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LT1319CS 数据表(PDF) 6 Page - Linear Technology |
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LT1319CS 数据表(HTML) 6 Page - Linear Technology |
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6 / 12 page ![]() 6 LT1319 ing the voltage noise gain. Referring to the Block Diagram, at frequencies beyond the corner frequency of the AC coupling loop, the preamp is in a noise gain of 2.5 due to the ratio of (RFB + RL1)/RL1. At high frequencies the input capacitance approaches the same impedance as RL1 so the noise gain increases. For example, at 500kHz the 30pF input capacitance looks like 10.6k Ω which increases the noise gain to almost 4. The preamp is compensated to provide a flat current-to-voltage frequency response with a –3dB corner at 7MHz. The input current noise peaks up considerably if full bandwidth is used. To obtain best noise performance, the output of the preamp should be filtered to the minimum bandwidth required for the desired modula- tion scheme. The graph of input-referred noise versus lowpass filtering on the preamp output shows the noise penalty for higher bandwidths. AC Coupling Loops There are three AC loops in the circuit that reject low frequency inputs. The first loop is around the preamp and provides rejection of ambient light sources. The operation can be explained by looking at the Block Diagram. For low frequency signals the transconductance amplifier, GM1, compares the preamp output to the VBIAS voltage. This differential voltage is transformed into a current that is fed into the high impedance node at Pin 3 and transformed back to a voltage. There is a voltage gain of approximately 60dB to this point which is then buffered to drive a 10k resistor that is connected back to the input of the preamp. This high gain loop attenuates the effect of low frequency signals by the amount of the loop gain times the ratio of RL1 to RFB (i.e., 1000V/V • 15/10 = 1500). For higher frequen- cies the attenuation decreases due to the external capacitor on Pin 3. At frequencies beyond where the loop gain equals 10/15, signals are no longer attenuated. This high fre- quency cutoff is at: f = (15/10)/(2 π • 4kΩ • CPIN3) where 1/(4k Ω) is the transconductance of the loop ampli- fier. For example, if CPIN3 = 300pF, the highpass frequency is 200kHz which can aid in rejection of a wide range of ambient interference. The other two loops operate similarly around the gain stages and also provide low frequency rejection. In addi- APPLICATIONS INFORMATION Layout and Passive Components The LT1319 requires careful layout techniques to minimize parasitic signal coupling to the preamp input. A sample board layout for the circuit on the first page is shown in the Typical Application section. The lead lengths on the photo- diode must be as short as possible to Pin 2. Shielding is recommended over the entire circuit. A ground plane must be used and connected to Pin 1. The ground plane should extend under the package and surround Pins 1 to 9 and Pin 16. A single point connection should be made to the ground plane at Pin 12 (DIG_GND). The leads on Pins 6 and 8 should be short to prevent pickup into the gain stages. The comparator output leads (Pins 10 and 13) should be as short as possible to minimize coupling back to the input via parasitic capacitance. Capacitance on Pin 10 should be minimized as the com- parator output is pulled up by an internal 5k resistor. The associated digital circuitry should be located on the oppo- site side of the PC board from the LT1319 or separated as much as possible if on the same side of the board. Filter components should be located on the analog ground side of the package. Bypass capacitors should be used on Pins 5, 11, 15 and 16 for best supply rejection. Preamp The LT1319 preamp is a low noise, high speed current-to- voltage converter that has been optimized for an input capacitance of 30pF (which corresponds to the capaci- tance of the above-mentioned photodiodes with approxi- mately 2V of back bias). A range of 0pF to 50pF is acceptable. The amplifier obtains high bandwidth by pro- viding a low impedance input so that the input current is not filtered by the photodiode capacitance. The dynamic range of the circuit will be limited at the low end by the input-referred current noise of the preamplifier and the desired signal-to-noise ratio. At the other extreme of the dynamic range for very large input signals, the output of the preamp is clamped by Schottky diodes across the feedback resistor. The noise bandwidth is shaped by filtering at the output of the preamplifier and by the AC coupling loop. The input capacitance causes noise peaking for high bandwidth applications. Noise peaking can be explained by consider- |
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