LTC6362
13
6362fa
The LTC6362’s input referred voltage noise contributes the
equivalent noise of a 920Ω resistor. When the feedback
network is comprised of resistors whose values are larger
than this, the output noise is resistor noise and amplifier
current noise dominant. For feedback networks consisting
of resistors with values smaller than 920Ω, the output
noise is voltage noise dominant.
Lower resistor values always result in lower noise at the
penalty of increased distortion due to increased loading of
the feedback network on the output. Higher resistor values
will result in higher output noise, but typically improved
distortion due to less loading on the output. For this rea-
son, when LTC6362 is configured in a differential gain of
1, using feedback resistors of at least 1k is recommended.
GBW vs f
–3dB
Gain-bandwidth product (GBW) and –3dB frequency
(f
–3dB
) have been specified in the Electrical Characteristics
table as two different metrics for the speed of the LTC6362.
GBW is obtained by measuring the open-loop gain of the
amplifier at a specific frequency (f
TEST
), then calculating
gain f
TEST
. GBW is a parameter that depends only on the
internal design and compensation of the amplifier and is
a suitable metric to specify the inherent speed capability
of the amplifier.
f
–3dB
, on the other hand, is a parameter of more practical
interest in different applications and is by definition the
frequency at which the closed-loop gain is 3dB lower than
its low frequency value. The value of f
–3dB
depends on the
APPLICATIONS INFORMATION
Figure 4. Simplified Noise Model
+
e
no
2
R
F
e
nRI
2
R
F
R
I
R
I
e
nRF
2
e
nRI
2
e
ni
2
e
nRF
2
i
n+
2
i
n–
2
6362 F04
speed of the amplifier as well as the feedback factor. Since
the LTC6362 is designed to be stable in a differential signal
gain of 1 (where R
I
= R
F
or β = 1/2), the maximum f
–3dB
is obtained and measured in this gain setting, as reported
in the Electrical Characteristics table.
In most amplifiers, the open-loop gain response exhibits a
conventional single-pole roll-off for most of the frequencies
before the unity-gain crossover frequency, and the GBW and
unity-gain frequency are close to each other. However, the
LTC6362 is intentionally compensated in such a way that
its GBW is significantly larger than its f
–3dB
. This means
that at lower frequencies where the amplifier inputs gen-
erally operate, the amplifiers gain and thus the feedback
loop gain is larger. This has the important advantage of
further linearizing the amplifier and improving distortion
at those frequencies.
Feedback Capacitors
In cases where the LTC6362 is connected such that the
combination of parasitic capacitances (device + PCB) at the
inverting input forms a pole whose frequency lies within
the closed-loop bandwidth of the amplifier, a capacitor
(C
F
) can be added in parallel with the feedback resistor
(R
F
) to cancel the degradation on stability. C
F
should be
chosen such that it generates a zero at a frequency close
to the frequency of the pole.
In general, a larger value for C
F
reduces the peaking (over-
shoot) of the amplifier in both frequency and time domains,
but also decreases the closed-loop bandwidth (f
–3dB
).
Board Layout and Bypass Capacitors
For single supply applications, it is recommended that
high quality 0.1µF ceramic bypass capacitors be placed
directly between the V
+
and the V
pin with short con-
nections. The V
pins (including the exposed pad in the
DD8 package) should be tied directly to a low impedance
ground plane with minimal routing. For dual (split) power
supplies, it is recommended that additional high quality
0.1µF ceramic capacitors be used to bypass V
+
to ground
and V
to ground, again with minimal routing. Small
geometry (e.g., 0603) surface mount ceramic capacitors
have a much higher self-resonant frequency than leaded
capacitors, and perform best with LTC6362.
LTC6362
14
6362fa
APPLICATIONS INFORMATION
To prevent degradation in stability response, it is highly
recommended that any stray capacitance at the input pins,
+IN and –IN, be kept to an absolute minimum by keeping
printed circuit connections as short as possible.
At the output, always keep in mind the differential nature of
the LTC6362, because it is critical that the load impedances
seen by both outputs (stray or intended), be as balanced
and symmetric as possible. This will help preserve the
balanced operation of the LTC6362 that minimizes the
generation of even-order harmonics and maximizes the
rejection of common mode signals and noise.
The V
OCM
pin should be bypassed to the ground plane with
a high quality 0.1µF ceramic capacitor. This will prevent
common mode signals and noise on this pin from being
inadvertently converted to differential signals and noise
by impedance mismatches both externally and internally
to the IC.
