LTC6244
19
6244fb
Small Area Photodiode Amplifi ers
Small area photodiodes have very low capacitance, typically
under 10pF and some even below 1pF. Their low capaci-
tance makes them more approximate current sources to
higher frequencies than large area photodiodes. One of
the challenges of small area photodiode amplifi er design
is to maintain low input capacitance so that voltage noise
does not become an issue and current noise dominates. A
simple small area photodiode amplifi er using the LTC6244
is shown in Figure 7. The input capacitance of the ampli-
er consists of C
DM
and one C
CM
(because the +input is
Figure 8a: Using Both Op Amps for Higher Bandwidth. A1 Provides a Gain of 3 Within the Loop, Increasing the Gain Bandwidth
Product. This Bootstraps the C
DM
Accross A1’s Inputs, Reducing Amplifi er Input Capacitance. Inversion is Provided by A2, so that
the Photodiode Looks Into a Noninverting Input. Pin 5 was Selected Because it is in the Corner, Removing One Lead Capacitance
Figure 7. LTC6244 in a Normal TIA Confi guration
grounded), or about 6pF total. The small photodiode has
1.8pF, so the input capacitance of the amplifi er is dominating
the capacitance. The small feedback capacitor is an actual
component (AVX Accu-F series), but it is also in parallel
with the op amp lead, resistor and parasitic capacitances,
so the total real feedback capacitance is probably about
0.4pF. The reason this is important is that this sets the
compensation of the circuit and, with op amp gain band-
width, the circuit bandwidth. The circuit as shown has a
bandwidth of 350kHz, with an output noise of 120µV
RMS
measured over that bandwidth.
The circuit of Figure 8a makes some slight improvements.
Operation is still transimpedance mode, with R
F
setting
the gain to 1M. However, a noninverting input stage A1
with a gain of 3 has been inserted, followed by the usual
inverting stage performed by A2. Note what this achieves.
The amplifi er input capacitance is bootstrapped by the
feedback of R2:R1, eliminating the effect of A1’s input
C
DM
(3.5pF), and leaving only one C
CM
(2.1pF). The op
amp at Pins 5, 6 and 7 was chosen for the input amplifi er
to eliminate extra pin-to-pin capacitance on the (+) input.
The lead capacitance on the corner of an MSOP package
is only about 0.15pF. By using this noninverting confi gura-
tion, input capacitance is minimized.
APPLICATIONS INFORMATION
5V
V
OUT
= 1M • I
PD
BW = 350kHz
NOISE = 120µV
RMS
MEASURED ON A
350kHz BW
I
PD
R
F
1M
SMALL AREA
PHOTODIODE
VISHAY
TEMD1000
C
PD
= 1.8pF
C
F
0.1pF
–5V
–5V
6244 F07
+
1/2
LTC6244HV
V
OUT
5V
–5V
I
PD
R
F
1M
R3
1k
R2
1k
R4
6.98k
R1
499Ω
SMALL AREA
PHOTODIODE
VISHAY
TEMD1000
C
PD
= 1.8pF
0.07pF
(PARASITIC)
C2
150pF
C1
56pF
–5V
6244 F08a
+
A1 1/2
LTC6244HV
V
OUT
8
4
1
7
5
6
+
A2 1/2
LTC6244HV
2
3
V
OUT
= 1M • I
PD
BW = 1.6MHz
NOISE = 1.2mV
RMS
MEASURED ON A
2MHz BW
LTC6244
20
6244fb
Figure 8b: Output Noise Spectrum of the Circuit in Figure 8a.
Noise at 1MHz is 782nV/√Hz, Due Mostly to the Input Current
Noise Rising with Frequency
Total capacitance at the amplifi ers input is now one C
CM
(2.1pF) plus the photodiode capacitance C
PD
(1.8pF), or
about 4pF accounting for parasitics. The shunt impedance
at 1MHz, for example, is X
C
= 1/(2πfC) = 39.8k, and
therefore, the noise gain at 1MHz is NG = 1+Rf/X
C
= 26.
The input voltage noise of this amplifi er is about 15nV/√Hz,
after accounting for the effects of R1 through R3, the
noise of the second stage and the fact that voltage noise
does rise with frequency. Multiplying the noise gain by
the input voltage noise gives an output noise density due
to voltage noise of 26 • 15nV/√Hz = 390nV/√Hz. But the
noise spectral density plot of Figure 8b shows an output
noise of 782nV/√Hz at 1MHz. The extra output noise is
due to input current noise, multiplied by the feedback
impedance. So while the circuit of Figure 8a does increase
bandwidth, it does not offer a noise advantage. Note,
however, that the 1.2mV
RMS
of noise is now measured in
a 2MHz bandwidth, instead of over a 350kHz bandwidth
of the previous example.
