NSC LMV793MFX 88 mhz, low noise, 1.8v cmos input, decompensated operational amplifier Datasheet

LMV793/LMV794
88 MHz, Low Noise, 1.8V CMOS Input, Decompensated
Operational Amplifiers
General Description
Features
The LMV793 (single) and the LMV794 (dual) CMOS input
operational amplifiers offer a low input voltage noise density
while consuming only 1.15 mA (LMV793) of
of 5.8 nV/
quiescent current. The LMV793/LMV794 are stable at a gain
of 10 and have a gain bandwidth product (GBW) of 88 MHz.
The LMV793/LMV794 have a supply voltage range of 1.8V to
5.5V and can operate from a single supply. The LMV793/
LMV794 each feature a rail-to-rail output stage capable of
driving a 600Ω load and sourcing as much as 60 mA of current.
The LMV793/LMV794 provide optimal performance in low
voltage and low noise systems. A CMOS input stage, with
typical input bias currents in the range of a few femto-Amperes, and an input common mode voltage range, which
includes ground, make the LMV793/LMV794 ideal for low
power sensor applications where high speeds are needed.
The LMV793/LMV794 are manufactured using National’s advanced VIP50 process. The LMV793 is offered in either a 5Pin SOT23 or an 8-Pin SOIC package. The LMV794 is offered
in either the 8-Pin SOIC or the 8-Pin MSOP.
(Typical 5V supply, unless otherwise noted)
5.8 nV/√Hz
■ Input referred voltage noise
100 fA
■ Input bias current
88 MHz
■ Gain bandwidth product
■ Supply current per channel
1.15 mA
— LMV793
1.30 mA
— LMV794
Rail-to-rail
output
swing
■
25 mV from rail
— @ 10 kΩ load
45 mV from rail
— @ 2 kΩ load
■ Guaranteed 2.5V and 5.0V performance
0.04% @1 kHz, 600Ω
■ Total harmonic distortion
−40°C to 125°C
■ Temperature range
Applications
■
■
■
■
■
■
ADC interface
Photodiode amplifiers
Active filters and buffers
Low noise signal processing
Medical instrumentation
Sensor interface applications
Typical Application
20216369
Photodiode Transimpedance Amplifier
© 2007 National Semiconductor Corporation
202163
20216339
Input Referred Voltage Noise vs. Frequency
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LMV793/LMV794 88 MHz, Low Noise, 1.8V CMOS Input, Decompensated Operational Amplifiers
August 2007
LMV793/LMV794
Soldering Information
Absolute Maximum Ratings (Note 1)
If Military/Aerospace specified devices are required,
please contact the National Semiconductor Sales Office/
Distributors for availability and specifications.
235°C
Wave Soldering Lead Temp (10 sec)
260°C
Operating Ratings
ESD Tolerance (Note 2)
Human Body Model
Machine Model
VIN Differential
Supply Voltage (V+ – V−)
Input/Output Pin Voltage
Storage Temperature Range
Junction Temperature (Note 3)
Infrared or Convection (20 sec)
200V
±0.3V
6.0V
V+ +0.3V, V− −0.3V
−65°C to 150°C
+150°C
2.5V Electrical Characteristics
(Note 1)
Temperature Range (Note 3)
Supply Voltage (V+ – V−)
−40°C ≤ TA ≤ 125°C
2000V
−40°C to 125°C
2.0V to 5.5V
0°C ≤ TA ≤ 125°C
1.8V to 5.5V
Package Thermal Resistance (θJA (Note 3))
5-Pin SOT23
8-Pin SOIC
8-Pin MSOP
180°C/W
190°C/W
236°C/W
(Note 4)
Unless otherwise specified, all limits are guaranteed for TA = 25°C, V+ = 2.5V, V− = 0V, VCM = V+/2 = VO. Boldface limits apply at
the temperature extremes.
