Wide Supply Range: VS = ±2.5V to ±15V
(Enhanced θJA 16-Pin SO Package)
■
Enhanced θJA SO-8 Package for ±5V Operation
■
0.02% Differential Gain: AV = 2, RL = 150Ω
■
0.015° Differential Phase: AV = 2, RL = 150Ω
■
±13V Output Swing: IL = 100mA, VS = ±15V
■
±3.1V Output Swing: IL = 100mA, VS = ±5V
■
55ns Settling Time to 0.1%, 10V Step
■
Thermal Shutdown Protection
U
APPLICATIONS
■
Twisted-Pair Drivers
■
Video Amplifiers
■
Cable Drivers
■
Test Equipment Amplifiers
■
Buffers
LT1497
Dual 125mA, 50MHz
Current Feedback Amplifier
U
DESCRIPTION
The LT®1497 dual current feedback amplifier features low
power, high output drive, excellent video characteristics
and outstanding distortion performance. From a low 7mA
maximum supply current per amplifier, the LT1497 drives
±100mA with only 1.9V of headroom. Twisted pairs can be
driven differentially with – 70dBc distortion up to 1MHz for
±40mA peak signals.
The LT1497 is available in a low thermal resistance 16-pin
SO package for operation with supplies up to ± 15V. For
±5V operation the device is also available in a low thermal
resistance SO-8 package. The device has thermal and
current limit circuits that protect against fault conditions.
The LT1497 is manufactured on Linear Technology’s
complementary bipolar process. The device has characteristics that bridge the performance between the LT1229
and LT1207 dual current feedback amplifiers. The LT1229
has 30mA output drive, 100MHz bandwidth and 12mA
supply current. The LT1207 has 250mA output drive,
60MHz bandwidth and 40mA supply current.
, LTC and LT are registered trademarks of Linear Technology Corporation.
VS = ±15V, RF = RG = 510Ω, RL = 50Ω0.19%
VS = ±5V, RF = RG = 510Ω, RL = 150Ω0.08%
V
= ±5V, RF = RG = 510Ω, RL = 50Ω0.41%
S
VS = ±15V, RF = RG = 510Ω, RL = 50Ω0.235Deg
VS = ±5V, RF = RG = 510Ω, RL = 150Ω0.045Deg
V
= ±5V, RF = RG = 510Ω, RL = 50Ω0.310Deg
S
●400V/µs
●150V/µs
The ● denotes specifications which apply over the full operating
temperature range.
Note 1: Applies to short circuits to ground only. A short circuit between the
output and either supply may damage the part when operated on supplies
greater than ±10V
Note 2: The LT1497 is designed, characterized and expected to operate
over the temperature range of –40°C to 85°C, but is not tested at –40°C
and 85°C. Guaranteed industrial grade parts are available, consult factory.
Note 3: Thermal resistance varies depending upon the amount of PC board
metal attached to the device. θ
covered with 2oz copper on both sides.
is specified for a 2500mm2 test board
JA
Note 4: Slew rate is measured between ±5V on a ±10V output signal while
operating on ±15V supplies with R
On ±5V supplies slew rate is measured between ±1V on a ±3V output
signal. The slew rate is much higher when the input is overdriven and
when the amplifier is operated inverting. See the Applications Information
section.
Note 5: NTSC composite video with an amplifier output level of 2V peak.
= 453Ω, RG = 49.9Ω and RL = 150Ω.
