7
LT1193
1193fb
TEMPERATURE (°C)
–50
300
SLEW RATE (V/µs)
500
700
800
–25 125
LT1193 • TPC20
0 25 50 75 100
V
S
= ±5V
T
A
= 25°C
R
L
= 1k
V
O
= ±2V
900
600
400
+SLEW RATE
–SLEW RATE
SETTLING TIME (ns)
40
–4
OUTPUT VOLTAGE STEP (V)
–2
2
4
50 100
LT1193 • TPC21
60 70 80 90
V
S
= ±5V
T
A
= 25°C
R
L
= 1k
0
10mV
10mV
LOAD RESISTANCE (Ω)
10
–5
OUTPUT VOLTAGE SWING (V)
–3
1
5
100 1000
LT1193 • TPC19
V
S
= ±5V
3
–1
T
A
= –55°C
T
A
= 25°C
T
A
= 125°C
T
A
= 125°C
T
A
= –55°C, 25°C
Large-Signal Transient Response
TYPICAL PERFOR A CE CHARACTERISTICS
UW
Output Voltage Swing
vs Load Resistance
Slew Rate vs Temperature
Output Voltage Step
vs Settling Time, A
V
= 2
Small-Signal Transient Response Small-Signal Transient Response
LT1193 • TPC22
A
V
= 2, R
L
= 150Ω, R
FB
= 300Ω, R
G
= 300Ω
LT1193 • TPC23
A
V
= –10, SMALL-SIGNAL RISE TIME = 43ns
LT1193 • TPC24
A
V
= 2, R
FB
= 300Ω, R
G
= 300Ω,
OVERSHOOT = 25%, RISE TIME = 4.7ns
APPLICATIO S I FOR ATIO
WUUU
The LT1193 is a video difference amplifier which has two
uncommitted high input impedance (+) and (–) inputs.
The amplifier has one set of inputs that can be used for
reference and feedback. Additionally, this set of inputs
give gain adjust and DC control to the differential amplifier.
The voltage gain of the LT1193 is set like a conventional
operational amplifier. Feedback is applied to Pin 8 and it is
optimized for gains of 2 or greater. The amplifier can be
operated single-ended by connecting either the (+) or (–)
inputs to +/REF, Pin 1. The voltage gain is set by the
resistors: (R
FB
+ R
G
)/R
G
.
The primary usefulness of the LT1193 is in converting
high speed differential signals to a single-ended output.
The amplifier has common mode rejection beyond 50MHz
and a full-power bandwidth of 40MHz at 4V
P-P
. Like the
single-ended case, the differential voltage gain is set by the
external resistors: (R
FB
+ R
G
)/R
G
. The maximum input
differential signal for which the output will respond is
approximately ±1.3V.
Power Supply Bypassing
The LT1193 is quite tolerant of power supply bypassing.
In some applications a 0.1µF ceramic disc capacitor
placed 1/2 inch from the amplifier is all that is required. A
scope photo of the amplifier output with no supply by-
passing is used to demonstrate this bypassing tolerance,
R
L
= 1k.