Symbol
Parameter
Conditions
Min
(Note 6)
Typ
(Note 5)
Max
(Note 6)
0.1
±1.35
±1.65
VOS
Input Offset Voltage
TC VOS
Input Offset Average Drift
(Note 7)
LMV793
−1.0
LMV794
−1.8
Input Bias Current
VCM = 1.0V
(Notes 8, 9)
IB
IOS
Input Offset Current
CMRR
Common Mode Rejection Ratio 0V ≤ VCM ≤ 1.4V
PSRR
Power Supply Rejection Ratio
CMVR
AVOL
100
1.8V ≤ V+ ≤ 5.5V, VCM = 0V
80
98
Open Loop Gain
VOUT = 0.15V to 2.2V,
CMRR ≥ 55 dB
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fA
dB
1.5
1.5
LMV793
85
80
98
LMV794
82
78
92
88
84
110
V+/2
25
75
82
RL = 10 kΩ to V+/2
20
65
71
RL = 2 kΩ to V+/2
30
75
78
RL = 10 kΩ to V+/2
15
65
67
Sourcing to V−
VIN = 200 mV (Note 10)
35
28
47
Sinking to V+
VIN = –200 mV (Note 10)
7
5
15
V
dB
RL = 2 kΩ to V+/2
2
pA
dB
−0.3
-0.3
RL = 10 kΩ to V+/2
Output Short Circuit Current
1
100
80
75
VOUT = 0.15V to 2.2V,
IOUT
0.05
2.0V ≤ V+ ≤ 5.5V, VCM = 0V
CMRR ≥ 60 dB
Output Swing Low
−40°C ≤ TA ≤ 125°C
10
Input Common-Mode Voltage
Range
Output Swing High
1
25
94
RL = 2 kΩ to
VOUT
0.05
80
75
mV
μV/°C
−40°C ≤ TA ≤ 85°C
(Note 9)
Units
mV from
rail
mA
Supply Current Per Amplifier
SR
Slew Rate
LMV793
0.95
1.30
1.65
LMV794
1.1
1.50
1.85
AV = +10, Rising (10% to 90%)
32
AV = +10, Falling (90% to 10%)
24
mA
V/μs
GBWP
Gain Bandwidth Product
AV = +10, RL = 10 kΩ
88
en
Input-Referred Voltage Noise
f = 1 kHz
6.2
nV/
in
Input-Referred Current Noise
f = 1 kHz
0.01
pA/
THD+N
Total Harmonic Distortion +
Noise
f = 1 kHz, AV = 1, RL = 600Ω
0.01
5V Electrical Characteristics
MHz
%
(Note 4)
Unless otherwise specified, all limits are guaranteed for TA = 25°C, V+ = 5V, V− = 0V, VCM = V+/2 = VO. Boldface limits apply at
the temperature extremes.
Symbol
Parameter
Conditions
Min
(Note 6)
Typ
(Note 5)
Max
(Note 6)
0.1
±1.35
±1.65
VOS
Input Offset Voltage
TC VOS
Input Offset Average Drift
(Note 7)
LMV793
−1.0
LMV794
−1.8
Input Bias Current
VCM = 2.0V
(Notes 8, 9)
IB
IOS
Input Offset Current
CMRR
Common Mode Rejection Ratio 0V ≤ VCM ≤ 3.7V
PSRR
Power Supply Rejection Ratio
CMVR
AVOL
0.1
1
25
−40°C ≤ TA ≤ 125°C
0.1
1
100
10
80
75
100
2.0V ≤ V+ ≤ 5.5V, VCM = 0V
80
75
100
1.8V ≤
80
98
V+
≤ 5.5V, VCM = 0V
Input Common-Mode Voltage
Range
CMRR ≥ 60 dB
Open Loop Gain
VOUT = 0.3V to 4.7V,
85
80
97
LMV794
82
78
89
88
84
110
VOUT = 0.3V to 4.7V,
RL = 10 kΩ to V+/2
VOUT
Output Swing High
RL = 2 kΩ to V+/2
RL = 2 kΩ to V+/2
RL = 10 kΩ to V+/2
3
dB
V
dB
LMV793
35
75
82
LMV794
35
75
82
25
65
71
LMV793
42
75
78
LMV794
45
80
83
20
65
67
RL = 10 kΩ to V+/2
Output Swing Low
fA
4
4
LMV793
RL = 2 kΩ to V+/2
pA
dB
−0.3
-0.3
CMRR ≥ 55 dB
mV
μV/°C
−40°C ≤ TA ≤ 85°C
(Note 9)
Units
mV from
rail
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LMV793/LMV794
IS
LMV793/LMV794
IOUT
IS
Output Short Circuit Current
Supply Current per Amplifier
SR
Slew Rate
Sourcing to V−
VIN = 200 mV (Note 10)
45
37
60
Sinking to V+
VIN = –200 mV (Note 10)
10
6
21
mA
LMV793
1.15
1.40
1.75
LMV794 per Channel
1.30
1.70
2.05
AV = +10, Rising (10% to 90%)
35
AV = +10, Falling (90% to 10%)
28
88
mA
V/μs
GBWP
Gain Bandwidth Product
AV = +10, RL = 10 kΩ
MHz
en
Input-Referred Voltage Noise
f = 1 kHz
5.8
nV/
in
Input-Referred Current Noise
f = 1 kHz
0.01
pA/
THD+N
Total Harmonic Distortion +
Noise
f = 1 kHz, AV = 1, RL = 600Ω
0.01
%
Note 1: Absolute Maximum Ratings indicate limits beyond which damage to the device may occur. Operating Ratings indicate conditions for which the device is
intended to be functional, but specific performance is not guaranteed. For guaranteed specifications and the test conditions, see the Electrical Characteristics
Tables.
