impedance defined
based on board material and trace dimensions, a matching
series resistor into the trace from the output of the OPA843
is used as well as a terminating shunt resistor at the input of
the destination device. Remember also that the terminating
impedance will be the parallel combination of the shunt
resistor and input impedance of the destination device; this
total effective impedance should be set to match the trace
impedance. If the 6dB attenuation of a doubly-terminated
transmission line is unacceptable, a long trace can be series-
terminated at the source end only. Treat the trace as a
capacitive load in this case and set the series resistor value
as shown in the plot of RS vs Capacitive Load. This will not
preserve signal integrity as well as a doubly-terminated line.
If the input impedance of the destination device is low, there
will be some signal attenuation due to the voltage divider
formed by the series output into the terminating impedance.
a) Minimize parasitic capacitance to any AC ground for
all of the signal I/O pins. Parasitic capacitance on the
output and inverting input pins can cause instability: on the
noninverting input, it can react with the source impedance to
cause unintentional bandlimiting. To reduce unwanted ca-
pacitance, a window around the signal I/O pins should be
opened in all of the ground and power planes around those
pins. Otherwise, ground and power planes should be unbro-
ken elsewhere on the board.
b) Minimize the distance (< 0.25") from the power-supply
pins to high-frequency 0.1µF decoupling capacitors. At
the device pins, the ground and power-plane layout should
not be in close proximity to the signal I/O pins. Avoid narrow
power and ground traces to minimize inductance between
the pins and the decoupling capacitors. The power-supply
connections should always be decoupled with these capaci-
tors. Larger (2.2µF to 6.8µF) decoupling capacitors, effective
at lower frequency, should also be used on the main supply
pins. These may be placed somewhat farther from the device
and may be shared among several devices in the same area
of the PC board.
c) Careful selection and placement of external compo-
nents will preserve the high-frequency performance of
the OPA843. Resistors should be a very low reactance type.
Surface-mount resistors work best and allow a tighter overall
layout. Metal-film and carbon composition, axially-leaded
resistors can also provide good high-frequency performance.
Again, keep their leads and PC board trace length as short
as possible. Never use wire-wound type resistors in a high-
frequency application. Since the output pin and inverting
input pin are the most sensitive to parasitic capacitance,
always position the feedback and series output resistor, if
any, as close as possible to the output pin. Other network
components, such as noninverting input termination resis-
tors, should also be placed close to the package. Where
double-feedback side component mounting is allowed, place
the feedback resistor directly under the package on the other
side of the board between the output and inverting input pins.
Even with a low parasitic capacitance shunting the external
resistors, excessively high resistor values can create signifi-
cant time constants that can degrade performance. Good
axial metal-film or surface-mount resistors have approxi-
mately 0.2pF in shunt with the resistor. For resistor values
e) Socketing a high-speed part like the OPA843 is not
recommended. The additional lead length and pin-to-pin
capacitance introduced by the socket can create an ex-
tremely troublesome parasitic network, which can make it
almost impossible to achieve a smooth, stable frequency
response. Best results are obtained by soldering the OPA843
onto the board.
OPA843
18
SBOS268C
www.ti.com
INPUT AND ESD PROTECTION
These diodes provide moderate protection to input overdrive
voltages above the supplies as well. The protection diodes
can typically support 30mA continuous current. Where higher
currents are possible (e.g., in systems with ±15V supply parts
driving into the OPA843), current-limiting series resistors
should be added into the two inputs. Keep these resistor
values as low as possible since high values degrade both
noise performance and frequency response. Figure 17 shows
one example of an overdrive protection circuit added to a
G = +5V/V design.
The OPA843 is built using a very high-speed complementary
bipolar process. The internal junction breakdown voltages are
relatively low for these very small geometry devices. These
breakdowns are reflected in the Absolute Maximum Ratings
table. All device pins are protected with internal ESD protec-
tion diodes to the power supplies, as shown in Figure 16.
50Ω Source
125Ω
Power-supply
decoupling not shown.
+5V
+VCC
50Ω
External
Pin
Internal
Cicuitry
D1
D2
OPA843
VO
50Ω
RF
505Ω
50Ω
–VCC
–5V
RG
126Ω
D1 = D2 IN5911 (or equivalent)
FIGURE 16. Internal ESD Protection.
FIGURE 17. Gain of +5 with Input Protection.
OPA843
SBOS268C
19
www.ti.com
Revision History
DATE
REVISION PAGE
SECTION
Absolute Maximum Ratings Changed minimum Storage Temperature Range from −40°C to −65°C.
Design-In Tools Board part number changed.
DESCRIPTION
12/08
C
B
2
3/06
13
NOTE: Page numbers for previous revisions may differ from page numbers in the current version.
