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ADCMP609BRMZ1 Scheda tecnica(PDF) 9 Page - Analog Devices |
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ADCMP609BRMZ1 Scheda tecnica(HTML) 9 Page - Analog Devices |
9 / 12 page ADCMP609 Rev. 0 | Page 9 of 12 Propagation delay dispersion is a specification that becomes important in high speed, time-critical applications, such as data communication, automatic test and measurement, and instru- mentation. It is also important in event-driven applications, such as pulse spectroscopy, nuclear instrumentation, and medical imaging. Dispersion is defined as the variation in propagation delay as the input overdrive conditions are changed (see Figure 12 and Figure 13). ADCMP609 dispersion is typically <12 ns as the overdrive varies from 10 mV to 125 mV. This specification applies to both positive and negative signals because the device has very closely matched delays for both positive-going and negative-going inputs, and very low output skews. Remember to add the actual device offset to the overdrive for repeatable dispersion measurements. Q/Q OUTPUT INPUT VOLTAGE 500mV OVERDRIVE 10mV OVERDRIVE DISPERSION VN ± VOS Figure 12. Propagation Delay—Overdrive Dispersion Q/Q OUTPUT INPUT VOLTAGE 10V/ns 1V/ns DISPERSION VN ± VOS Figure 13. Propagation Delay—Slew Rate Dispersion COMPARATOR HYSTERESIS The addition of hysteresis to a comparator is often desirable in a noisy environment, or when the differential input amplitudes are relatively small or slow moving. The transfer function for a comparator with hysteresis is shown in Figure 14. As the input voltage approaches the threshold (0.0 V, in this example) from below the threshold region in a positive direction, the compara- tor switches from low to high when the input crosses +VH/2. The new switching threshold becomes −VH/2. The comparator remains in the high state until the threshold, −VH/2, is crossed from below the threshold region in a negative direction. In this manner, noise or feedback output signals centered on 0.0 V input cannot cause the comparator to switch states unless it exceeds the region bounded by ±VH/2. OUTPUT INPUT 0 VOL VOH +VH 2 –VH 2 Figure 14. Comparator Hysteresis Transfer Function The customary technique for introducing hysteresis into a comparator uses positive feedback from the output back to the input. One limitation of this approach is that the amount of hysteresis varies with the output logic levels, resulting in hysteresis that is not symmetric about the threshold. The external feedback network can also introduce significant parasitics that reduce high speed performance and can even induce oscillation in some cases. The ADCMP609 comparator offers a programmable hysteresis feature that significantly improves accuracy and stability. Con- necting an external pull-down resistor or a current source from the HYS pin to GND varies the amount of hysteresis in a pre- dictable, stable manner. Leaving the HYS pin disconnected or driving it high removes the hysteresis. The maximum hysteresis that can be applied using this pin is approximately 160 mV. Figure 15 illustrates the amount of hysteresis applied as a function of the external resistor value. 160 150 140 130 120 110 100 90 80 70 60 50 40 30 20 10 0 1300 1200 1100 1000 900 800 700 600 500 400 300 200 100 0 HYS RESISTOR (kΩ) VCC = 5.5 VCC = 2.5 Figure 15. Hysteresis vs. HYS Resistor The hysteresis control pin appears as a 1.25 V bias voltage seen through a series resistance of 7 kΩ ± 20% throughout the hysteresis control range. The advantages of applying hysteresis in this manner are improved accuracy, improved stability, reduced component count, and maximum versatility. An external bypass capacitor is not recommended on the HYS pin because it impairs the latch function and often degrades the jitter performance of the device. |
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