Note 2: Human Body Model, applicable std. MIL-STD-883, Method 3015.7. Machine Model, applicable std. JESD22-A115-A (ESD MM std. of JEDEC)
Field-Induced Charge-Device Model, applicable std. JESD22-C101-C (ESD FICDM std. of JEDEC).
Note 3: The maximum power dissipation is a function of TJ(MAX), θJA. The maximum allowable power dissipation at any ambient temperature is
PD = (TJ(MAX) - TA)/θJA. All numbers apply for packages soldered directly onto a PC Board.
Note 4: Electrical Table values apply only for factory testing conditions at the temperature indicated. Factory testing conditions result in very limited self-heating
of the device such that TJ = TA. No guarantee of parametric performance is indicated in the electrical tables under conditions of internal self-heating where TJ >
TA.
Note 5: Typical values represent the most likely parametric norm as determined at the time of characterization. Actual typical values may vary over time and will
also depend on the application and configuration. The typical values are not tested and are not guaranteed on shipped production material.
Note 6: Limits are 100% production tested at 25°C. Limits over the operating temperature range are guaranteed through correlations using the statistical quality
control (SQC) method.
Note 7: Offset voltage average drift is determined by dividing the change in VOS by temperature change.
Note 8: Positive current corresponds to current flowing into the device.
Note 9: Input bias current and input offset current are guaranteed by design
Note 10: The short circuit test is a momentary test, the short circuit duration is 1.5 ms.
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4
LMV793/LMV794
Connection Diagrams
5-Pin SOT23 (LMV793)
8-Pin SOIC (LMV793)
8-Pin SOIC/MSOP (LMV794)
20216301
Top View
20216302
20216385
Top View
Top View
Ordering Information
Package
5-Pin SOT23
Part Number
LMV793MF
LMV793MFX
LMV793MA
8-Pin SOIC
LMV793MAX
LMV794MA
LMV794MAX
8-Pin MSOP
LMV794MM
LMV794MMX
Package Marking
AS4A
LMV793MA
LMV794MA
AN4A
5
Transport Media
1k Units Tape and Reel
3k Units Tape and Reel
NSC Drawing
MF05A
95 Units/Rail
2.5k Units Tape and Reel
95 Units/Rail
M08A
2.5k Units Tape and Reel
1k Units Tape and Reel
3.5k Units Tape and Reel
MUA08A
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LMV793/LMV794
Typical Performance Characteristics
Unless otherwise specified, TA = 25°C, V– = 0, V+ = Supply Voltage
= 5V, VCM = V+/2.
Supply Current vs. Supply Voltage (LMV793)
Supply Current vs. Supply Voltage (LMV794)
20216305
20216381
VOS vs. VCM
VOS vs. VCM
20216351
20216309
VOS vs. VCM
VOS vs. Supply Voltage
20216311
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20216312
6
LMV793/LMV794
Slew Rate vs. Supply Voltage
Input Bias Current vs. VCM
20216352
20216362
Input Bias Current vs. VCM
Sourcing Current vs. Supply Voltage
20216387
20216320
Sinking Current vs. Supply Voltage
Sourcing Current vs. Output Voltage
20216350
20216319
7
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LMV793/LMV794
Sinking Current vs. Output Voltage
Positive Output Swing vs. Supply Voltage
20216317
20216354
Negative Output Swing vs. Supply Voltage
Positive Output Swing vs. Supply Voltage
20216315
20216316
Negative Output Swing vs. Supply Voltage
Positive Output Swing vs. Supply Voltage
20216314
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20216318
8
Input Referred Voltage Noise vs. Frequency
20216339
20216313
Overshoot and Undershoot vs. CLOAD
THD+N vs. Frequency
20216326
20216330
THD+N vs. Frequency
THD+N vs. Peak-to-Peak Output Voltage (VOUT)
20216304
20216374
9
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LMV793/LMV794
Negative Output Swing vs. Supply Voltage
LMV793/LMV794
THD+N vs. Peak-to-Peak Output Voltage (VOUT)
Open Loop Gain and Phase
20216306
20216375
Closed Loop Output Impedance vs. Frequency
Small Signal Transient Response, AV = +10
20216353
20216332
Large Signal Transient Response, AV = +10
Small Signal Transient Response, AV = +10
20216355
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20216357
10
LMV793/LMV794
Large Signal Transient Response, AV = +10
PSRR vs. Frequency
20216363
20216370
CMRR vs. Frequency
Input Common Mode Capacitance vs. VCM
20216356
20216376
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LMV793/LMV794
The LMV793/LMV794 require a gain of ±10 to be stable.
