LT1016
7
1016fc
applicaTions inForMaTion
The circuit shown in Figure 1 is the best electronic means
of generating a known fast, clean step to test comparators.
It uses a very fast transistor in a common base configura
-
tion. The transistor is switchedoff” with a fast edge from
the generator and the collector voltage settles to exactly 0V
in just a few nanoseconds. The most important feature of
this circuit is the lack of feedthrough from the generator
to the comparator input. This prevents overshoot on the
comparator input that would give a false fast reading on
comparator response time.
To adjust this circuit for exactly 5mV overdrive, V1 is
adjusted so that the LT1016 output under test settles to
1.4V (in the linear region). Then V1 is changed –5V to set
overdrive at 5mV.
The test circuit shown measures low to high transition
on the “+” input. For opposite polarity transitions on the
output, simply reverse the inputs of the LT1016.
High Speed Design Techniques
A substantial amount of design effort has made the LT1016
relatively easy to use. It is much less prone to oscillation
and other vagaries than some slower comparators, even
with slow input signals. In particular, the LT1016 is
stable
in its linear region, a feature no other high speed compara-
tor has. Additionally, output stage switching does not ap-
preciably
change
power supply current, further enhancing
stability. These features make the application of the 50GHz
gain-bandwidth LT1016 considerably easier than other
fast comparators. Unfortunately, laws of physics dictate
that the circuit environment the LT1016 works in must be
properly prepared. The performance limits of high speed
circuitry are often determined by parasitics such as stray
capacitance, ground impedance and layout. Some of these
considerations are present in digital systems where design
-
ers are comfortable describing bit patterns and memory
access times in terms of nanoseconds. The LT1016 can
be used in such fast digital systems and Figure2 shows
just how fast the device is. The simple test circuit allows
us to see that the LT1016’s (Trace B) response to the pulse
generator (Trace A) is as fast as a TTL inverter (Trace C)
even when the LT1016 has only millivolts of input signal!
Linear circuits operating with this kind of speed make many
engineers justifiably wary. Nanosecond domain linear
circuits are widely associated with oscillations, mysteri
-
ous shifts in circuit characteristics, unintended modes of
operation and outright failure to function.
Figure 1. Response Time Test Circuit
+
PULSE
IN
0V
0V
–100mV
3V
5V
5V
5V
0.1µF
50Ω
25Ω
25Ω
10Ω
400Ω
130Ω
750Ω
10k
2N3866
V1
0.01µF
0.01µF**
LT1016
L
Q
Q
10X SCOPE PROBE
(C
IN
≈ 10pF)
10X SCOPE PROBE
(C
IN
≈ 10pF)
* SEE TEXT FOR CIRCUIT EXPLANATION
** TOTAL LEAD LENGTH INCLUDING DEVICE PIN.
SOCKET AND CAPACITOR LEADS SHOULD BE
LESS THAN 0.5 IN. USE GROUND PLANE
(V
OS
+ OVERDRIVE) • 1000
1016 F01
LT1016
8
1016fc
applicaTions inForMaTion
Other common problems include different measurement
results using various pieces of test equipment, inability
to make measurement connections to the circuit without
inducing spurious responses and dissimilar operation
between twoidentical” circuits. If the components used
in the circuit are good and the design is sound, all of the
above problems can usually be traced to failure to pro
-
vide a proper circuitenvironment.” To
learn how to do
this requires studying the causes of the aforementioned
difficulties.
By
far the most common error involves power supply
bypassing. Bypassing is necessary to maintain low sup
-
ply impedance. DC resistance and inductance in supply
wires and PC traces can quickly build up to unacceptable
levels. This allows the supply line to move as internal
current levels of the devices connected to it change. This
will almost always cause unruly operation. In addition,
several devices connected to an unbypassed supply can
“communicate” through the finite supply impedances,
causing erratic modes. Bypass capacitors furnish a simple
way to eliminate this problem by providing a local reser
-
voir of energy at the device. The bypass capacitor acts
like
an electrical flywheel to keep supply impedance low
at high frequencies. The choice of
what type of capaci-
tors
to use for bypassing is a critical issue and should be
approached
carefully. An unbypassed LT1016 is shown
responding to a pulse input in Figure 3. The power supply
the LT1016 sees at its terminals has high impedance at
high frequency. This impedance forms a voltage divider
with the LT1016, allowing the supply to move as internal
conditions in the comparator change. This causes local
feedback and oscillation occurs. Although the LT1016
responds to
the input pulse, its output is a blur of 100MHz
oscillation.
Always use bypass capacitors.
Figure 2. LT1016 vs a TTL Gate
Figure 3. Unbypassed LT1016 Response
TRACE A
5V/DIV
TRACE B
5V/DIV
TRACE C
5V/DIV
10ns/DIV
+
OUTPUTS
PULSE
GENERATOR
1k
10Ω
V
REF
1016 F02
LT1016
TEST CIRCUIT
7404
2V/DIV
100ns/DIV
1016 F03
LT1016
9
1016fc
applicaTions inForMaTion
In Figure 4 the LT1016’s supplies are bypassed, but it still
oscillates. In this case, the bypass units are either too far
from the device or are lossy capacitors. Use capacitors with
good high frequency characteristics and mount them as
close as possible to the LT1016. An inch of wire between
the capacitor and the LT1016 can cause problems. If op
-
eration in the linear region is desired, the LT1016 must
be over a ground plate with good RF bypass capacitors
(≥0.01µF) having lead lengths less than 0.2 inches. Do
not use sockets.
In Figure 5 the device is properly bypassed but a new
problem pops up. This photo shows both outputs of the
comparator. Trace A appears normal, but Trace B shows an
excursion of almost 8V—quite a trick for a device running
from a 5V supply. This is a commonly reported problem
in high speed circuits and can be quite confusing. It is
not due to suspension of natural law, but is traceable to
a grossly miscompensated or improperly selected oscil
-
loscope probe. Use probes that match your oscilloscope’s
input characteristics and compensate them properly.
Figure 6 shows another probe-induced problem. Here,
the amplitude
seems correct but the 10ns response time
LT1016 appears to have 50ns edges! In this case, the
probe used is too heavily compensated or slow for the
oscilloscope. Never use 1× orstraight” probes. Their
bandwidth is 20MHz or less and capacitive loading is
high. Check probe bandwidth to ensure it is adequate for
the measurement. Similarly, use an oscilloscope with
adequate bandwidth.
Figure 4. LT1016 Response with Poor Bypassing
Figure 5. Improper Probe Compensation Causes
Seemingly Unexplainable Amplitude Error
Figure 6. Overcompensated or Slow Probes
Make Edges Look Too Slow
2V/DIV
100ns/DIV
1016 F04
TRACE A
2V/DIV
TRACE B
2V/DIV
10ns/DIV
1016 F05
1V/DIV
50ns/DIV
1016 F06

LT1016IS8#PBF

Mfr. #:
Manufacturer:
Analog Devices Inc.
Description:
Analog Comparators High Speed COMPARATOR
Lifecycle:
New from this manufacturer.
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