LT1720/LT1721
13
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Circuit Description
The block diagram of one comparator in the LT1720/LT1721
is shown in Figure 6. There are differential inputs (+IN/–IN),
an output (OUT), a single positive supply (V
CC
) and ground
(GND). All comparators are completely independent, shar-
ing only the power and ground pins. The circuit topology
consists of a differential input stage, a gain stage with
hysteresis and a complementary common-emitter output
stage. All of the internal signal paths utilize low voltage
swings for high speed at low power.
The input stage topology maximizes the input dynamic
range available without requiring the power, complex-
ity and die area of two complete input stages such as
are found in rail-to-rail input comparators. With a 2.7V
supply, the LT1720/LT1721 still have a respectable 1.6V
of input common mode range. The differential input volt-
age range is rail-to-rail, without the large input currents
found in competing devices. The input stage also features
phase reversal protection to prevent false outputs when
the inputs are driven below the –100mV common mode
voltage limit.
The internal hysteresis is implemented by positive, nonlin-
ear feedback around a second gain stage. Until this point,
the signal path has been entirely differential. The signal
path is then split into two drive signals for the upper and
lower output transistors. The output transistors are con-
nected common emitter for rail-to-rail output operation.
The Schottky clamps limit the output voltages at about
300mV from the rail, not quite the 50mV or 15mV of Linear
APPLICATIONS INFORMATION
Technologys rail-to-rail amplifiers and other products. But
the output of a comparator is digital, and this output stage
can drive TTL or CMOS directly. It can also drive ECL, as
described earlier, or analog loads as demonstrated in the
applications to follow.
The bias conditions and signal swings in the output stages
are designed to turn their respective output transistors off
faster than on. This nearly eliminates the surge of current
from V
CC
to ground that occurs at transitions, keeping
the power consumption low even with high output-toggle
frequencies.
The low surge current is what keeps the power consump-
tion low at high output-toggle frequencies. The frequency
dependence of the supply current is shown in the Typical
Performance Characteristics. Just 20pF of capacitive load
on the output more than triples the frequency dependent
rise. The slope of the no-load curve is just 32μA/MHz. With
a 5V supply, this current is the equivalent of charging and
discharging just 6.5pF. The slope of the 20pF load curve is
133μA/MHz, an addition of 101μA/MHz, or 20μA/MHz-V,
units that are equivalent to picoFarads.
The LT1720/LT1721 dynamic current can be estimated
by adding the external capacitive loading to an internal
equivalent capacitance of 5pF to 15pF, multiplied by the
toggle frequency and the supply voltage. Because the
capacitance of routing traces can easily approach these
values, the dynamic current is dominated by the load in
most circuits.
Figure 6. LT1720/LT1721 Block Diagram
+
+
+
+
+IN
–IN
A
V1
A
V2
NONLINEAR STAGE
OUT
GND
17201 F06
V
CC
+
3
+
3
LT1720/LT1721
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Speed Limits
The LT1720/LT1721 comparators are intended for high
speed applications, where it is important to understand a
few limitations. These limitations can roughly be divided
into three categories: input speed limits, output speed
limits, and internal speed limits.
There are no significant input speed limits except the shunt
capacitance of the input nodes. If the 2pF typical input
nodes are driven, the LT1720/LT1721 will respond.
The output speed is constrained by two mechanisms,
the fi rst of which is the slew currents available from the
output transistors. To maintain low power quiescent op-
eration, the LT1720/LT1721 output transistors are sized
to deliver 25mA to 45mA typical slew currents. This is
sufficient to drive small capacitive loads and logic gate
inputs at extremely high speeds. But the slew rate will
slow dramatically with heavy capacitive loads. Because
the propagation delay (t
PD
) definition ends at the time the
output voltage is halfway between the supplies, the fixed
slew current actually makes the LT1720/LT1721 faster at
3V than 5V with 20mV of input overdrive.
Another manifestation of this output speed limit is skew,
the difference between t
PDLH
and t
PDHL
. The slew currents
of the LT1720/LT1721 vary with the process variations of
the PNP and NPN transistors, for rising edges and falling
edges respectively. The typical 0.5ns skew can have either
polarity, rising edge or falling edge faster. Again, the skew
will increase dramatically with heavy capacitive loads.
The skews of comparators in a single package are corre-
lated, but not identical. Besides some random variability,
there is a small (100ps to 200ps) systematic skew due to
physical parasitics of the packages. For the LT1720 SO-8,
comparator A, whose output is adjacent to the V
CC
pin,
will have a relatively faster rising edge than comparator
B. Likewise, comparator B, by virtue of an output adjacent
to the ground pin will have a relatively faster falling edge.
Similar dependencies occur in the LT1721 S16, while the
systemic skews in the smaller MSOP and SSOP packages
are half again as small. Of course, if the capacitive loads on
the two comparators of a single package are not identical,
the differential timing will degrade further.
APPLICATIONS INFORMATION
The second output speed limit is the clamp turnaround.
The LT1720/LT1721 output is optimized for fast initial
response, with some loss of turnaround speed, limiting
the toggle frequency. The output transistors are idled in a
low power state once V
OH
or V
OL
is reached by detecting
the Schottky clamp action. It is only when the output has
slewed from the old voltage to the new voltage, and the
clamp circuitry has settled, that the idle state is reached
and the output is fully ready to transition again. This clamp
turnaround time is typically 8ns for each direction, resulting
in a maximum toggle frequency of 62.5MHz, or a 125MB
data rate. With higher frequencies, dropout and runt pulses
can occur. Increases in capacitive load will increase the time
needed for slewing due to the limited slew currents and
the maximum toggle frequency will decrease further. For
higher toggle frequency applications, refer to the LT1715,
whose output stage can toggle at 150MHz typical.
