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ADA4895-1ARZ-R7 数据表(PDF) 21 Page - Analog Devices |
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ADA4895-1ARZ-R7 数据表(HTML) 21 Page - Analog Devices |
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21 / 24 page ![]() Data Sheet ADA4895-1/ADA4895-2 Rev. B | Page 21 of 24 WIDEBAND PHOTOMULTIPLIER PREAMPLIFIER A decompensated amplifier can provide significantly greater speed in transimpedance applications than a unity-gain stable amplifier. The speed increases by the square root of the ratio of the bandwidth of the two amplifiers; that is, a 1 GHz GBP amplifier is 10 times faster than a 10 MHz amplifier in the same trans- impedance application if all other parameters are kept constant. Additionally, the input voltage noise normally dominates the total output rms noise because it is multiplied by the capacitive noise gain network. F D F M S C C C C C In the case of the ADA4895-1/ADA4895-2, the input noise is low, but the capacitive noise gain network must be kept greater than 10 for stability reasons. One disadvantage of using the ADA4895-1/ADA4895-2 in transimpedance applications is that the input current and input current noise can create large offsets and output voltage noise when coupled with an excessively high feedback resistance. Despite these two issues, the ADA4895-1/ADA4895-2 noise and gain bandwidth can provide a significant increase in performance within certain transimpedance ranges. Figure 55 shows an I/V converter with an electrical model of a photomultiplier. – + VOUT VB CF +CS CD CM CM RF RSH CS IPHOTO CF RF Figure 55. Wideband Photomultiplier Preamplifier The basic transfer function is F F F PHOTO OUT R sC R I V 1 where IPHOTO is the output current of the photomultiplier, and the parallel combination of RF and CF sets the signal bandwidth. The stable bandwidth attainable with this preamplifier is a function of RF, the gain bandwidth product of the amplifier, and the total capacitance at the summing junction of the amplifier, including CS and the amplifier input capacitance. RF and the total capacitance produce a pole in the loop trans- mission of the amplifier that can result in peaking and instability. Adding CF creates a zero in the loop transmission that compensates for the pole effect and reduces the signal bandwidth. It can be shown that the signal bandwidth resulting in a 45° phase margin (f(45)) is defined as follows: S F 45 C R GBP f π 2 where: GBP is the gain bandwidth product. RF is the feedback resistance. CS is the total capacitance at the amplifier summing junction (amplifier + photomultiplier + board parasitics). The value of CF that produces f(45) is GBP R C C F S F π 2 The frequency response in this case shows approximately 2 dB of peaking and 15% overshoot. Doubling CF and reducing the bandwidth by half results in a flat frequency response with approximately 5% transient overshoot. The output noise over frequency for the preamplifier is shown in Figure 56. FREQUENCY (Hz) RF NOISE f1 NOISE DUE TO AMPLIFIER ven f2 1 2π RF f1 = f2 = 1 2πRFCF f3 = GBP ven (CS + CM + CF + CD)/CF f3 (CS + CM + CF + CD) (CS + CM + CF + CD)/CF Figure 56. Photomultiplier Voltage Noise Contributions Table 12. RMS Noise Contributions of Photomultiplier Preamplifier Contributor Expression RF 57 1 4 . f R kT 2 F Amplifier ven 57 . 1 3 F D F M S f C C C C C ven Amplifier ien 57 1. f R ien 2 F |
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