F
4
LT1497
SUPPLY VOLTAGE (±V)
0
0
–3dB BANDWIDTH (MHz)
10
30
40
50
12
90
1497 G03
20
618
10
416
8
214
60
70
80
PEAKING ≤ 1dB
PEAKING ≤ 5dB
RF = 470Ω
R
F
= 560Ω
RF = 750Ω
RF = 1k
GAIN = 2
R
L
= 100Ω
W
UU
SMALL-SIGNAL BANDWIDTH
VS = ±15V, Peaking ≤ 1dB
A
V
–115056056059.2
1150560–57.0
215051051059.1
101502703043.4
R
L
R
F
R
G
5056056043.1
2062062030.0
50560–42.7
20560–30.3
5056056041.7
2062062020.7
502703030.9
202703019.0
–3dB BW (MHz)
VS = ±5V, Peaking ≤ 1dB
A
V
–115051051045.0
1150510–44.3
215051051041.7
101502703028.1
UW
TYPICAL PERFORMANCE CHARACTERISTICS
Voltage Gain and Phase
vs Frequency, Gain = 6dB
9
8
7
6
5
4
3
VOLTAGE GAIN (dB)
2
1
RL = 100Ω
0
= RG = 560Ω
R
F
–1
0.1
PHASE
GAIN
110100
FREQUENCY (MHz)
±5V
±5V
±15V
±15V
1497 G01
0
45
90
PHASE SHIFT (DEG)
135
180
225
270
–3dB Bandwidth
vs Supply Voltage
90
80
70
60
50
40
30
–3dB BANDWIDTH (MHz)
20
10
0
PEAKING ≤ 1dB
PEAKING ≤ 5dB
RF = 470Ω
416
214
0
SUPPLY VOLTAGE (±V)
R
= 560Ω
F
RF = 750Ω
RF = 1k
618
10
8
12
R
L
R
F
R
G
–3dB BW (MHz)
5056056032.0
2056056023.2
50560–31.7
20560–22.9
5056056030.4
2056056021.9
502703021.9
202703014.6
–3dB Bandwidth
vs Supply Voltage
GAIN = 2
= 1k
R
L
1497 G02
28
26
24
22
20
18
16
VOLTAGE GAIN (dB)
14
12
10
8
0.1
Voltage Gain and Phase
vs Frequency, Gain = 20dB
0
PHASE
RL = 100Ω
= 270Ω
R
F
= 30Ω
R
G
110100
FREQUENCY (MHz)
GAIN
±5V
±5V
±15V
±15V
1497 G04
45
90
PHASE SHIFT (DEG)
135
180
225
270
–3dB Bandwidth
vs Supply Voltage
90
80
70
60
50
40
30
–3dB BANDWIDTH (MHz)
20
10
0
PEAKING ≤ 1dB
PEAKING ≤ 5dB
416
214
0
SUPPLY VOLTAGE (±V)
–3dB Bandwidth
vs Supply Voltage
GAIN = 10
= 1k
R
L
= 270Ω
R
F
RF = 560Ω
618
8
RF = 430Ω
RF = 750Ω
RF = 1k
10
12
1497 G05
90
80
70
60
50
40
30
–3dB BANDWIDTH (MHz)
20
10
0
PEAKING ≤ 1dB
PEAKING ≤ 5dB
RF = 560Ω
618
416
214
0
SUPPLY VOLTAGE (±V)
GAIN = 10
= 100Ω
R
L
RF = 430Ω
RF = 750Ω
8
RF = 270Ω
RF = 1k
10
12
1497 G06
5
LT1497
FEEDBACK RESISTOR (kΩ)
10
CAPACITIVE LOAD (pF)
1000
10000
023
1497 G09
1
1
100
RL = 1k
A
V
= 2
PEAKING ≤ 5dB
VS = ±5V
V
S
= ±15V
TEMPERATURE (°C)
–50
200
250
350
0
2575
1497 G15
150
100
–250
50100 125
50
300
OUTPUT SHORT-CIRCUIT CURRENT (mA)
VS = ±15V
R
L
= 1Ω
SINKING
SOURCING
UW
TYPICAL PERFORMANCE CHARACTERISTICS
Differential Phase
vs Supply Voltage
0.5
RF = RG = 510Ω
= 2
A
V
AMPLIFIER OUTPUT = 2V PEAK
0.4
0.3
0.2
DIFFERENTIAL PHASE (DEG)
0.1
RL = 150Ω
0
7
5
9
SUPPLY VOLTAGE (±V)
Output Saturation Voltage
vs Junction Temperature, ±15V
+
V
VS = ±15V
= 50mA
I
–1
–2
IL = 125mA
–3
3
IL = 125mA
2
1
OUTPUT SATURATION VOLTAGE (V)
–
V
–50
–250
L
IL = 100mA
IL = 100mA
IL = 50mA
2575
TEMPERATURE (°C)
RL = 50Ω
RL = 1k
11
13
15
1497 G07
IL = 75mA
IL = 75mA
50100 125
1497 G10
Differential Gain
vs Supply Voltage
0.5
0.4
0.3
0.2
DIFFERENTIAL GAIN (%)
0.1
0
5
RF = RG = 510Ω
= 2
A
V
AMPLIFIER OUTPUT = 2V PEAK
RL = 1k
7
9
SUPPLY VOLTAGE (±V)
Output Saturation Voltage
vs Junction Temperature, ±5V
+
V
VS = ±5V
= 50mA
I
–1
–2
IL = 125mA
–3
3
IL = 125mA
2