However, with an external compensation network (a simple
RC network) these parts can be stable with gains of ±1 and
still maintain the higher slew rate. Looking at the Bode plots
for the LMV793 and its closest equivalent unity gain stable op
amp, the LMV796, one can clearly see the increased bandwidth of the LMV793. Both plots are taken with a parallel
combination of 20 pF and 10 kΩ for the output load.
Application Information
ADVANTAGES OF THE LMV793/LMV794
Wide Bandwidth at Low Supply Current
The LMV793/LMV794 are high performance op amps that
provide a GBW of 88 MHz with a gain of 10 while drawing a
low supply current of 1.15 mA. This makes them ideal for providing wideband amplification in data acquisition applications.
With the proper external compensation the LMV793/LMV794
can be operated at gains of ±1 and still maintain much faster
slew rates than comparable unity gain stable amplifiers. The
increase in bandwidth and slew rate is obtained without any
additional power consumption over the LMV796.
Low Input Referred Noise and Low Input Bias Current
The LMV793/LMV794 have a very low input referred voltage
at 1 kHz). A CMOS input stage ennoise density (5.8 nV/
sures a small input bias current (100 fA) and low input referred
current noise (0.01 pA/
). This is very helpful in maintaining signal integrity, and makes the LMV793/LMV794 ideal for
audio and sensor based applications.
Low Supply Voltage
The LMV793 and LMV794 have performance guaranteed at
2.5V and 5V supply. These parts are guaranteed to be operational at all supply voltages between 2.0V and 5.5V, for
ambient temperatures ranging from −40°C to 125°C, thus utilizing the entire battery lifetime. The LMV793/LMV794 are
also guaranteed to be operational at 1.8V supply voltage, for
temperatures between 0°C and 125°C optimizing their usage
in low-voltage applications.
20216322
FIGURE 1. LMV793 AVOL vs. Frequency
RRO and Ground Sensing
Rail-to-rail output swing provides the maximum possible dynamic range. This is particularly important when operating at
low supply voltages. An innovative positive feedback scheme
is used to boost the current drive capability of the output
stage. This allows the LMV793/LMV794 to source more than
40 mA of current at 1.8V supply. This also limits the performance of these parts as comparators, and hence the usage
of the LMV793 and the LMV794 in an open-loop configuration
is not recommended. The input common-mode range includes the negative supply rail which allows direct sensing at
ground in single supply operation.
Small Size
The small footprint of the LMV793 and the LMV794 package
saves space on printed circuit boards, and enables the design
of smaller electronic products, such as cellular phones,
pagers, or other portable systems. Long traces between the
signal source and the op amp make the signal path more
susceptible to noise pick up.
The physically smaller LMV793/LMV794 packages, allow the
op amp to be placed closer to the signal source, thus reducing
noise pickup and maintaining signal integrity.
20216323
FIGURE 2. LMV796 AVOL vs. Frequency
Figure 1 shows the much larger 88 MHz bandwidth of the
LMV793 as compared to the 17 MHz bandwidth of the
LMV796 shown in Figure 2. The decompensated LMV793
has five times the bandwidth of the LMV796.
What is a Decompensated Op Amp?
The differences between the unity gain stable op amp and the
decompensated op amp are shown in Figure 3. This Bode plot
assumes an ideal two pole system. The dominant pole of the
decompensated op amp is at a higher frequency, f1, as compared to the unity-gain stable op amp which is at fd as shown
in Figure 3. This is done in order to increase the speed capability of the op amp while maintaining the same power dissipation of the unity gain stable op amp. The LMV793/LMV794
have a dominant pole at 8.6 Hz. The unity gain stable
LMV796/LMV797 have their dominant pole at 1.6 Hz.
