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ADA4530-1ARZ-R7 数据表(PDF) 47 Page - Analog Devices |
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ADA4530-1ARZ-R7 数据表(HTML) 47 Page - Analog Devices |
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47 / 52 page ![]() Data Sheet ADA4530-1 PHOTODIODE INTERFACE analog.com Rev. C | 47 of 52 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 feedback 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. 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, sur- face-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 eliminates the frequency peaking completely (blue curve) but it reduces the −3 dB bandwidth from 390 Hz to 50 Hz. 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 consid- erable (20%) overshoot. The compensated circuit (blue curve) is overdamped. 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 resist- ance, 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. Table 14. Low Frequency Noise Budget Error Source 25°C 45°C 60°C VNRF 12.8 µV/√Hz 13.2 µV/√Hz 13.5 µV/√Hz RSHUNT 5 GΩ 1.25 GΩ 442 MΩ |
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