LTC6405
16
6405fb
For more information www.linear.com/6405
applications inForMation
In general, the degree of feedback pair mismatch is a
source of common mode to differential conversion of both
signals and noise. Using 1% resistors or better will mitigate
most problems, and will provide about 34dB worst case of
common mode rejection. Using 0.1% resistors will provide
about 54dB of common mode rejection. A low impedance
ground plane should be used as a reference for both the
input signal source and the V
OCM
pin. Bypassing the V
OCM
with a high quality 0.1µF ceramic capacitor to this ground
plane will further help prevent common mode signals from
being converted to differential signals.
There may be concern on how feedback factor mismatch
affects distortion. Feedback factor mismatch from using
1% resistors or better, has a negligible effect on distortion.
However, in single supply level shifting applications where
there is a voltage difference between the input common
mode voltage and the output common mode voltage,
resistor mismatch can make the apparent voltage offset
of the amplifier appear worse than specified.
The apparent input referred offset induced by feedback
factor mismatch is derived from the above equation:
V
OSDIFF(APPARENT)
≈ (V
ICM
– V
OCM
) • ∆b
Using the LTC6405 in a single supply application on a
single
5V supply with 1% resistors, and the input common
mode grounded, with the V
OCM
pin biased at 2.5V, the
worst case DC offset can induce 25mV of apparent offset
voltage. With 0.1% resistors, the worst case apparent
offset reduces to 2.5mV.
Input Impedance and Loading Effects
The input impedance looking into the V
INP
or V
INM
input
of Figure 1 depends on whether or not the sources V
INP
and V
INM
are fully differential or not. For balanced input
sources (V
INP
= –V
INM
), the input impedance seen at either
input is simply:
R
INP
= R
INM
= R
I
For single ended inputs, because of the signal imbalance
at the input, the input impedance actually increases over
the balanced differential case. The input impedance looking
into either input is:
R
INP
= R
INM
=
R
I
1
1
2
R
F
R
I
+ R
F
Input signal sources with non-zero output impedances can
also cause feedback imbalance between the pair of feedback
networks. For the best performance, it is recommended
that the input source output impedance be compensated
for. If input impedance matching is required by the source,
a termination resistor R1 should be chosen (see Figure 4):
R1=
R
INM
R
S
R
INM
R
S
According to Figure 4, the input impedance looking into
Figure 4. Optimal Compensation for Signal Source Impedance
V
S
+
+
R
F
R
F
R
I
R
INM
R
S
R
I
R2 = R
S
|| R1
R1 CHOSEN SO THAT R1 || R
INM
= R
S
R2 CHOSEN TO BALANCE R1 || R
S
R1
6405 F04
the differential amp (R
INM
) reflects the single ended source
case, thus:
R
INM
=
R
I
1
1
2
R
F
R
I
+ R
F
R2 is chosen to equal R1 || R
S
:
R2 =
R1 R
S
R1+ R
S
LTC6405
17
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+
R
F
V
–OUT
V
+OUT
V
VOCM
V
OCM
6405 F05
R
F
R
I
R
I
+
V
INP
+
V
CM
+
V
INM
V
–IN
V
+IN
applications inForMation
Input Common Mode Voltage Range
The LTC6405’s input common mode voltage (V
ICM
) is
defined as the average of the two input voltages, V
+IN
, and
V
IN
. At the inputs to the actual op amp, the range extends
from V
to V
+
. This makes it easy to interface to a wide
range of common mode signals, from ground referenced to
V
CC
referenced signals. Moreover, due to external resistive
divider action of the gain and feedback resistors, the effective
range of signals that can be processed is even wider. The
input common mode range at the op amp inputs depends
on the circuit configuration (gain), V
OCM
and V
CM
(refer to
Figure 5). For fully differential input applications, where
V
INP
= –V
INM
, the common mode input is approximately:
V
ICM
=
V
+IN
+ V
IN
2
V
OCM
R
I
R
I
+ R
F
+
V
CM
R
F
R
F
+ R
I
Figure 5. Circuit for Common Mode Range
Manipulating the Rail-to-Rail Input Stage with V
TIP
To achieve rail-to-rail input operation, the LTC6405 features
an NPN input stage in parallel with a PNP input stage. When
the input common mode voltage is near V
+
, the NPNs are
active while the PNPs are off. When the input common
mode is near V
, the PNPs are active while the NPNs are
off. At some range in the middle, both input stages are
active. This ‘hand-off’ operation happens automatically.
In the QFN package, a special pin, V
TIP
, is made available
that can be used to manipulate thehand-off’ operation
between the NPN and PNP input stages. By default, the
V
TIP
pin is internally biased by an internal resistive divider
between the supplies, developing a default 2.8V voltage
with a 5V supply. If desired, V
TIP
can be over-driven by
an external voltage (the Thevenin equivalent resistance is
approximately 17k).
If V
TIP
is pulled closer to V
, the range over which the NPN
input pair remains active is increased, while the range over
which the PNP input pair is active is reduced. In applica-
tions
where the input common mode does not come close
to V
, this mode can be used to further improve linearity
beyond the specified performance (see Figure 6).