USING THE DECOMPENSATED LMV793
Advantages of Decompensated Op Amps
A unity gain stable op amp, which is fully compensated, is
designed to operate with good stability down to gains of ±1.
The large amount of compensation does provide an op amp
that is relatively easy to use; however, a decompensated op
amp is designed to maximize the bandwidth and slew rate
without any additional power consumption. This can be very
advantageous.
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LMV793/LMV794
20216325
FIGURE 4. LMV793 with Lead-Lag Compensation for
Inverting Configuration
20216324
To cover how to calculate the compensation network values
it is necessary to introduce the term called the feedback factor
or F. The feedback factor F is the feedback voltage VA-VB
across the op amp input terminals relative to the op amp output voltage VOUT.
FIGURE 3. Open Loop Gain for Unity-Gain Stable Op Amp
and Decompensated Op Amp
Having a higher frequency for the dominate pole will result in:
1. The DC open-loop gain (AVOL) extending to a higher
frequency.
2. A wider closed loop bandwidth.
3. Better slew rate due to reduced compensation
capacitance within the op amp.
The second open loop pole (f2) for the LMV793/LMV794 occurs at 45 MHz. The unity gain (fu’) occurs after the second
pole at 51 MHz. An ideal two pole system would give a phase
margin of 45° at the location of the second pole. The LMV793/
LMV794 have parasitic poles close to the second pole, giving
a phase margin closer to 0°. Therefore it is necessary to operate the LMV793/LMV794 at a closed loop gain of 10 or
higher, or to add external compensation in order to assure
stability.
For the LMV796, the gain bandwidth product occurs at 17
MHz. The curve is constant from fd to fu which occurs before
the second pole.
For the LMV793/LMV794, the GBW = 88 MHz and is constant
between f1 and f2. The second pole at f2 occurs before AVOL
= 1. Therefore fu’ occurs at 51 MHz, well before the GBW
frequency of 88 MHz. For decompensated op amps the unity
gain frequency and the GBW are no longer equal. Gmin is the
minimum gain for stability and for the LMV793/LMV794 this
is a gain of 10 or 20 dB.
From feedback theory the classic form of the feedback equation for op amps is:
A is the open loop gain of the amplifier and AF is the loop gain.
Both are highly important in analyzing op amps. Normally AF
>>1 and so the above equation reduces to:
Deriving the equations for the lead-lag compensation is beyond the scope of this datasheet. The derivation is based on
the feedback equations that have just been covered. The inverse of feedback factor for the circuit in Figure 4 is:
Input Lead-Lag Compensation
The recommended technique which allows the user to compensate the LMV793/LMV794 for stable operation at any gain
is lead-lag compensation. The compensation components
added to the circuit allow the user to shape the feedback
function to make sure there is sufficient phase margin when
the loop gain is as low as 0 dB and still maintain the advantages over the unity gain op amp. Figure 4 shows the leadlag configuration. Only RC and C are added for the necessary
compensation.
(1)
where 1/F's pole is located at
(2)
1/F's zero is located at
(3)
(4)
13
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LMV793/LMV794
The circuit gain for Figure 4 at low frequencies is −RF/RIN, but
F, the feedback factor is not equal to the circuit gain. The
feedback factor is derived from feedback theory and is the
same for both inverting and non-inverting configurations. Yes,
the feedback factor at low frequencies is equal to the gain for
the non-inverting configuration.
(5)
From this formula, we can see that
• 1/F's zero is located at a lower frequency compared with
1/F's pole.
• 1/F's value at low frequency is 1 + RF/RIN.
• This method creates one additional pole and one
additional zero.
• This pole-zero pair will serve two purposes:
— To raise the 1/F value at higher frequencies prior to its
intercept with A, the open loop gain curve, in order to
meet the Gmin = 10 requirement. For the LMV793/
LMV794 some overcompensation will be necessary for
good stability.
— To achieve the previous purpose above with no
additional loop phase delay.
Please note the constraint 1/F ≥ Gmin needs to be satisfied
only in the vicinity where the open loop gain A and 1/F intersect; 1/F can be shaped elsewhere as needed. The 1/F pole
must occur before the intersection with the open loop gain A.
In order to have adequate phase margin, it is desirable to follow these two rules:
Rule 1 1/F and the open loop gain A should intersect at the
frequency where there is a minimum of 45° of phase
margin. When over-compensation is required the intersection point of A and 1/F is set at a frequency
where the phase margin is above 45°, therefore increasing the stability of the circuit.