A Low Noise Fully Differential Buffer/Amplifi er
In differential signal conditioning circuits, there is often a
need to monitor a differential source without loading or
adding appreciable noise to the circuit. In addition, add-
ing gain to low level signals over appreciable bandwidth
is extremely useful. A typical application for a low noise,
high impedance, differential amplifi er is in the baseband
circuit of an RFID (radio frequency identifi cation) receiver.
The baseband signal of a UHF RFID receiver is typically a
low level differential signal at the output of a demodulator
with differential output impedance in the range of 100 to
400. The bandwidth of this signal is 1MHz or less.
The circuit of Figure 9a uses an LTC6244 to make a low
noise fully differential amplifi er. The amplifi ers gain, input
impedance and –3dB bandwidth can be specifi ed indepen-
dently. Knowing the desired gain, input impedance and
–3dB bandwidth, R
G
, C
F
and C
IN
can be calculated from
the equations shown in Figure 9b. The common mode
gain of this amplifi er is equal to one (V
OUTCM
= V
INCM
)
and is independent of resistor matching. The component
values in the Figure 9a circuit implement a 970kHz, gain
= 5, differential amplifi er with 4k input impedance. The
output differential DC offset is typically less than 500µV.
The differential input referred noise voltage density is
shown in Figure 10. The total input referred noise in a
1MHz bandwidth is 16µV
RMS
.
APPLICATIONS INFORMATION
50k 1M
FREQUENCY (Hz)
6244 F08b
5M
OUTPUT NOISE (150nV/√Hz/DIV)
LTC6244
21
6244fb
A Low Noise AC Difference Amplifi er
In the signal conditioning of wideband sensors and trans-
ducers, a low noise amplifi er is often used to provide gain
for low level AC difference signals in the frequency range
of a few Hertz to hundreds of kilo-Hertz. In addition, the
amplifi er must reject common mode AC signals and its input
impedance should be higher than the differential source
impedance. Typical applications are piezoelectric sensors
used in sonar, sound and ultrasound systems and LVDT
(linear variable differential transformers) for displacement
measurements in process control and robotics.
The Figure 11a circuit is a low noise, single supply AC
difference amplifi er. The amplifi ers low frequency –3dB
bandwidth is set with resistor R5 and capacitor C3, while
the upper –3dB bandwidth is set with R2 and C1. The
input common mode DC voltage can vary from ground to
V
+
and the output DC voltage is equal to the V
REF
voltage.
The amplifi ers gain is the ratio of resistors R2 to R1 (R4
= R2 and R3 = R1). The component values in the circuit
of Figure 11a implement an 800Hz to 160kHz AC ampli-
er with a gain equal to 10 and 12nV/√Hz input referred
voltage noise density shown in Figure 11b. The total input
referred wideband noise is 4.5µV
RMS
, in the bandwidth of
500Hz to 200kHz.
Input Impedance = 2 • R
IN
Gain =
V
OUT
+
–V
OUT
V
IN
+
–V
IN
=
R
G
R
IN
Maximum Gain =
5MHz
f
3dB
C
F
=
1
4398 f
3dB
•Gain+ 2
()
C
IN
=
Gain + 2
8.977 Gain R
IN
•f
3dB
f
3dB
=
1
4000 π
2
•R
G
•C
F
•C
IN
Figure 9b. Design Equations for Figure 9a Circuit
Figure 10. Differential Input Referred Noise
Figure 9a. Low Noise Fully Differential Buffer/Amplifi er
(f
–3dB
= 970kHz, Gain = 5, R
IN
= 4k)
APPLICATIONS INFORMATION
2k2k
V
IN
+
R
G
10k
R
IN
2k
R
IN
2k
C
IN
82pF
C
IN
82pF
C
F
33pF
C
F
33pF
+
1/2
LTC6244
V
OUT
+
+
1/2
LTC6244
V
OUT
2k
6244 F09a
V
+
V
2k
R
G
10k
V
IN
32
28
24
20
16
12
8
10k 100k
FREQUENCY (Hz)
6244 F10
1M
4
INPUT REFERRED NOISE (nV/√Hz)
f
–3dB
= 970kHz
GAIN = 5
R
IN
= 4k

LTC6244HVCDD#PBF

Mfr. #:
Manufacturer:
Analog Devices Inc.
Description:
Precision Amplifiers 2x 50MHz, L N, R2R, CMOS Op Amp
Lifecycle:
New from this manufacturer.
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