OPA4658

FEATURES

GAIN BANDWIDTH: 900MHz at G = 2

GAIN OF 2 STABLE

LOW POWER: 50mW PER AMP

LOW DIFF GAIN/PHASE ERRORS:
0.015%/0.02

HIGH SLEW RATE: 1700V/

PACKAGE: 14-Pin DIP and SO-14

Quad Wideband, Low Power Current Feedback

OPERATIONAL AMPLIFIER

APPLICATIONS

MEDICAL IMAGING

HIGH-RESOLUTION VIDEO

HIGH-SPEED SIGNAL PROCESSING

COMMUNICATIONS

PULSE AMPLIFIERS

ADC/DAC GAIN AMPLIFIER

MONITOR PREAMPLIFIER

CCD IMAGING AMPLIFIER

DESCRIPTION

The OPA4658 is a quad ultra-wideband, low power
current feedback video operational amplifier featuring
high slew rate and low differential gain/phase error.
The current feedback design allows for superior large
signal bandwidth, even at high gains. The low differ-
ential gain/phase errors, wide bandwidth and low

quiescent current make the OPA4658 a perfect choice
for numerous video, imaging and communications
applications.

The OPA4658 is internally compensated for stability in
gains of 2 or greater. The OPA4658 is also available in
dual (OPA2658) and single (OPA658) configurations.

COMP

Current Mirror

OUT

BIAS

Current Mirror

Buffer

OPA4658

NOTE: Diagram reflects only one-fourth of the OPA4658.

International Airport Industrial Park · Mailing Address: PO Box 11400, Tucson, AZ 85734 · Street Address: 6730 S. Tucson Blvd., Tucson, AZ 85706 · Tel: (520) 746-1111 · Twx: 910-952-1111

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PDS-1270C

Printed in U.S.A. March, 1998

OPA4658

FREQUENCY RESPONSE
Closed-Loop Bandwidth

(2)

G = +2

450

(1)

MHz

G = +5

195

MHz

G = +10

130

MHz

Slew Rate

(3)

G = +2, 2V Step

1700

1000

At Minimum Specified Temperature

1500

900

Settling Time: 0.01%

G = +2, 2V Step

0.1%

G = +2, 2V Step

15.1

G = +2, 2V Step

4.8

Spurious Free Dynamic Range

f = 5MHz, G = +2, V

= 2Vp-p

dBc

f = 20MHz, G = +2, V

= 2Vp-p

dBc

Third-Order Intercept Point

f = 10MHz

dBm

Differential Gain

G = +2, NTSC, V

= 1.4Vp-p, R

= 150

0.015

Differential Phase

G = +2, NTSC, V

= 1.4Vp-p, R

= 150

0.02

degrees

Crosstalk

Input Referred, 5MHz, Three Active Channels

Input Referred, 5MHz, Channel-to-Channel

OFFSET VOLTAGE
Input Offset Voltage

1.5

5.5

Over Temperature

Power Supply Rejection

4.5 to

5.5V

INPUT BIAS CURRENT
Non-Inverting

= 0V

6.5

Over Temperature

Inverting

= 0V

1.1

Over Temperature

NOISE
Input Voltage Noise Density

f = 100Hz

nV/

f = 10kHz

3.6

nV/

f = 1MHz

3.2

nV/

= 100Hz to 200MHz

Vrms

Inverting Input Bias Current

Noise Density: f = 10MHz

pA/

Non-Inverting Input Current

Noise Density: f = 10MHz

pA/

Noise Figure (NF)