Rule 2 1/F’s pole should be set at least one decade below
the intersection with the open loop gain A in order to
take advantage of the full 90° of phase lead brought
by 1/F’s pole which is F’s zero. This ensures that the
effect of the zero is fully neutralized when the 1/F and
A plots intersect each other.
20216348
FIGURE 5. LMV793/LMV794 Simplified Bode Plot
To obtain stable operation with gains under 10 V/V the open
loop gain margin must be reduced at high frequencies to
where there is a 45° phase margin when the gain margin of
the circuit with the external compensation is 0 dB. The pole
and zero in F, the feedback factor, control the gain margin at
the higher frequencies. The distance between F and AVOL is
the gain margin; therefore, the unity gain point (0 dB) is where
F crosses the AVOL curve.
For the example being used RIN = RF for a gain of −1. Therefore F = 6 dB at low frequencies. At the higher frequencies
the minimum value for F is 18 dB for 45° phase margin. From
Equation 5 we have the following relationship:
Now set RF = RIN = R. With these values and solving for RC
we have RC = R/5.9. Note that the value of C does not affect
the ratio between the resistors. Once the value of the resistors
are set, then the position of the pole in F must be set. A
2 kΩ resistor is used for RF and RIN in this design. Therefore
the value for RC is set at 330Ω, the closest standard value for
2 kΩ/5.9.
Rewriting Equation 2 to solve for the minimum capacitor value
gives the following equation:
Calculating Lead-Lag Compensation for LMV793/
LMV794
Figure 5 is the same plot as Figure 1, but the AVOL and phase
curves have been redrawn as smooth lines to more readily
show the concepts covered, and to clearly show the key parameters used in the calculations for lead-lag compensation.
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C = 1/(2πfpRC)
The feedback factor curve, F, intersects the AVOL curve at
about 12 MHz. Therefore the pole of F should not be any
larger than 1.2 MHz. Using this value and Rc = 330Ω the minimum value for C is 390 pF. Figure 6 shows that there is too
much overshoot, but the part is stable. Increasing C to 2.2 nF
did not improve the ringing, as shown in Figure 7.
14
LMV793/LMV794
20216310
20216303
FIGURE 9. RC = 240Ω and C = 2.2 nF, Gain = −1
FIGURE 6. First Try at Compensation, Gain = −1
To summarize, the following steps were taken to compensate
the LMV793 for a gain of −1:
1. Values for Rc and C were calculated from the Bodie plot
to give an expected phase margin of 45°. The values
were based on RIN = RF = 2 kΩ. These calculations gave
Rc = 330Ω and C = 390 pF.
2. To reduce the ringing C was increased to 2.2 nF which
moved the pole of F, the feedback factor, farther away
from the AVOL curve.
3. There was still too much ringing so 2 dB of overcompensation was added to F. This was done by
decreasing RC to 240Ω.
The LMV796 is the fully compensated part which is comparable to the LMV793. Using the LMV796 in the same setup,
but removing the compensation network, provide the response shown in Figure 10 .
20216307
FIGURE 7. C Increased to 2.2 nF, Gain = −1
Some over-compensation appears to be needed for the desired overshoot characteristics. Instead of intersecting the
AVOL curve at 18 dB, 2 dB of over-compensation will be used,
and the AVOL curve will be intersected at 20 dB. Using Equation 5 for 20 dB, or 10 V/V, the closest standard value of RC
is 240Ω. The following two waveforms show the new resistor
value with C = 390 pF and 2.2 nF. Figure 9 shows the final
compensation and a very good response for the 1 MHz
square wave.
20216321
FIGURE 10. LMV796 Response
For large signal response the rise and fall times are dominated by the slew rate of the op amps. Even though both parts
are quite similar the LMV793 will give rise and fall times about
2.5 times faster than the LMV796. This is possible because
the LMV793 is a decompensated op amp and even though it
is being used at a gain of −1, the speed is preserved by using
a good technique for external compensation.
20216308
FIGURE 8. RC = 240Ω and C = 390 pF, Gain = −1
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LMV793/LMV794
The most difficult op amp configuration to stabilize is the gain
of +1. With proper compensation the LMV793/LMV794 can
be used in this configuration and still maintain higher speeds
than the fully compensated parts. Figure 13 shows the gain =
1, or the buffer configuration, for these parts.
