Showing posts with label Metastability in VLSI. Show all posts
Showing posts with label Metastability in VLSI. Show all posts

Metastability


What is metastability: Metastability is a phenomenon of unstable equilibrium in digital electronics in which the sequential element is not able to resolve the state of the input signal; hence, the output goes into unresolved state for an unbounded interval of time. Almost always, this happens when data transitions very close to active edge of the clock, hence, violating setup and hold requirements. Since, data makes transition close to active edge of clock, the flop is not able to capture the data completely. The flop starts to capture the data and output also starts to transition. But, before output has changed its state, the input is cut-off from the output as clock edge has arrived. The output is, then, left hanging between state ‘0’ and state ‘1’. Theoretically, the output may remain in this state for an indefinite period of time. But, given the time to settle down, the output will eventually settle to either its previous state or the new state. Thus, the effect of signal present at input of flop may not travel to the output of the flop partly or completely. In other words, we can say that when a flip-flop enters metastable state, one cannot predict its output voltage level after it exits the metastability state nor when the output will settle to some stable voltage level. The metastability failure is said to have occurred if the output has not resolved itself by the time it must be available for use. Also, since, the output remains in-between ‘0’ and ‘1’, which means both P-MOS and N-MOS are not switched off. Hence, VDD is shorted to GND terminal making it cause a high current to flow through as long as the output is hanging in-between.


Metastability example: Consider a CMOS inverter circuit as shown below. The current vs voltage (we can also say power vs voltage as VDD is constant) characteristics for this circuit are also shown. It can be observed that output current is 0 for both input voltage levels; i.e. ‘0’ and ‘1’. As the voltage level is increased from ‘logic 0’, the current increases. It attains its maximum value at ‘Vin’ somewhere near VDD/2. It again starts decreasing as ‘Vin’ is increased further and again becomes 0 when ‘Vin’ is at ‘logic 1’. Thus, there is a local maxima for power consumption for CMOS inverter. At this point, the device is in unstable equilibrium. As for CMOS inverter, for other CMOS devices too, there lies ‘a local maxima’ at some value of input voltage. We all know that for a flip-flop, the output stage is a combinational gate (mostly an inverter). So, we can say that the output of the flip-flop is prone to metastability provided right input level.


Power characteristics of CMOS inverter
Figure 1: Power characteristics of CMOS inverter

As we now know that a CMOS combinational gate has a point on its ‘voltage characteristic’ curve that is quasi-stable, let us look at a CMOS latch from the same perspective. The CMOS latch has a transmission gate followed by two inverters connected in feedback loop. The voltage characteristic curves for the two inverters are shown. The metastable point, here, lies where the two curves intersect as this point is the resulting peak point of the ‘Superposition curve’ resulting from the two individual curves. A latch goes into metastable state very frequently, especially if the input is changing fast. But, this metastability is resolved quickly as the output tends to go to one of its stable states. As a flop is generally made by connecting two latches in master-slave configuration, the flops are also prone to be metastable. The difference here is just that the probability of a flip-flop being metastable is a lot less than latches as ‘flops are edge sensitive’ as compared to latches which are level sensitive.


Figure showing transfer curve for D-latch and metastable point
Figure 2: Transfer curves of two inverters in a D-latch



We have just came to know that different elements are prone to metastability to different extents. There is a measure to determine the extent to which an element is prone to metastability failure. This is given by an interval known as ‘Mean Time Between Failures’ (MTBF) and is a measure of how prone an element is to failure. It gives the average time interval between two successive failures. The failure rate is given as the reciprocal of MTBF.