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ADA4530-1ARZ-R7 数据表(PDF) 48 Page - Analog Devices

部件名 ADA4530-1ARZ-R7
功能描述  Femtoampere Input Bias Current Electrometer Amplifier
PDF  51 Pages
Scroll/Zoom Zoom In 100%  Zoom Out
制造商  AD [Analog Devices]
网页  http://www.analog.com
标志 AD - Analog Devices

ADA4530-1ARZ-R7 数据表(HTML) 48 Page - Analog Devices

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Data Sheet
ADA4530-1
Rev. A | Page 47 of 50
The total RTI error over the entire temperature range is less
than 150 fA, which is equal to 300 ppm of the 500 pA full-scale
range. Note that the extraordinarily low input bias current of
the ADA4530-1 is not a significant contributor to the total error
over temperature. The interaction of the offset voltage with the
shunt resistance of the photodiode is the most significant error
source.
This circuit was constructed as described with a 10 GΩ feed-
back resistor (Ohmite RX-1M1008JE). The dc error performance
was measured over the 25°C to 60°C temperature range (see
Figure 128). The error increases rapidly with temperature as the
shunt resistance changes the noise gain exponentially. The total
RTI error ranges from +2 fA to −10 fA, considerably lower than
the worst case error budget, as expected.
20
–120
–100
–80
–60
–40
–20
0
2
–12
–10
–8
–6
–4
–2
0
070
60
50
40
30
20
10
TEMPERATURE (°C)
VSY = 10V
VCM = VSY/2
Figure 128. DC Error vs. Temperature
The ac performance of the circuit was also measured. The
circuit was initially constructed without a physical feedback
capacitor as a baseline. The transimpedance gain vs. frequency
is shown in Figure 129. The 30% frequency peaking seen in the
frequency response (red curve) indicates that the feedback loop
is marginally compensated with parasitic capacitance.
A physical capacitor was added to improve the loop compensa-
tion. This capacitor is a 300 fF C0G ceramic in a Size 0805,
surface-mount package (AVX UQCFVA0R3BAT2A\500). C0G
ceramic capacitors are good candidates for electrometer circuits
because they have adequate insulation resistance and dielectric
absorption performance. These low valued capacitors are designed
for RF use and are readily available. The 300 fF capacitor elimi-
nates the frequency peaking completely (blue curve) but it
reduces the −3 dB bandwidth from 390 Hz to 50 Hz.
0.1
1
10
0.1
1
10
100
1k
10k
100k
FREQUENCY (Hz)
VSY = 10V
VCM = VSY/2
TA = 25°C
CF = 0fF
CF = 300fF
Figure 129. Transimpedance Gain vs. Frequency
The stability improvement can be seen in the time domain as
well. The circuits step response to a 10 pA photocurrent is
shown in Figure 130. The uncompensated circuit (red curve)
shows considerable (20%) overshoot. The compensated circuit
(blue curve) is overdamped.
40
–140
–120
–100
–80
–60
–40
–20
0
20
4
–14
–12
–10
–8
–6
–4
–2
0
2
040
35
30
25
20
15
10
5
TIME (ms)
VSY = 10V
TA = 25°C
IPD = 10pA
CF = 0fF
CF = 300fF
Figure 130. 10 pA Step Response
A noise budget is constructed based on the Noise Analysis
section. The RTO noise budget is separated into noise sources
integrated with a low bandwidth (see Table 14) and those
integrated with a high bandwidth (see Table 15).
The low frequency noise contributors include the feedback
resistance, the shunt resistance and the amplifier current noise.
Each of these sources has a −3 dB bandwidth equal to the signal
bandwidth (50 Hz); this is equivalent to a noise bandwidth of
79 Hz. The most significant noise source is the photodiode
shunt resistance by a large margin. The second most significant
source is the feedback resistor. The amplifier current noise is so
low that it can be ignored.



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