Non-Inverting Compensation
For the non-inverting amp the same theory applies for establishing the needed compensation. When setting the inverting
configuration for a gain of −1, F has a value of 2. For the noninverting configuration both F and the actual gain are the
same, making the non-inverting configuration more difficult to
compensate. Using the same circuit as shown in Figure 4, but
setting up the circuit for non-inverting operation (gain of +2)
results in similar performance as the inverting configuration
with the inputs set to half the amplitude to compensate for the
additional gain. Figure 11 below shows the results.
20216384
FIGURE 13. LMV793 with Lead-Lag Compensation for
Non-Inverting Configuration
Figure 13 is the result of using Equation 5 and additional experimentation in the lab. RP is not part of Equation 5, but it is
necessary to introduce another pole at the input stage for
good performance at gain = +1. Equation 5 is shown below
with RIN = ∞.
20216382
FIGURE 11. RC = 240Ω and C = 2.2 nF, Gain = +2
Using 2 kΩ for RF and solving for RC gives RC = 2000/6.9 =
290Ω. The closest standard value for RC is 300Ω. After some
fine tuning in the lab RC = 330Ω and RP = 1.5 kΩ were
choosen as the optimum values. RP together with the input
capacitance at the non-inverting pin inserts another pole into
the compensation for the LMV793/LMV794. Adding this pole
and slightly reducing the compensation for 1/F (using a slightly higher resistor value for RC) gives the optimum response
for a gain of +1. Figure 14 is the response of the circuit shown
in Figure 13. Figure 15 shows the response of the LMV796 in
the buffer configuration with no compensation and RP = RF =
0.
20216383
FIGURE 12. LMV796 Response Gain = +2
The response shown in Figure 11 is close to the response
shown in Figure 9. The part is actually slightly faster in the
non-inverting configuration. Decreasing the value of RC to
around 200Ω can decrease the negative overshoot but will
have slightly longer rise and fall times. The other option is to
add a small resistor in series with the input signal. Figure 12
shows the performance of the LMV796 with no compensation.
Again the decompensated parts are almost 2.5 times faster
than the fully compensated op amp.
20216388
FIGURE 14. RC = 330Ω and C = 10 nF, Gain = +1
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16
LMV793/LMV794
20216361
FIGURE 16. Transimpedance Amplifier
Figure 16 is the complete schematic for a transimpedance
amplifier. Only the supply bypass capacitors are not shown.
CD represents the photo diode capacitance which is given on
its datasheet. CCM is the input common mode capacitance of
the op amp and, for the LMV793 it is shown in the last drawing
of the Typical Performance Characteristics section of this
datasheet. In Figure 16 the inverting input pin of the LMV793
is kept at virtual ground. Even though the diode is connected
to the 2.5V line, a power supply line is AC ground, thus CD is
connected to ground.
Figure 17 shows the schematic needed to derive F, the feedback factor, for a transimpedance amplifier. In this figure CD
+ CCM = CIN. Therefore it is critical that the designer knows
the diode capacitance and the op amp input capacitance. The
photo diode is close to an ideal current source once its capacitance is included in the model. What kind of circuit is this?
Without CF there is only an input capacitor and a feedback
resistor. This circuit is a differentiator! Remember, differentiator circuits are inherently unstable and must be compensated. In this case CF compensates the circuit.
20216389
FIGURE 15. LMV796 Response Gain = +1
With no increase in power consumption the decompensated
op amp offers faster speed over the compensated equivalent
part. These examples used RF = 2 kΩ. This value is high
enough to be easily driven by the LMV793/LMV794, yet small
enough to minimize the effects from the parasitic capacitance
of both the PCB and the op amp.
Note: When using the LMV793/LMV794, proper high frequency PCB layout must be followed. The GBW of these parts
is 88 MHz, making the PCB layout significantly more critical
than when using the compensated counterparts which have
a GBW of 17 MHz.
TRANSIMPEDANCE AMPLIFIER
An excellent application for either the LMV793 or the LMV794
is as a transimpedance amplifier. With a GBW product of 88
MHz these parts are ideal for high speed data transmission
by light. The circuit shown on the front page of the datasheet
is the circuit used to test the LMV793/LMV794 as transimpedance amplifiers. The only change is that VB is tied to
the VCC of the part, thus the direction of the diode is reversed
from the circuit shown on the front page.
Very high speed components were used in testing to check
the limits of the LMV793/LMV794 in a transimpedance configuration. The photo diode part number is PIN-HR040 from
OSI Optoelectronics. The diode capacitance for this part is
only about 7 pF for the 2.5V bias used (VCC to virtual ground).