If V
TIP
is pulled closer to V
+
, the range over which the PNP
input pair remains active is increased, while the range over
which the NPN input pair is active is reduced. In applica-
tions where the input common mode does not come close
to V
+
, this mode can be used to further improve linearity
beyond the specified performance.
With single ended inputs, there is an input signal compo-
nent to the input common mode voltage. Applying only
V
INP
(setting V
INM
to zero), the input common voltage is
approximately:
V
ICM
=
V
+IN
+ V
IN
2
V
OCM
R
I
R
I
+ R
F
+
V
CM
R
F
R
F
+ R
I
+
V
INP
2
R
F
R
F
+ R
I
Use the equations above to check that the V
ICM
at the op
amp inputs is within range (V
to V
+
).
Figure 6. Manipulating V
TIP
to Improve Harmonic Distortion
HD2
V
TIP
= OPEN
HD3
V
TIP
= OPEN
FREQUENCY (MHz)
6405 F06
DISTORTION (dBc)
V
S
= 5V
V
OCM
= V
ICM
= 2.5V
R
LOAD
= 800
R
I
= R
F
= 499
V
OUTDIFF
= 2V
P-P
SINGLE-ENDED INPUT
QFN PACKAGE
–30
–40
–50
–60
–70
–80
–90
–110
–100
1 10010
HD3
V
TIP
= 1V
HD2
V
TIP
= 1V
LTC6405
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6405fb
For more information www.linear.com/6405
Output Common Mode Voltage Range
The output common mode voltage is defined as the aver-
age of the two outputs:
V
OUTCM
= V
OCM
=
V
+OUT
+
V
OUT
2
The V
OCM
pin sets this average by an internal common
mode feedback loop which internally forces V
OUTCM
= V
OCM
.
The output common mode range extends from 0.5V above
V
to typically 1V below V
+
. The V
OCM
voltage is internally
set by a resistive divider between the supplies, developing
a default voltage potential of 2.5V with a 5V supply.
In single supply applications, where the LTC6405 is used
to interface to an ADC, the optimal common mode input
range to the ADC is often determined by the ADC’s refer-
ence. If the ADC makes a reference available for setting the
input common mode voltage, it can be directly tied to the
V
OCM
pin (as long as it is able to drive the 19Thevenin
equivalent input impedance presented by the V
OCM
pin).
The V
OCM
pin should be bypassed with a high quality
ceramic bypass capacitor of at least 0.01µF to filter any
common mode noise rather than being converted to dif-
ferential noise and to prevent common mode signals on
this pin from being inadvertently converted to differential
signals by impedance mismatches both externally and
internally to the IC.
applications inForMation
Output Filter Considerations and Use
Filtering at the output of the LTC6405 is often desired to
provide
anti-aliasing or to improve signal to noise ratio.
To simplify this filtering, the LTC6405 in the QFN package
includes an additional pair of differential outputs (+OUTF
andOUTF) which incorporate an internal lowpass RC
network with a –3dB bandwidth of 850MHz (Figure 7).
These pins each have an output resistance of 50Ω (toler-
ance ±12%). Internal capacitances are 1.25pF (tolerance
±15%) to V
on each filtered output, plus an additional
1.25pF (tolerance ±15%) capacitor connected between the
two filtered outputs. This resistor/capacitor combination
creates filtered outputs that look like a series 50Ω resistor
with a 3.75pF capacitor shunting each filtered output to
AC ground, providing a –3dB bandwidth of 850MHz, and
a noise bandwidth of 1335MHz. The filter cutoff frequency
is easily modified with just a few external components. To
increase the cutoff frequency, simply add two equal value
resistors, one between +OUT and +OUTF and the other
betweenOUT andOUTF (Figure 8). These resistors, in
parallel with the internal 50Ω resistors, lower the overall
resistance and therefore increase filter bandwidth. For
example, to double the filter bandwidth, add two external
50Ω resistors to lower the series filter resistance to 25Ω.
The 3.75pF
of capacitance remains unchanged, so filter
bandwidth doubles. Keep in mind, the series resistance
also serves to decouple the outputs from load capaci-
Figure 7. LTC6405 Internal Filter Topology
+
7
+OUT
8
+OUTF
14
–OUT
13
–OUTF
+OUTF
–OUTF
1.25pF
1.25pF
50Ω
50Ω
1.25pF
12
V
9
V
V
V
6405 F07
LTC6405
FILTERED OUTPUT
Figure 8. LTC6405 Filter Topology Modified for 2x Filter
Bandwidth (Tw o External Resistors)
+
7 8
14 13
12
V
9
V
V
V
6405 F08
LTC6405
FILTERED OUTPUT
(1.7GHz)
+OUTF
OUTF
49.9Ω
49.9Ω
1.25pF
1.25pF
50Ω
50Ω
1.25pF
+OUT +OUTF
OUT OUTF

LTC6405CMS8E#PBF

Mfr. #:
Manufacturer:
Analog Devices Inc.
Description:
High Speed Operational Amplifiers 2.7GHz, 5V Low Noise, Rail-to-Rail Input Differential Amp/Driver
Lifecycle:
New from this manufacturer.
Delivery:
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