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ADA4530-1ARZ-R7 数据表(PDF) 46 Page - Analog Devices |
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ADA4530-1ARZ-R7 数据表(HTML) 46 Page - Analog Devices |
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46 / 52 page ![]() Data Sheet ADA4530-1 PHOTODIODE INTERFACE analog.com Rev. C | 46 of 52 Figure 127. Photodiode TIA RTO Noise Spectral Density Table 12. Photodiode Interface Noise Sources Noise Source RTO Noise Noise Bandwidth RF √(4kTRF) π/2 × f2 Photodiode (RF/RSHUNT)√(4kTRSHUNT) π/2 × f2 IN− Amplifier RF × IN− π/2 × f2 VN Amplifier VN × noise gain π/2 × f3 DESIGN RECOMMENDATIONS The design goal for a large area photodiode TIA circuit is usually to maximize signal-to-noise ratio (SNR) and minimize dc errors. Increasing the feedback resistor size accomplishes both goals. The signal gain increases directly with RF, whereas the noise increases in a square root fashion. High gains also make the output signal large relative to output voltage errors (such as VOS). The upper limit for RF is typically determined by one of the follow- ing: ► Amplifier output swing. The maximum photocurrent multiplied by RF must be less than amplifier swing limitations. ► Signal bandwidth (or settling time). Signal bandwidth is depend- ent on RF × CF. Achieving high signal bandwidths with large feedback resistors can require vanishingly small feedback capac- itors to implement. The ultimate limitation is due to the parasitic feedback capacitance from the fringing electric fields in the circuit. Parasitic capacitances in the 50 fF to 100 fF range are possible. For example, a 100 fF parasitic capacitance limits the signal bandwidth of a 100 GΩ TIA to 16 Hz. ► The thermal noise of the photodiode (RSHUNT). When RF is significantly larger than RSHUNT, the total noise is dominated by the photodiode and the SNR stops improving. ► The current noise of the amplifier. When the current noise of the amplifier is larger than the noise of RF, the SNR stops improving. The photodiode noise is higher than the amplifier current noise in nearly all practical photodiodes. ► The low frequency noise gain due to RSHUNT. When RF is larger than RSHUNT, the noise gain multiplies VOS and TCVOS errors and the signal to error ratio stops improving. The signal bandwidth increases as the feedback capacitance (CF) decreases. The lower limit for CF is typically limited by one of the following: ► Parasitic feedback capacitances limit the minimum value of CF to 50 fF to 100 fF. ► Available component values. Physical components can be found in surface mount packages for values from 0.1 pF to 1 pF in 100 fF increments. ► Feedback loop stability. CF must be large enough to recover enough phase shift prior to the loop crossover for stable opera- tion. This capacitance value can be a significant consideration for smaller values of RF. Large values (>1 GΩ) tend to be self compensating through the parasitic feedback capacitance. ► High frequency noise gain. The high frequency noise gain is set by the ratio of CSHUNT to CF. For very large noise gains, it is possible for the amplifier voltage noise to be greater than the feedback resistor noise. DESIGN EXAMPLE In this section, an example TIA circuit is designed using a photo- metry grade photodiode (Hamamatsu S1226-18BQ). This medium area (1.2 mm2) silicon photodiode is responsive in the ultraviolet (UV) through visible frequency range. The minimum shunt resist- ance (RSHUNT) is specified at 5 GΩ at 25°C. The shunt capacitance (CSHUNT) is specified at 35 pF. The quartz window limits the maxi- mum operating temperature to 60°C. Based on the specified minimum shunt resistance and the recom- mendations in the Design Recommendations section, a value of 10 GΩ is chosen for RF. This example circuit is powered from ±5 V with the input common-mode voltage set at 0 V, which allows a maximum photocurrent of approximately 500 pA. An error budget is constructed based on the DC Error Analysis section (see Table 13). The amplifier offset voltage applies the maximum temperature drift limit to the maximum room temperature offset limit. The photo diode shunt resistance limit is reduced by half for every 10°C. Table 13. Photodiode Interface DC Error Budget Error Source 25°C 45°C 60°C VOS 40 µV 40 µV + 10 µV 40 µV + 18 µV RSHUNT 5 GΩ 1.25 GΩ 442 MΩ Noise Gain 3 9 23 VOS Error RTO 120 µV 450 µV 1.3 mV IB 20 fA 20 fA 20 fA IB Error RTO 200 µV 200 µV 200 µV Total Error RTO 320 µV 650 µV 1.5 mV Total Error RTI 32 fA 65 fA 150 fA 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. The low input bias current of the ADA4530-1 is not a significant contributor to the total error over temperature. The interaction of |
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