= 100

9.5

dBm

= 50

dBm

INPUT VOLTAGE RANGE
Common-Mode Input Range

2.9

Over Temperature

2.5

Common-Mode Rejection

INPUT IMPEDANCE
Non-Inverting

500 || 1

||pF

Inverting

OPEN-LOOP TRANSIMPEDANCE
Open-Loop Transimpedance

2V, R

= 100

150

350

200

360

Over Temperature

2V, R

= 100

100

290

150

300

OUTPUT
Voltage Output

No Load

2.7

3.0

Over Temperature

2.5

2.75

Voltage Output

= 250

2.7

3.0

Over Temperature

2.5

2.7

Voltage Output

= 100

2.2

2.7

Over Temperature

2.0

2.5

Output Current, Sourcing

120

Over Temperature Range

Output Current, Sinking

Over Temperature Range

Short Circuit Current

150

Output Resistance

1MHz, G = +2

0.1

POWER SUPPLY
Specified Operating Voltage

Operating Voltage Range

4.5

5.5

Quiescent Current

All Channels, V

Over Temperature

TEMPERATURE RANGE
Specification: P, U, UB

+85

Thermal Resistance,

C/W

SPECIFICATIONS

OPA4658P, U

OPA4658UB

PARAMETER

CONDITION

MIN

TYP

MAX

MIN

TYP

MAX

UNITS

At T

= +25

C, V

5V, R

= 100

, C

= 2pF, R

= 402

, unless otherwise noted.

NOTES: (1) An asterisk (

) specifies the same value as the grade to the left. (2) Bandwidth can be affected by a non-optimal PC board layout. Refer to the

demonstration board layout for details. (3) Slew rate is rate of change from 10% to 90% of output voltage step.

OPA4658

Output 4

Input 4

+Input 4

+Input 3

Input 3

Output 3

Output 1

Input 1

+Input 1

+Input 2

Input 2

Output 2

ABSOLUTE MAXIMUM RATINGS

Supply ..........................................................................................

5.5VDC

Internal Power Dissipation

(1)

....................... See Applications Information

Differential Input Voltage .............................................................. Total V

Input Voltage Range .................................... See Applications Information
Storage Temperature Range: P, U, UB ........................ 40

C to +125

Lead Temperature (soldering, 10s) .............................................. +300

(soldering, SOIC 3s) ...................................................................... +260

Junction Temperature (T

) ............................................................ +175

NOTE: (1) Packages must be derated based on specified

. Maximum

must be observed.

PACKAGE INFORMATION

PACKAGE DRAWING

PRODUCT

PACKAGE

NUMBER

(1)

OPA4658P

14-Pin Plastic DIP

010

OPA4658U, UB

SO-14 Surface Mount

235

NOTE: (1) For detailed drawing and dimension table, please see end of data
sheet, or Appendix C of Burr-Brown IC Data Book.

PIN CONFIGURATION

Top View

DIP/SO-14

ORDERING INFORMATION

(1)

PRODUCT

PACKAGE

TEMPERATURE RANGE

OPA4658P

14-Pin Plastic DIP

C to +85

OPA4658U, UB

SO-14 Surface Mount

C to +85

NOTE: (1) The "B" grade of the SOIC package will be marked with a "B" by pin 8.
Refer to mechanical section for the location.

ELECTROSTATIC
DISCHARGE SENSITIVITY

This integrated circuit can be damaged by ESD. Burr-Brown
recommends that all integrated circuits be handled with
appropriate precautions. Failure to observe proper handling
and installation procedures can cause damage.

ESD damage can range from subtle performance degradation
to complete device failure. Precision integrated circuits may
be more susceptible to damage because very small parametric
changes could cause the device not to meet its published
specifications.

The information provided herein is believed to be reliable; however, BURR-BROWN assumes no responsibility for inaccuracies or omissions. BURR-BROWN assumes
no responsibility for the use of this information, and all use of such information shall be entirely at the user's own risk. Prices and specifications are subject to change
without notice. No patent rights or licenses to any of the circuits described herein are implied or granted to any third party. BURR-BROWN does not authorize or warrant
any BURR-BROWN product for use in life support devices and/or systems.

OPA4658

TYPICAL PERFORMANCE CURVES

(CONT)

At T

= +25

C, V

5V, R

= 100

, C

= 2pF, R

= 402

unless otherwise noted.