OPA843
20
SBOS268C
www.ti.com
PACKAGE OPTION ADDENDUM
www.ti.com
10-Jun-2014
PACKAGING INFORMATION
Orderable Device
OPA843ID
Status Package Type Package Pins Package
Eco Plan
Lead/Ball Finish
MSL Peak Temp
Op Temp (°C)
-40 to 85
-40 to 85
-40 to 85
-40 to 85
-40 to 85
-40 to 85
-40 to 85
Device Marking
Samples
Drawing
Qty
(1)
(2)
(6)
(3)
(4/5)
ACTIVE
SOIC
SOT-23
SOT-23
SOT-23
SOIC
D
8
5
5
5
8
8
8
75
Green (RoHS
& no Sb/Br)
CU NIPDAU
CU NIPDAU
CU NIPDAU
CU NIPDAU
CU NIPDAU
CU NIPDAU
CU NIPDAU
Level-2-260C-1 YEAR
Level-2-260C-1 YEAR
Level-2-260C-1 YEAR
Level-2-260C-1 YEAR
Level-2-260C-1 YEAR
Level-2-260C-1 YEAR
Level-2-260C-1 YEAR
OPA
843
OPA843IDBVR
OPA843IDBVT
OPA843IDBVTG4
OPA843IDG4
OPA843IDR
ACTIVE
ACTIVE
ACTIVE
ACTIVE
ACTIVE
ACTIVE
DBV
DBV
DBV
D
3000
250
Green (RoHS
& no Sb/Br)
OARI
OARI
OARI
Green (RoHS
& no Sb/Br)
250
Green (RoHS
& no Sb/Br)
75
Green (RoHS
& no Sb/Br)
OPA
843
SOIC
D
2500
2500
Green (RoHS
& no Sb/Br)
OPA
843
OPA843IDRG4
SOIC
D
Green (RoHS
& no Sb/Br)
OPA
843
(1) The marketing status values are defined as follows:
ACTIVE: Product device recommended for new designs.
LIFEBUY: TI has announced that the device will be discontinued, and a lifetime-buy period is in effect.
NRND: Not recommended for new designs. Device is in production to support existing customers, but TI does not recommend using this part in a new design.
PREVIEW: Device has been announced but is not in production. Samples may or may not be available.
OBSOLETE: TI has discontinued the production of the device.
(2) Eco Plan - The planned eco-friendly classification: Pb-Free (RoHS), Pb-Free (RoHS Exempt), or Green (RoHS & no Sb/Br) - please check http://www.ti.com/productcontent for the latest availability
information and additional product content details.
TBD: The Pb-Free/Green conversion plan has not been defined.
Pb-Free (RoHS): TI's terms "Lead-Free" or "Pb-Free" mean semiconductor products that are compatible with the current RoHS requirements for all 6 substances, including the requirement that
lead not exceed 0.1% by weight in homogeneous materials. Where designed to be soldered at high temperatures, TI Pb-Free products are suitable for use in specified lead-free processes.
Pb-Free (RoHS Exempt): This component has a RoHS exemption for either 1) lead-based flip-chip solder bumps used between the die and package, or 2) lead-based die adhesive used between
the die and leadframe. The component is otherwise considered Pb-Free (RoHS compatible) as defined above.
Green (RoHS & no Sb/Br): TI defines "Green" to mean Pb-Free (RoHS compatible), and free of Bromine (Br) and Antimony (Sb) based flame retardants (Br or Sb do not exceed 0.1% by weight
in homogeneous material)
(3) MSL, Peak Temp. - The Moisture Sensitivity Level rating according to the JEDEC industry standard classifications, and peak solder temperature.
(4) There may be additional marking, which relates to the logo, the lot trace code information, or the environmental category on the device.
Addendum-Page 1
PACKAGE OPTION ADDENDUM
www.ti.com
10-Jun-2014
(5) Multiple Device Markings will be inside parentheses. Only one Device Marking contained in parentheses and separated by a "~" will appear on a device. If a line is indented then it is a continuation
of the previous line and the two combined represent the entire Device Marking for that device.
(6) Lead/Ball Finish - Orderable Devices may have multiple material finish options. Finish options are separated by a vertical ruled line. Lead/Ball Finish values may wrap to two lines if the finish
value exceeds the maximum column width.
Important Information and Disclaimer:The information provided on this page represents TI's knowledge and belief as of the date that it is provided. TI bases its knowledge and belief on information
provided by third parties, and makes no representation or warranty as to the accuracy of such information. Efforts are underway to better integrate information from third parties. TI has taken and
continues to take reasonable steps to provide representative and accurate information but may not have conducted destructive testing or chemical analysis on incoming materials and chemicals.
TI and TI suppliers consider certain information to be proprietary, and thus CAS numbers and other limited information may not be available for release.
In no event shall TI's liability arising out of such information exceed the total purchase price of the TI part(s) at issue in this document sold by TI to Customer on an annual basis.
Addendum-Page 2
PACKAGE MATERIALS INFORMATION
www.ti.com
14-Jul-2012
TAPE AND REEL INFORMATION
*All dimensions are nominal
Device
Package Package Pins
Type Drawing
SPQ
Reel
Reel
A0
B0
K0
P1
W
Pin1
Diameter Width (mm) (mm) (mm) (mm) (mm) Quadrant
(mm) W1 (mm)
OPA843IDBVR
OPA843IDBVT
OPA843IDR
SOT-23
SOT-23
SOIC
DBV
DBV
D
5
5
8
3000
250
180.0
180.0
330.0
8.4
8.4
3.2
3.2
6.4
3.1
3.1
5.2
1.39
1.39
2.1
4.0
4.0
8.0
8.0
8.0
Q3
Q3
Q1
2500
12.4
12.0
Pack Materials-Page 1
PACKAGE MATERIALS INFORMATION
www.ti.com
14-Jul-2012
*All dimensions are nominal
Device
Package Type Package Drawing Pins
SPQ
Length (mm) Width (mm) Height (mm)
OPA843IDBVR
OPA843IDBVT
OPA843IDR
SOT-23
SOT-23
SOIC
DBV
DBV
D
5
5
8
3000
250
210.0
210.0
367.0
185.0
185.0
367.0
35.0
35.0
35.0
2500
Pack Materials-Page 2
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相关型号：
OPA843IDBVTG4
Wideband, Low Distortion, Medium Gain, Voltage Feedback Operational Amplifier 5-SOT-23 -40 to 85
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