The internal speed limits manifest themselves as disper-
sion. All comparators have some degree of dispersion,
defined as a change in propagation delay versus input
overdrive. The propagation delay of the LT1720/LT1721
will vary with overdrive, from a typical of 4.5ns at 20mV
overdrive to 7ns at 5mV overdrive (typical). The LT1720/
LT1721’s primary source of dispersion is the hysteresis
stage. As a change of polarity arrives at the gain stage,
the positive feedback of the hysteresis stage subtracts
from the overdrive available. Only when enough time has
elapsed for a signal to propagate forward through the gain
stage, backwards through the hysteresis stage and forward
through the gain stage again, will the output stage receive
the same level of overdrive that it would have received in
the absence of hysteresis.
With 5mV of overdrive, the LT1720/LT1721 are faster with
a 5V supply than with a 3V supply, the opposite of what
is true with 20mV overdrive. This is due to the internal
speed limit, because the gain stage is faster at 5V than 3V
due primarily to the reduced junction capacitances with
higher reverse voltage bias.
In many applications, as shown in the following examples,
there is plenty of input overdrive. Even in applications
providing low levels of overdrive, the LT1720/LT1721
are fast enough that the absolute dispersion of 2.5ns
(= 7 – 4.5) is often small enough to ignore.
LT1720/LT1721
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The gain and hysteresis stage of the LT1720/LT1721 is
simple, short and high speed to help prevent parasitic
oscillations while adding minimum dispersion. This
internal “self-latch” can be usefully exploited in many
applications because it occurs early in the signal chain, in
a low power, fully differential stage. It is therefore highly
immune to disturbances from other parts of the circuit,
either in the same comparator, on the supply lines, or from
the other comparator(s) in the same package. Once a high
speed signal trips the hysteresis, the output will respond,
after a fixed propagation delay, without regard to these
external influences that can cause trouble in nonhysteretic
comparators.
±V
TRIP
Test Circuit
The input trip points are tested using the circuit shown in
the Test Circuits section that precedes this Applications
Information section. The test circuit uses a 1kHz triangle
wave to repeatedly trip the comparator being tested. The
LT1720/LT1721 output is used to trigger switched capaci-
tor sampling of the triangle wave, with a sampler for each
direction. Because the triangle wave is attenuated 1000:1
and fed to the LT1720/LT1721’s differential input, the
sampled voltages are therefore 1000 times the input trip
voltages. The hysteresis and offset are computed from
the trip points as shown.
Crystal Oscillators
A simple crystal oscillator using one comparator of an
LT1720/LT1721 is shown on the fi rst page of this data
sheet. The 2k-620Ω resistor pair set a bias point at the
comparators noninverting input. The 2k-1.8k-0.1μF path
sets the inverting input node at an appropriate DC aver-
age level based on the output. The crystal’s path provides
resonant positive feedback and stable oscillation occurs.
Although the LT1720/LT1721 will give the correct logic
output when one input is outside the common mode range,
additional delays may occur when it is so operated, open-
ing the possibility of spurious operating modes. Therefore,
the DC bias voltages at the inputs are set near the center
of the LT1720/LT1721’s common mode range and the
220Ω resistor attenuates the feedback to the noninvert-
ing input. The circuit will operate with any AT-cut crystal
from 1MHz to 10MHz over a 2.7V to 6V supply range.
APPLICATIONS INFORMATION
As the power is applied, the circuit remains off until the
LT1720/LT1721 bias circuits activate, at a typical V
CC
of
2V to 2.2V (25°C), at which point the desired frequency
output is generated.
The output duty cycle for this circuit is roughly 50%, but
it is affected by resistor tolerances and, to a lesser extent,
by comparator offsets and timings. If a 50% duty cycle is
required, the circuit of Figure 7 creates a pair of comple-
mentary outputs with a forced 50% duty cycle. Crystals are
narrow-band elements, so the feedback to the noninverting
input is a filtered analog version of the square wave output.
Changing the noninverting reference level can therefore
vary the duty cycle. C1 operates as in the previous example,
whereas C2 creates a complementary output by compar-
ing the same two nodes with the opposite input polarity.
A1 compares band-limited versions of the outputs and
biases C1’s negative input. C1’s only degree of freedom to
respond is variation of pulse width; hence the outputs are
forced to 50% duty cycle. Again, the circuit operates from
2.7V to 6V, and the skew between the edges of the two
outputs are shown in Figure 8. There is a slight duty cycle
dependence on comparator loading, so equal capacitive
and resistive loading should be used in critical applications.
This circuit works well because of the two matched delays
and rail-to-rail style outputs of the LT1720.
Figure 7. Crystal Oscillator with Complementary
Outputs and 50% Duty Cycle
+
+
+
C1
1/2 LT1720
C2
1/2 LT1720
A1
LT1636
V
CC
2.7V TO 6V
2k
620Ω
220Ω
1MHz TO 10MHz
CRYSTAL (AT-CUT)
100k
100k
17201 F07
1.8k
2k
1k
0.1μF
0.1μF
0.1μF
OUTPUT
OUTPUT
GROUND
CASE

LT1720IMS8#PBF

Mfr. #:
Manufacturer:
Analog Devices Inc.
Description:
Analog Comparators Dual 3V/5V Hi Speed Comparator
Lifecycle:
New from this manufacturer.
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