OPEN-LOOP GAIN AND PHASE vs FREQUENCY

Frequency (Hz)

135

180

225

10k

100k

10M

100M

Open-Loop Gain (dB)

Open-Loop Phase (°)

Gain

Phase

COMMON-MODE REJECTION

vs INPUT COMMON-MODE VOLTAGE

Common-Mode Rejection (dB)

Common-Mode Voltage (V)

CLOSED-LOOP BANDWIDTH (G = +5)

Frequency (Hz)

10M

100M

Bandwidth = 205MHz

Gain (dB)

135

180

225

10k

100k

10M

100M

OPEN-LOOP TRANSIMPEDANCE AND PHASE

vs FREQUENCY

Frequency (Hz)

Transimpedance (

)

Open-Loop Phase (°)

Phase

Transimpedance

CLOSED-LOOP BANDWIDTH (G = +10)

Frequency (Hz)

10M

100M

Gain (dB)

Bandwidth = 134MHz

CLOSED-LOOP BANDWIDTH (G = +2)

Frequency (Hz)

10M

100M

10G

Gain (dB)

SO-14 Bandwidth = 458MHz

(Dashed Line)

DIP Bandwidth = 435M

(Solid Line)

OPA4658

For non-inverting operation, the input signal is applied to the
non-inverting (high impedance buffer) input. The output
(buffer) error current (I

) is generated at the low impedance

inverting input. The signal generated at the output is fed back
to the inverting input such that the overall gain is (1 + R

Where a voltage-feedback amplifier has two symmetrical high
impedance inputs, a current feedback amplifier has a low
inverting (buffer output) impedance and a high non-inverting
(buffer input) impedance.

The closed-loop gain for the OPA4658 can be calculated
using the following equations:

(1)

(2)

At higher gains the small value inverting input impedance
causes an apparent loss in bandwidth. This can be seen from
the equation:

(3)

This loss in bandwidth at high gains can be corrected
without affecting stability by lowering the value of the
feedback resistor from the specified value of 402

OFFSET VOLTAGE AND NOISE

The output offset is the algebraic sum of the input offset
voltage and bias current errors. The output offset for non-
inverting operation is calculated by the following equation:

(4)

If all terms are divided by the gain (1 + R

) it can be

observed that input referred offsets improve as gain increases.
The effective noise at the output can be determined by taking

APPLICATIONS INFORMATION

THEORY OF OPERATION

Conventional op amps depend on feedback to drive their
inputs to the same potential, however the current feedback
op amp's inverting and non-inverting inputs are connected
by a unity gain buffer, thus enabling the inverting input to
automatically assume the same potential as the non-invert-
ing input. This results in very low impedance at the inverting
input to sense the feedback as an error current signal.

DISCUSSION OF PERFORMANCE

The OPA4658 is a low-power, unity gain stable, current
feedback operational amplifier which operates on

5V power

supply. The current feedback architecture offers the follow-
ing important advantages over voltage feedback architec-
tures: (1) the high slew rate allows the large signal perfor-
mance to approach the small signal performance, and (2)
there is very little bandwidth degradation at higher gain
settings.

The current feedback architecture of the OPA4658 provides
the traditional strength of excellent large signal response
plus wide bandwidth, making it a good choice for use in high
resolution video, medical imaging and DAC I/V Conver-
sion. The low power requirements make it an excellent
choice for numerous portable applications.

DC GAIN TRANSFER CHARACTERISTICS

The circuit in Figure 1 shows the equivalent circuit for
calculating the DC gain. When operating the device in the
inverting mode, the input signal error current (I

) is ampli-

fied by the open loop transimpedance gain (T

). The output

signal generated is equal to T

. Negative feedback is

applied through R

such that the device operates at a gain

equal to R

FIGURE 1. Equivalent Circuit.

(50

)

Inverting Gain

Loop Gain

Non

Inverting Gain

Loop Gain

where Loop Gain

ACTUAL

(

)

[

]

x 1. 25

(

)

Output Offset Voltage

= ±

F B

FIGURE 2. Output Offset Voltage Equivalent Circuit.