1
OUTPUT SATURATION VOLTAGE (V)
–
V
–50
–250
L
IL = 100mA
IL = 100mA
IL = 50mA
2575
TEMPERATURE (°C)
RL = 50Ω
RL = 150Ω
11
13
1497 G08
IL = 75mA
IL = 75mA
50100 125
1497 G11
Maximum Capacitive Load
vs Feedback Resistor
15
Output Saturation Voltage
vs Junction Temperature, ±2.5V
+
V
VS = ±2.5V
–1
–2
–3
3
2
1
OUTPUT SATURATION VOLTAGE (V)
–
V
–50
–250
IL = 25mA
IL = 50mA
IL = 75mA
IL = 25mA
50100 125
2575
TEMPERATURE (°C)
IL = 75mA
IL = 50mA
1497 G12
Supply Current
vs Ambient Temperature
8.5
8.0
7.5
7.0
6.5
6.0
5.5
SUPPLY CURRENT PER AMPLIFIER (mA)
5.0
–50
6
VS = ±15V
VS = ±5V
–250
TEMPERATURE (°C)
VS = ±2.5V
50100 125
2575
1497 G13
Input Common Mode Limit
vs Junction Temperature
+
V
–0.5
–1.0
–1.5
1.5
1.0
COMMON MODE RANGE (V)
0.5
–
V
–50
–250
V+ = 2V TO 18V
V– = –2V TO –18V
TEMPERATURE (°C)
50100 125
2575
Output Short-Circuit Current
vs Junction Temperature
1497 G14
UW
FREQUENCY (Hz)
–80
OUTPUT TO INPUT CROSSTALK (dB)
–60
–40
–50
–20
–10
–90
–70
–30
10k1M10M100M
1497 G24
–100
–110
100k
VS = ±15V
A
V
= 10
R
L
= 100Ω
R
F
= 560Ω
R
G
= 62Ω
TYPICAL PERFORMANCE CHARACTERISTICS
LT1497
Settling Time to 10mV
vs Output Step
10
8
6
4
2
0
–2
OUTPUT STEP (V)
–4
–6
–8
–10
AV = –1
20
0
AV = 1
SETTLING TIME (ns)
40
A
V
AV = –1
Total Harmonic Distortion
vs Frequency
0.10
VS = ±15V
= 100Ω
R
L
= RG = 560Ω
R
F
0.01
TOTAL HARMONIC DISTORTION (%)
0.001
10100
V
OUT
V
OUT
1k10k100k
FREQUENCY (Hz)
60
= 1
= 7V
= 2V
VS = ±15V
= 560Ω
R
F
80
1497 G16
RMS
RMS
1497 G19
100
Settling Time to 1mV
vs Output Step
10
VS = ±15V
8
= 560Ω
R
F
6
A
= 1
V
4
2
0
–2
OUTPUT STEP (V)
–4
AV = 1
–6
–8
–10
25
0
AV = –1
AV = –1
50
100
75
SETTLING TIME (ns)
125
150
2nd and 3rd Harmonic Distortion
vs Frequency
–20
VS = ±15V
= 5V
= 50Ω
= 560Ω
2ND
3RD
P-P
110
FREQUENCY (MHz)
AV = 1
3RD
V
OUT
–30
R
L
R
F
–40
–50
–60
AV = 1
–70
DISTORTION (dBc)
–80
AV = –1
–90
–100
0.1
175
200
AV = –1
2ND
225
1497 G17
1497 G20
250
Spot Noise Voltage and Current
vs Frequency
100
10
SPOT NOISE (nV/√Hz OR pA/√Hz)
1
10100
1k10k100k
FREQUENCY (Hz)
3rd Order Intercept vs Frequency
40
35
30
25
20
3RD ORDER INTERCEPT (dBm)
15
10
0
101520
5
FREQUENCY (MHz)
VS = ±15V
= 50Ω
R
L
= 270Ω
R
F
= 30Ω
R
G
PO1 = PO2 = 4dBm
–i
n
e
n
+i
n
2530
1497 G18
1497 G21
Output Impedance vs Frequency
100
VS = ±15V
10
1
RF = RG = 1.5k
0.1
OUTPUT IMPEDANCE (Ω)
RF = RG = 560Ω
0.01
10k100k
1M10M100M
FREQUENCY (Hz)
1497 G22
Power Supply Rejection
vs Frequency
80
70
60
50
40
30
20
POWER SUPPLY REJECTION (dB)
10
0
10k1M10M100M
100k
FREQUENCY (Hz)
VS = ±15V
= 50Ω
R
L
= RG = 560Ω
R
F
POSITIVENEGATIVE
Amplifier Crosstalk vs Frequency
1497 G23
7
LT1497
U
WUU
APPLICATIONS INFORMATION
The LT1497 is a dual current feedback amplifier with high
output current drive capability. Bandwidth is maintained
over a wide range of voltage gains by the appropriate
choice of feedback resistor. These amplifiers will drive low
impedance loads such as cables with excellent linearity at
high frequencies.