Interfacing to ADCs
When driving an ADC, an additional passive filter should be
used between the outputs of the LTC6362 and the inputs
of the ADC. Depending on the application, a single-pole
RC filter will often be sufficient. The sampling process
of ADCs creates a charge transient that is caused by the
switching in of the ADC sampling capacitor. This mo-
mentarily “shorts” the output of the amplifier as charge
is transferred between amplifier and sampling capacitor.
The amplifier must recover and settle from this load
transient before the acquisition period has ended, for a
valid representation of the input signal. The RC network
between the outputs of the driver and the inputs of the
ADC decouples the sampling transient of the ADC (see
Figure 5). The capacitance serves to provide the bulk
of the charge during the sampling process, while the
two resistors at the outputs of the LTC6362 are used to
dampen and attenuate any charge injected by the ADC.
The RC filter gives the additional benefit of band limiting
broadband output noise.
The selection of an appropriate filter depends on the specific
ADC, however the following procedure is suggested for
choosing filter component values. Begin by selecting an
appropriate RC time constant for the input signal. Gener-
ally, longer time constants improve SNR at the expense of
settling time. Output transient settling to 18-bit accuracy
will typically require over twelve RC time constants. To
select the resistor value, remember the resistors in the
decoupling network should be at least 10Ω. Keep in mind
that these resistors also serve to decouple the LTC6362
outputs from load capacitance. Too large of a resistor will
leave insufficient settling time. Too small of a resistor will
not properly dampen the load transient of the sampling
process, prolonging the time required for settling. For
lowest distortion, choose capacitors with low dielectric
absorption (such as a C0G multilayer ceramic capacitor). In
general, large capacitor values attenuate the fixed nonlinear
charge kickback, however very large capacitor values will
detrimentally load the driver at the desired input frequency
and thus cause driver distortion. Smaller input swings will
in general allow for larger filter capacitor values due to
decreased loading demands on the driver. This property
however may be limited by the particular input amplitude
dependence of differential nonlinear charge kickback for
the specific ADC used.
In some applications, placing series resistors at the inputs
of the ADC may further improve distortion performance.
These series resistors function with the ADC sampling
capacitor to filter potential ground bounce or other high
speed sampling disturbances. Additionally the resistors
limit the rise time of residual filter glitches that manage to
propagate to the driver outputs. Restricting possible glitch
propagation rise time to within the small signal bandwidth
of the driver enables less disturbed output settling.
For the specific application of LTC6362 driving the
LTC2379-18 SAR ADC in a gain of A
V
= –1 configuration,
the recommended component values of the RC filter for
varying filter bandwidths are provided in Figure 5. These
component values are chosen for optimal distortion per-
formance. Broadband output noise will vary with filter
bandwidth.
LTC6362
15
6362fa
APPLICATIONS INFORMATION
+
8 567
1 432
V
+
V
+
LTC6362
340k
340k
V
OCM
V
V
+IN
V
IN
5V
R
FILT
C
CM
–IN +OUTV
+
V
OCM
–OUTV
SHDN
1k
R
FILT
R
S
R
S
5V
C
CM
6362 F05
1k
1k1k
0.1µF
0.1µF
C
DIFF
A
IN
+
V
REF
V
DD
5V
LTC2379-18
SAR ADC
2.5V
GND
A
IN
FILTER BW
(Hz)
110k
380k
1.1M
3.0M
10M
29M
R
FILT
(Ω)
125
35.7
100
175
75
100
C
CM
(pF)
3900
3900
470
100
68
18
C
DIFF
(pF)
3900
3900
470
100
68
18
R
S
(Ω)
0
0
0
0
0
0
Figure 5. Recommended Interface Solutions for Driving the LTC2379-18 SAR ADC
TYPICAL APPLICATIONS
Single-Ended-to-Differential Conversion of a 20V
P-P
Ground-Referenced Input with Gain of A
V
= –0.4 to Drive an ADC
+
+
5V
3.9nF
3.9nF
3.9nF
A
IN
+
V
REF
V
DD
5V
LTC2379-18
SAR ADC
2.5V
GND
A
IN
6362 TA02
35.7Ω
35.7Ω
LTC6362
V
OCM
0.1µF
V
IN
2k
10V
–10V
V
IN
2k 806Ω
806Ω
SHDN
4.5V
4.5V
0.5V
0.5V
V
–OUT
V
+OUT

LTC6362HMS8#PBF

Mfr. #:
Manufacturer:
Analog Devices Inc.
Description:
Precision Amplifiers Low Power Differential OpAmp/ADC Driver
Lifecycle:
New from this manufacturer.
Delivery:
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