OPA4658

The feedback resistor value acts as the frequency response
compensation element for a current feedback type amplifier.
The 402

used in setting the specification achieves a nomi-

nal maximally flat butterworth response while assuming a
2pF output pin parasitic. Increasing the feedback resistor
will over compensate the amplifier, rolling off the frequency
response, while decreasing it will decrease phase margin,
peaking up the frequency response.

d) Connections to other wideband devices on the board
may be made with short direct traces or through on-board
transmission lines. For short connections, consider the trace
and the input to the next device as a lumped capacitive load.
Relatively wide traces (50 to 100 mils) should be used,
preferably with ground and power planes opened up around
them. Estimate the total capacitive load and set R

ISO

from

the plot of recommended R

ISO

vs capacitive load. Low

parasitic loads may not need an R

ISO

since the OPA4658 is

nominally compensated to operate with a 2pF parasitic load.

If a long trace is required and the 6dB signal loss intrinsic to
doubly terminated transmission lines is acceptable, imple-
ment a matched impedance transmission line using microstrip
or stripline techniques (consult an ECL design handbook for
microstrip and stripline layout techniques). A 50

environ-

ment is not necessary on board, and in fact a higher imped-
ance environment will improve distortion as shown in the
distortion vs load plot. With a characteristic impedance
defined based on board material and desired trace dimen-
sions, a matching series resistor into the trace from the
output of the amplifier 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 the input impedance of
the destination device; the total effective impedance should
match the trace impedance. Multiple destination devices are
best handled as separate transmission lines, each with their
own series and shunt terminations.

If the 6dB attenuation loss of a doubly terminated line is
unacceptable, a long trace can be series-terminated at the
source end only. This will help isolate the line capacitance
from the op amp output, but will not preserve signal integrity
as well as a doubly terminated line. If the shunt impedance
at the destination end is finite, there will be some signal
attenuation due to the voltage divider formed by the series
and shunt impedances.

e) Socketing a high speed part like the OPA4658 is not
recommended. The additional lead length and pin-to-pin
capacitance introduced by the socket creates an extremely
troublesome parasitic network which can make it almost
impossible to achieve a smooth, stable response. Best results
are obtained by soldering the part onto the board. If socket-
ing for the DIP package is desired, high frequency flush
mount pins (e.g., McKenzie Technology #710C) can give
good results.

the root sum of the squares of equation (4) and applying the
spectral noise values found in the Typical Performance Curve
graph section. This applies to noise from the op amp only.
Note that both the noise figure (NF) and the equivalent input
offset voltages improve as the closed loop gain increases (by
keeping R

fixed and reducing R

with R

= 0

INCREASING BANDWIDTH AT HIGH GAINS

The closed-loop bandwidth can be extended at high gains by
reducing the value of the feedback resistor R

. This band-

width reduction is caused by the feedback current being split
between R

and R

(refer to Figure 1). As the gain increases

(for a fixed R

), more feedback current is shunted through

, which reduces closed-loop bandwidth.

CIRCUIT LAYOUT AND BASIC OPERATION

Achieving optimum performance with a high frequency am-
plifier like the OPA4658 requires careful attention to layout
parasitics and selection of external components. Recommen-
dations for PC board layout and component selection include:

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 non-
inverting 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. Otherwise,
ground and power planes should be unbroken elsewhere on
the board.

b) Minimize the distance (< 0.25") from the two power pins
to high frequency 0.1

F decoupling capacitors. At the 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. Larger (2.2

F to 6.8

F) decoupling

capacitors, effective at lower frequencies, should also be
used. 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
OPA4658. Resistors should be a very low reactance type.
Surface mount resistors work best and allow a tighter overall
layout. Metal film or carbon composition axially-leaded
resistors can also provide good high frequency performance.
Again, keep their leads as short as possible. Never use
wirewound type resistors in a high frequency application.

Since the output pin and the inverting input pin are most
sensitive to parasitic capacitance, always position the feed-
back and series output resistor, if any, as close as possible to
the package pins. Other network components, such as non-
inverting input termination resistors, should also be placed
close to the package.

OPA4658

ESD PROTECTION

ESD damage has been well recognized for MOSFET de-
vices, but any semiconductor device is vulnerable to this
potentially damaging source. This is particularly true for
very high speed, fine geometry processes.

ESD damage can cause subtle changes in amplifier input
characteristics without necessarily destroying the device. In
precision operational amplifiers, this may cause a noticeable
degradation of offset voltage and drift. Therefore, ESD
handling precautions are strongly recommended when han-
dling the OPA4658.