The rise time for this diode is 1 nsec. A laser diode was used
for the light source. Laser diodes have on and off times under
5 nsec. The speed of the selected optical components allowed an accurate evaluation of the LMV793 as a transimpedance amplifier. Nationals Evaluation Board for decompensated op amps, PN 551013271-001 A, was used and only
minor modifications were necessary and no traces had to be
cut.
20216364
FIGURE 17. Transimpedance Feedback Model
17
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LMV793/LMV794
Using feedback theory, F = VA/VOUT, this becomes a voltage
divider giving the following equation:
After a bit of algebraic manipulation the above equation reduces to:
The noise gain is 1/F. Because this is a differentiator circuit,
a zero must be inserted. The location of the zero is given by:
In the above equation the only unknown is CF. In trying to
solve this equation the fourth power of CF must be dealt with.
An excel spread sheet with this equation can be used and all
the known values entered. Then through iteration, the value
of CF when both sides are equal will be found. That is the
correct value for CF, and of course the closest standard value
is used for CF.
Before moving the lab, the transfer function of the transimpedance amplifier must be found and the units must be in
Ohms.
CF has been added for stability. The addition of this part adds
a pole to the circuit. The pole is located at:
To attain maximum bandwidth and still have good stability the
pole is to be located on the open loop gain curve which is A.
If additional compensation is required one can always increase the value of CF, but this will also reduce the bandwidth
of the circuit. Therefore A = 1/F, or AF = 1. For A the equation
is:
The LMV793 was evaluated for RF = 10 kΩ and 100 kΩ, representing a somewhat lower gain configuration and with the
100 kΩ feedback resistor a fairly high gain configuration. The
RF = 10 kΩ is covered first. Looking at the Input Common
Mode Capacitance vs. VCM chart for CCM for the operating
point selected CCM = 15 pF. Note that for split supplies VCM =
2.5V, CIN = 22 pF and fGBW = 88 MHz. Solving for CF the calculated value is 1.75 pF, so 1.8 pF is selected for use.
Checking the frequency of the pole finds that it is at 8.8 MHz,
which is right at the minimum gain recommended for this part.
Some over compensation was necessary for stability and the
final selected value for CF is 2.7 pF. This moves the pole to
5.9 MHz. Figure 18 and Figure 19 show the rise and fall times
obtained in the lab with a 1V output swing. The laser diode
was difficult to drive due to thermal effects making the starting
and ending point of the pulse quite different, therefore the two
separate scope pictures.
The expression fGBW is the gain bandwidth product of the part.
For a unity gain stable part this is the frequency where A = 1.
For the LMV793 fGBW = 88 MHz. Multiplying A and F results
in the following equation:
For the above equation s = jω. To find the actual amplitude of
the equation the square root of the square of the real and
imaginary parts are calculated. At the intersection of F and A,
we have:
20216390
FIGURE 18. Fall Time
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18
LMV793/LMV794
20216391
20216392
FIGURE 19. Rise Time
FIGURE 20. High Gain Response
In Figure 18 the ringing and the hump during the on time is
from the laser. The higher drive levels for the laser gave ringing in the light source as well as light changing from the
thermal characteristics. The hump is due to the thermal characteristics.
Solving for CF using a 100 kΩ feedback resistor, the calculated value is 0.54 pF. One of the problems with more gain is
the very small value for CF. A 0.5 pF capacitor was used, its
measured value being 0.64 pF. For the 0.64 pF location the
pole is at 2.5 MHz. Figure 20 shows the response for a 1V
output.
A transimpedance amplifier is an excellent application for the
LMV793. Even with the high gain using a 100 kΩ feedback
resistor, the bandwidth is still well over 1 MHz. Other than a
little over compensation for the 10 kΩ feedback resistor configuration using the LMV793 was quite easy. Of course a very
good board layout was also used for this test. For information
on photo diodes please contact OSI Optoelectronics, (310)
978-0516. For further information on transimpedance amplifiers please contact your National Semiconductor representative.
19
www.national.com
LMV793/LMV794
Physical Dimensions inches (millimeters) unless otherwise noted
5-Pin SOT23
NS Package Number MF05A
8-Pin SOIC
NS Package Number M08A
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20
LMV793/LMV794
8-Pin MSOP
NS Package Number MUA08A
21
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LMV793/LMV794 88 MHz, Low Noise, 1.8V CMOS Input, Decompensated Operational Amplifiers
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