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ADCMP573BCP 数据表(PDF) 10 Page - Analog Devices |
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ADCMP573BCP 数据表(HTML) 10 Page - Analog Devices |
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10 / 16 page ![]() ADCMP572/ADCMP573 Preliminary Technical Data Rev. PrB | Page 10 of 16 external 500 Ω resistor, and leaving the LE pin disconnected. In this case, the resistor value does not depend on the chosen VCCO supply voltage, assuming the VTT pin is properly connected to VCCO – 2 V. OPTIMIZING HIGH SPEED PERFORMANCE As with any high speed comparator, proper design and layout techniques are essential to obtaining the specified performance. Stray capacitance, inductance, inductive power and ground impedances, or other layout issues can severely limit performance and can often cause oscillation. Discontinuities along input and output transmission lines can also severely limit the specified pulse-width dispersion performance. For applications working in a 50 Ω environment, input and output matching has a significant impact on data dependant (or deterministic) jitter (DJ) and pulse-width dispersion perform- ance. The ADCMP572/ADCMP573 comparators provide internal 50 Ω termination resistors for both VP and VN inputs, and the ADCMP572 provides 50 Ω back terminated outputs. The return side for each input termination is pinned out separately with the VTP and VTN pins, respectively. If a 50 Ω termination is desired at one or both of the VP/VN inputs, then the VTP and VTN pins can be connected (or disconnected) to (from) the desired termination potential as required. The termination potential should be carefully bypassed using high quality bypass capacitors as discussed above to prevent undesired aberrations on the input signal due to parasitic inductance in the circuit board layout. If a 50 Ω input termination is not desired, either one or both of the VTP/VTN termination pins can be left disconnected. In this case, the pins should be left floating with no external pull-downs or bypassing capacitors. It should be understood that when leaving an input termination disconnected, the internal resistor acts as a small stub on the input transmission path and can cause problems for very high speed inputs. Reflections should then be expected from the comparator inputs because they no longer provide a matched impedance to the input path leading to the device. It then becomes important to back-match the drive source impedance to the input transmission path to minimize multiple reflections. For applications in which the comparator is very close to the driving signal source, the source impedance should be mini- mized. High source impedance in combination with parasitic input capacitance of the comparator could cause an undesirable degradation in bandwidth at the input, thus degrading the overall response. Although the ADCMP572/ ADCMP573 comparators have been designed to minimize input capacitance, some parasitic capacitance is inevitable. It is therefore recommended that the drive source impedance be no more than 50 Ω for best high speed performance. COMPARATOR PROPAGATION DELAY DISPERSION The ADCMP572/ADCMP573 comparators are designed to reduce propagation delay dispersion over a wide input overdrive range of 5 mV to 500 mV. Propagation delay dispersion is a variation in propagation delay that results from a change in the degree of overdrive or slew rate (how far or how fast the input signal exceeds the switching threshold). Propagation delay dispersion is a specification that becomes important in high speed time critical applications such as data communication, automatic test and measurement, instrumenta- tion, and event-driven applications such as pulse spectroscopy, nuclear instrumentation, and medical imaging. Dispersion is defined as the variation in propagation delay as the input over- drive conditions are changed (Figure 14 and Figure 15). For the ADCMP572/ADCMP573, dispersion is typically <15 ps because the overdrive is varied from 10 mV to 500 mV, and the input slew rate is varied from 2 V/ns to 10 V/ns. This specification applies for both positive and negative signals since the ADCMP572/ADCMP573 has substantially equal delays for either positive-going or negative-going inputs. Q/Q OUTPUT INPUT VOLTAGE 500mV OVERDRIVE 10mV OVERDRIVE DISPERSION VN ± VOS Figure 14. Propagation Delay—Overdrive Dispersion Q/Q OUTPUT INPUT VOLTAGE 10V/ns 1V/ns DISPERSION VN ± VOS Figure 15. Propagation Delay—Slew Rate Dispersion |
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