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LT6235IGN データシート(PDF) 24 Page - Linear Technology |
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LT6235IGN データシート(HTML) 24 Page - Linear Technology |
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24 / 24 page ![]() LT6233/LT6233-10/ LT6234/LT6235 24 623345f Linear Technology Corporation 1630 McCarthy Blvd., Milpitas, CA 95035-7417 (408) 432-1900 q FAX: (408) 434-0507 q www.linear.com © LINEAR TECHNOLOGY CORPORATION 2003 LT/TP 1003 1K • PRINTED IN USA RELATED PARTS PART NUMBER DESCRIPTION COMMENTS LT1028 Single, Ultra Low Noise 50MHz Op Amp 0.85nV/ √Hz LT1677 Single, Low Noise Rail-to-Rail Amplifier 3V Operation, 2.5mA, 4.5nV/ √Hz, 60µV Max VOS LT1806/LT1807 Single/Dual, Low Noise 325MHz Rail-to-Rail Amplifier 2.5V Operation, 550 µV Max VOS, 3.5nV/√Hz LT6200/LT6201 Single/Dual, Low Noise 165MHz 0.95nV √Hz, Rail-to-Rail Input and Output LT6202/LT6203/LT6204 Single/Dual/Quad, Low Noise, Rail-to-Rail Amplifier 1.9nV/ √Hz, 3mA Max, 100MHz Gain Bandwidth Photodiode Amplifier Time Domain Response Low Power Avalanche Photodiode Transimpedance Amplifier IS = 1.2mA 100ns/DIV 623345 TA02b + – R1 10k R2 10k C2 0.1 µF 5V –5V ENABLE LT6233 ≈ 200V BIAS ADVANCED PHOTONIX 012-70-62-541 WWW.ADVANCEDPHOTONIX.COM OUTPUT OFFSET = 500 µV TYPICAL BANDWIDTH = 7.8MHz OUTPUT NOISE = 1mVP–P (20MHz MEASUREMENT BW) 623345 TA02a C1 2.7pF TYPICAL APPLICATIO S The LT6233 is applied as a transimpedance amplifier with an I-to-V conversion gain of 10k Ω set by R1. The LT6233 is ideally suited to this application because of its low input offset voltage and current, and its low noise. This is be- cause the 10k resistor has an inherent thermal noise of 13nV/ √Hz or 1.3pA/√Hz at room temperature, while the LT6233 contributes only 2nV and 0.8pA / √Hz. So, with respect to both voltage and current noises, the LT6233 is actually quieter than the gain resistor. The circuit uses an avalanche photodiode with the cathode biased to approximately 200V. When light is incident on the photodiode, it induces a current IPD which flows into the amplifier circuit. The amplifier output falls negative to maintain balance at its inputs. The transfer function is therefore VOUT = –IPD • 10k. C1 ensures stability and good settling characteristics. Output offset was measured at better than 500 µV, so low in part because R2 serves to cancel the DC effects of bias current. Output noise was measured at below 1mVP–P on a 20MHz measurement bandwidth, with C2 shunting R2’s thermal noise. As shown in the scope photo, the rise time is 45ns, indicating a signal bandwidth of 7.8MHz. |
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