OUTPUT DRIVE CAPABILITY

The OPA4658 has been optimized to drive 75

and 100

resistive loads. The device can drive 2Vp-p into a 75

load.

This high-output drive capability makes the OPA4658 an
ideal choice for a wide range of RF, IF, and video applica-
tions. In many cases, additional buffer amplifiers are un-
needed.

Many demanding high-speed applications such as
ADC/DAC buffers require op amps with low wideband
output impedance. For example, low output impedance is
essential when driving the signal-dependent capacitances at
the inputs of flash A/D converters. As shown in Figure 3, the
OPA4658 maintains very low closed-loop output impedance
over frequency. Closed-loop output impedance increases
with frequency since loop gain is decreasing with frequency.

max = (

)

/4R

. Note that it is the voltage across the

output transistor, and not the load, that determines the power
dissipated in the output stage.

The short-circuit condition represents the maximum amount
of internal power dissipation that can be generated. The
variation of output current with temperature is shown in the
Typical Performance Curves.

CAPACITIVE LOADS

The OPA4658's output stage has been optimized to drive
low resistive loads. Capacitive loads, however, will decrease
the amplifier's phase margin which may cause high fre-
quency peaking or oscillations. Capacitive loads greater than
5pF should be buffered by connecting a small resistance,
usually 5

to 25

, in series with the output as shown in

Figure 4. This is particularly important when driving high
capacitance loads such as flash A/D converters.

In general, capacitive loads should be minimized for opti-
mum high frequency performance. Coax lines can be driven
if the cable is properly terminated. The capacitance of coax
cable (29pF/foot for RG-58) will not load the amplifier
when the coaxial cable or transmission line is terminated
with its characteristic impedance.

FIGURE 3. Closed-Loop Output Impedance vs Frequency.

100

0.1

0.01

0.001

10k

100k

10M

100M

Output Impedance (

)

Frequency (Hz)

G = +2

THERMAL CONSIDERATIONS

The OPA4658 does not require a heat sink for operation in
most environments. At extreme temperatures and under full
load conditions a heat sink may be necessary.

The internal power dissipation is given by the equation
P

= P

+ P

, where P

is the quiescent power dissipa-

tion and P

is the power dissipation in the output stage due

to the load. (For

5V, P

= 10V

34mA = 340mW,

max). For the case where the amplifier is driving a grounded
load (R

) with a DC voltage (

OUT

) the maximum value of

occurs at

OUT

/2, and is equal to P

OPA4658

typically 5

to 25

)

402

1/4

COMPENSATION

The OPA4658 is internally compensated and is stable in
gains of two or greater, with a phase margin of approxi-
mately 66

in a gain of +2V/V. (Note that, from a stability

standpoint, an inverting gain of 1V/V is equivalent to a
noise gain of 2.) Gain and phase response for other gains are
shown in the Typical Performance Curves.

The high-frequency response of the OPA4658 in a good
layout is very flat with frequency.

DISTORTION

The OPA4658's Harmonic Distortion characteristics into a
100

load are shown vs frequency and power output in the

Typical Performance Curves. Distortion can be further im-
proved by increasing the load resistance as illustrated in
Figure 5. Remember to include the contribution of the
feedback resistance when calculating the effective load re-
sistance seen by the amplifier.

FIGURE 4. Driving Capacitive Loads.

OPA4658

100

Load Resistance (

)

Harmonic Distortion (dBc)

100

G = +2

The third-order intercept is an important parameter for many
RF amplifier applications. Figure 6 shows the OPA4658's
two tone, third-order intercept vs frequency. This curve is
particularly useful for determining the magnitude of the
third harmonic as a function of frequency, load resistance,
and gain. For example, assume that the application requires
the OPA4658 to operate in a gain of +2V/V and drive
2Vp-p into 100

at a frequency of 10MHz. Referring to

Figure 6 we find that the intercept point is +38dBm. The
magnitude of the third harmonic can now be easily calcu-
lated from the expression:

Third Harmonic (dBc) = 2(OPI

P P

)

where OPI

P = third-order output intercept, dBm

= output level, dBm

For this case OPI

P = 38dBm, P

= 7dBm, and the third

Harmonic = 2(38 7) = 62dB below the fundamental. The
OPA4658's low distortion makes the device an excellent
choice for a variety of RF signal processing applications.