Feedback Resistor Selection
The optimum value for the feedback resistor is a function
of the operating conditions of the device, the load impedance and the desired flatness of frequency response. The
Small-Signal Bandwidth table gives the values which
result in the highest bandwidth with less than 1dB of
peaking for various gains, loads and supply voltages. If
this level of flatness is not required, a higher bandwidth
can be obtained by use of a lower feedback resistor. The
characteristic curves of Bandwidth vs Supply Voltage
indicate feedback resistors for peaking up to 5dB. These
curves use a solid line when the response has less than
1dB of peaking and a dashed line when the response has
1dB to 5dB of peaking. Note that in a gain of 10 peaking is
always under 1dB for the resistor ranges shown. Reducing
the feedback resistor further than 270Ω in a gain of 10 will
increase the bandwidth, but it also loads the amplifier and
reduces the maximum current available to drive the load.
Capacitive Loads
The LT1497 can drive capacitive loads directly when the
proper value of feedback resistor is used. The graph of
Maximum Capacitive Load vs Feedback Resistor should
be used to select the appropriate value. The graph shows
feedback resistor values for 5dB frequency peaking when
driving a 1k load at a gain of 2. This is a worst-case
condition. The amplifier is more stable at higher gains and
driving heavier loads (smaller load resistors). Alternatively, a small resistor (10Ω to 20Ω) can be put in series
with the output to isolate the capacitive load from the
amplifier output. This has the advantage in that the amplifier bandwidth is only reduced when the capacitive load is
present, and the disadvantage that the gain is a function of
the load resistance.
Capacitance on the Inverting Input
Current feedback amplifiers require resistive feedback
from the output to the inverting input for stable operation.
Take care to minimize the stray capacitance between the
output and the inverting input. Capacitance on the inverting input to ground will cause peaking in the frequency
response (and overshoot in the transient response), but it
does not degrade the stability of the amplifier.
Power Supplies
The LT1497 will operate on single or split supplies from
±2V (4V total) to ±15V (30V total). It is not necessary to
use equal value split supplies, however, the offset voltage
and inverting input bias current will change. The offset
voltage changes about 1mV per volt of supply mismatch.
The inverting bias current can change as much as 10µA
per volt of supply mismatch, though typically the change
is less than 2.5µA per volt.
Thermal Considerations
The LT1497 contains a thermal shutdown feature that
protects against excessive internal (junction) temperature. If the junction temperature of the device exceeds the
protection threshold, the device will begin cycling
between normal operation and an off state. The cycling is
not harmful to the part. The thermal cycling occurs at a
slow rate, typically 10ms to several seconds, depending
upon the power dissipation and the thermal time constants of the package and the amount of copper on the
board under the package. Raising the ambient temperature until the device begins thermal shutdown gives a
good indication of how much margin there is in the
thermal design.
For surface mount devices heat sinking is accomplished
by using the heat spreading capabilities of the PC board
and its copper traces. Experiments have shown that the
heat spreading copper layer does not need to be electrically connected to the leads of the device. The PCB
material can be very effective at transmitting heat between
the pad area attached to V– pins of the device and a ground
8
LT1497
560Ω
–15V
560Ω
–
+
560Ω
560Ω
86.4mA
15V
200Ω
200Ω
1497 F01
–
+
A
–10V
10V
f = 2MHz
U
WUU
APPLICATIONS INFORMATION
or power plane layer either inside or on the opposite side
of the board. Copper board stiffeners and plated throughholes can also be used to spread the heat generated by the
device. Table 1 lists the thermal resistance for several
different board sizes and copper areas. All measurements
were taken in still air on 3/32" FR-4 board with 2oz copper.
This data can be used as a rough guideline in estimating
thermal resistance. The thermal resistance for each application will be affected by thermal interactions with other
components as well as board size and shape.
thermal resistance is 40°C/W. The junction temperature
TJ is:
TJ = (1.24W)(40°C/W) + 85°C = 135°C
The maximum junction temperature for the LT1497 is
150°C, so the heat sinking capability of the board is
adequate for the application.
If the copper area on the PC board is reduced to 180mm
2
the thermal resistance increases to 61°C/W and the junction temperature becomes:
TJ = (1.24W)(61°C/W) + 85°C = 161°C
which is above the maximum junction temperature indicating that the heat sinking capability of the board is
inadequate and should be increased.
Calculating Junction Temperature
The junction temperature can be calculated from the
equation:
TJ = (PD)(θJA) + T
A
TJ = Junction Temperature
TA = Ambient Temperature
PD = Power Dissipation
θJA = Thermal Resistance (Junction-to-Ambient)
As an example, calculate the junction temperature for the
circuit in Figure 1 assuming an 85°C ambient temperature.
The device dissipation can be found by measuring the
supply currents, calculating the total dissipation and then
subtracting the dissipation in the load and feedback network. Both amplifiers are in a gain of –1.
The dissipation for each amplifier is:
The total dissipation is 1.24W. When a 2500mm2 PC
board with 2oz copper on top and bottom is used, the
Unlike a traditional op amp, the slew rate of a current
feedback amplifier is not independent of the amplifier gain
configuration. There are slew rate limitations in both the
input stage and the output stage. In the inverting mode and
for higher gains in the noninverting mode, the signal
amplitude on the input pins is small and the overall slew
rate is that of the output stage. The input stage slew rate
is related to the quiescent current in the input devices.
Referring to the Simplified Schematic, for noninverting
applications the two current sources in the input stage
slew the parasitic internal capacitances at the bases of Q3
and Q4. Consider a positive going input at the base of Q1
and Q2. If the input slew rate exceeds the internal slew rate,
9
LT1497
U
WUU
APPLICATIONS INFORMATION
the normally active emitter of Q2 will turn off as the entire
current available from the current source is used to slew
the base of Q3. The base of Q4 is driven by Q1 without slew
limitation. When the differential input voltage exceeds two
diode drops (about 1.4V) the extra clamp emitter on Q1
turns on and drives the base of Q3 directly. Once the base
of Q3 has been driven within 1.4V of its final value, the
clamp emitter of Q1 turns off and the node must finish
slewing using the current source.
This effect can be seen in Figure 2 which shows the large
signal behavior in a gain of 1 on ±15V supplies. The
clamping action enhances the slew rate beyond the input
limitation, but always leads to slew overshoot after the
clamps turn off. Figure 3 shows that for higher gain
configurations there is much less slew rate enhancement
because the input only moves 2V, barely enough to turn on
the input clamps. In inverting configurations as shown in
Figure 4 the noninverting input does not move so there is
no input slew rate limitation. Slew overshoot is due to
capacitance on the inverting input and can be reduced with
a larger feedback resistor.
The output slew rate is set by the value of the feedback
resistors and the internal capacitance. Larger feedback
resistors will reduce the slew rate as will lower supply
voltages, similar to the way the bandwidth is reduced.
The larger feedback resistors will also cut back on slew
overshoot.
AV = 1
V
= ±15V
S
R
= 560Ω
F
= 100Ω
R
L
1497 F02
Figure 2. Large-Signal Response
WW
SI PLIFIED SCHE ATIC
+IN
= ±15V
S
R
= 560Ω
F
R
= 100Ω
L
RG = 62Ω
AV = 10
V
Figure 3. Large-Signal Response
One Amplifier
Q5
Q3
Q2
–IN
Q1
Q4
Q10
Q6
Q11
Q7
Q8
Q9
Q12
1497 F03
R
AV = –1
V
= ±15V
S
= RG = 560Ω
F
R
= 100Ω
L
Figure 4. Large-Signal Response
+
V
Q13
V
OUT
Q14
–
V
1497 SS
1497 F04
10
U
TYPICAL APPLICATIONS
LT1497
Differential Input/Differential Output Power Amp (AV = 2)
V
IN
+
1/2 LT1497
V
OUT
–
560Ω
1.1k
560Ω
–
–V
1497 TA03
OUT
–V
1/2 LT1497
IN
+
U
PACKAGE DESCRIPTION
0.010 – 0.020
(0.254 – 0.508)
0.008 – 0.010
(0.203 – 0.254)
*
DIMENSION DOES NOT INCLUDE MOLD FLASH. MOLD FLASH
SHALL NOT EXCEED 0.006" (0.152mm) PER SIDE
**
DIMENSION DOES NOT INCLUDE INTERLEAD FLASH. INTERLEAD
FLASH SHALL NOT EXCEED 0.010" (0.254mm) PER SIDE
× 45°
0.016 – 0.050
0.406 – 1.270
0°– 8° TYP
Dimensions in inches (millimeters) unless otherwise noted.