CROSSTALK

Crosstalk is the undesired result of the signal of one channel
mixing with and reproducing itself in the output of another

channel or channels. Crosstalk is inclined to occur in most
multichannel integrated circuits. In quad devices, the effect of
crosstalk is measured by driving three channels and observing
the output of the undriven channel over various frequencies.
The magnitude of this effect is referenced in terms of channel-
to-channel isolation and expressed in decibels. Input referred
points to the fact that there is a direct correlation between gain
and crosstalk, therefore at increased gain, crosstalk also in-
creases by a factor equal to that of the gain. Figure 7 illustrates
the measured effect of crosstalk in the OPA4658U.

FIGURE 5. 5MHz Harmonic Distortion vs Load Resistance.

FIGURE 6. Third Order Intercept Point vs Frequency.

100k

10M

100M

Third Order Intercept Point (dBm)

Frequency (Hz)

G = +2

(G = +2, R

= 100

, R

= 402

)

FIGURE 8. Configuration for Testing Differential Gain/Phase.

OPA4658

402

TEK TSG 130A

TEK VM700A

1/4

DIFFERENTIAL GAIN AND PHASE

Differential Gain (DG) and Differential Phase (DP) are criti-
cal specifications for video applications. DG is defined as the
percent change in closed-loop gain over a specified change in
output voltage level. DP is defined as the change in degrees of
the closed-loop phase over the same output voltage change.
Both DG and DP are specified at the NTSC sub-carrier
frequency of 3.58MHz and the PAL subcarrier of 4.43MHz.
All NTSC measurements were performed using a Tektronix
model VM700A Video Measurement Set.

DG and DP of the OPA4658 were measured with the amplifier
in a gain of +2V/V with 75

input impedance and the output

back-terminated in 75

. The input signal selected from the

generator was a 0V to 1.4V modulated ramp with sync pulse.
With these conditions the test circuit shown in Figure 8
delivered a 100IRE modulated ramp to the 75

input of the

video analyzer. The signal averaging feature of the analyzer

FIGURE 7. Channel-to-Channel Isolation (three active channels).

Frequency (Hz)

10M

100M

Isolation (dB)

G = +2

OPA4658

FIGURE 9. Noise Figure vs Source Resistance.

100

10k

100k

Noise Figure (dB)

Source Resistance (

)

NF = 10LOG 1 +

+ (InR

)

4KTR

TYPICAL APPLICATIONS

FIGURE 10. Low Distortion Video Amplifier.

OPA4658

OUT

402

Video

Input

Transmission Line

1/4

was used to establish a reference against which the perfor-
mance of the amplifier was measured. Signal averaging was
also used to measure the DG and DP of the test signal in order
to eliminate the generator's contribution to measured ampli-
fier performance. Typical performance of the OPA4658 is
0.015% differential gain and 0.02

differential phase to both

NTSC and PAL standards.

NOISE FIGURE

The OPA4658's voltage and current noise spectral densities
are specified in the Typical Performance Curves. For RF
applications, however, Noise Figure (NF) is often the pre-
ferred noise specification since it allows system noise per-
formance to be more easily calculated. The OPA4658's
Noise Figure vs Source Resistance is shown in Figure 9.

SPICE MODELS

Computer simulation using SPICE is often useful when
analyzing the performance of analog circuits and systems.
This is particularly true for Video and RF amplifier circuits
where parasitic capacitance and inductance can have a major
effect on circuit performance. SPICE models using MicroSim
Corporation's PSpice are available for the OPA4658. Evalu-
ation PC boards are also available. Contract Burr-Brown
applications departments to receive a SPICE Diskette.

DEMONSTRATION BOARD

PACKAGE

PRODUCT

DEM-OPA465xP

8-Pin DIP

OPA4658P

DEM-OPA465xU

SO-8

OPA4658U

OPA4658UB

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