8-Lead Plastic Small Outline (Narrow 0.150)
0.053 – 0.069
(1.346 – 1.752)
0.014 – 0.019
(0.355 – 0.483)
Paralleling Both Amplifiers for Guaranteed 250mA Output Drive
S8 Package
(LTC DWG # 05-08-1610)
0.004 – 0.010
(0.101 – 0.254)
0.050
(1.270)
TYP
V
IN
0.228 – 0.244
(5.791 – 6.197)
560Ω
560Ω
+
1/2 LT1497
–
560Ω
+
1/2 LT1497
–
560Ω
0.189 – 0.197*
(4.801 – 5.004)
7
8
1
2
6
3
3Ω
3Ω
1497 TA04
5
0.150 – 0.157**
(3.810 – 3.988)
4
SO8 0996
V
OUT
0.010 – 0.020
(0.254 – 0.508)
0.008 – 0.010
(0.203 – 0.254)
*
DIMENSION DOES NOT INCLUDE MOLD FLASH. MOLD FLASH
SHALL NOT EXCEED 0.006" (0.152mm) PER SIDE
**
DIMENSION DOES NOT INCLUDE INTERLEAD FLASH. INTERLEAD
FLASH SHALL NOT EXCEED 0.010" (0.254mm) PER SIDE
× 45°
0.016 – 0.050
0.406 – 1.270
(1.346 – 1.752)
0° – 8° TYP
(0.355 – 0.483)
0.053 – 0.069
0.014 – 0.019
Information furnished by Linear Technology Corporation is believed to be accurate and reliable.
However, no responsibility is assumed for its use. Linear Technology Corporation makes no representation that the interconnection of its circuits as described herein will not infringe on existing patent rights.
S Package
16-Lead Plastic Small Outline (Narrow 0.150)
(LTC DWG # 05-08-1610)
16
1
0.050
(1.270)
TYP
0.004 – 0.010
(0.101 – 0.254)
(5.791 – 6.197)
0.228 – 0.244
0.386 – 0.394*
(9.804 – 10.008)
13
14
15
3
2
12
1110
5
4
6
7
9
0.150 – 0.157**
(3.810 – 3.988)
S16 0695
8
11
LT1497
TYPICAL APPLICATION
±4A Current Boosted Power Amp (AV = 10)Frequency Response of Current Boosted Power Amp
U
15V
3Ω
0.033Ω
Q1
D45VH4
V
OUT
6.2Ω
V
IN
200Ω
+
1/2 LT1497
0.01µF
+
V
–
1.8K
200Ω
+
1/2 LT1497
–
6.2Ω
–
V
1.8k
–15V
3Ω
0.01µF
1497 TA05
Q2
D44VH4
0.033Ω
22
21
20
19
18
17
16
VOLTAGE GAIN (dB)
VS = ±15V
15
= 10
A
V
14
= 1.8k
R
F
= 200Ω
R
G
13
= 6V
V
OUT
12
10k
RL = 50Ω
RL = 2.5Ω
P-P
100k1M10M
FREQUENCY (Hz)
1497 TA06
RELATED PARTS
PART NUMBERDESCRIPTIONCOMMENTS
LT1206Single 250mA, 60MHz Current Feedback AmplifierShutdown Function, Stable with CL = 10,000pF,
900V/µs Slew Rate
LT1207Dual 250mA, 60MHz Current Feedback AmplifierDual Version of LT1206
LT1210Single 1A, 30MHz Current Feedback AmplifierHigher Output Version of LT1206
LT1229/LT1230Dual/Quad 100MHz Current Feedback Amplifiers30mA Output Current, 1000V/µs Slew Rate
LT1363/LT1364/LT1365Single/Dual/Quad 70MHz, 1000V/µs, C-LoadTM Amplifiers50mA Output Current, 1.5mV Max VOS, 2µA Max I
C-Load is a trademark of Linear Technology Corporation.