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Static Noise Margin Analysis of Various SRAM Topologies - IJET

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IACSIT International Journal <strong>of</strong> Engineering and Technology, Vol.3, No.3, June 2011still precharged to ‘1’. The internal node <strong>of</strong> the bit-cell thatrepresents a zero gets pulled upward through the accesstransistor due to the voltage dividing effect across the accesstransistor and drive transistor. This increase in voltageseverely degrades the SNM during the read operation (readSNM) as shown in the Fig.3. The butterfly curve during holdand read illustrates the degradation in SNM during read.C. Dependence <strong>of</strong> SNM on Sizing <strong>of</strong> the TransistorsThe cell ratio has very little impact on SNM duringsub-threshold read. The lower impact <strong>of</strong> sizing is reasonableconsidering the exponential dependence <strong>of</strong> sub-thresholdcurrent on other parameters. Fig. 6 shows that the sizingchange affects linearly and only have a logarithmic impact onthe VTCs. As a result <strong>of</strong> narrow or short channel effects, theV T for deep submicron devices tends to vary with size. Theseeffects depend on the technology and make the general SNMmodeling more complicated, see [10,21].Fig. 3. Butterfly Curves during Read and Write [10]III. SNM DEPENDENCIESThis section explores the different parameters on which theSNM is dependent. The factors are supply voltage,temperature and doping variations.A. Dependence <strong>of</strong> SNM on VddThe SNM for a bit-cell with ideal VTCs is still limitedV dd /2 to because <strong>of</strong> the two sides <strong>of</strong> the butterfly curve. Anupper limit on the change in SNM with V dd is thus 1/2. Fig. 4,plots SNM versus V dd directly for both, hold and read mode.From [10], the slopes <strong>of</strong> the curves confirm that less than 1/2V dd <strong>of</strong> noise will translate into SNM changes.Fig. 4. SNM versus Vdd Curve [10]B. Dependence <strong>of</strong> SNM on TemperatureFig.5. SNM versus Temperature Curve [21][21] it is shown that the exponential dependence <strong>of</strong> currenton sub-threshold operation increases the random variationeffects.Fig. 6. SNM versus Cell Ratio Curve [10]IV. READ AND WRITE ABILITY OF <strong>SRAM</strong> CELLSThere are three operating modes in <strong>SRAM</strong>, standby, read,and write. Each mode can define its own operating margin.When the cell is in the standby, its wordline (WL) isconnected to the ground. In order to hold its data properly,the cross-coupled two inverters in the cell must sustainbi-stable operating points. As shown in [14], the SNM is acommon measure <strong>of</strong> the ability for the cell inverters tomaintain their state. The SNM equals the minimum noisevoltage present at each <strong>of</strong> the data storage nodes (VL, VR)necessary to flip state <strong>of</strong> the cell. As shown in the dotted linein Fig.2, it is graphically defined as the length <strong>of</strong> side <strong>of</strong> thepossible maximum square between the normal and inversevoltage transfer characteristic (VTC) <strong>of</strong> two identical cellinverters. Specifically, the Conventional 6T <strong>SRAM</strong> cell ismore sensitive to noise during read access. When the cell is in,the read access, the wordline is connected to V dd while thebit-line pairs (BL, BLB) are precharged to V dd . The data ‘0’storage node rises to a certain voltage higher than the groundaccording to the voltage dividing across the access transistorand driver transistor. Moreover, the gain <strong>of</strong> the <strong>Static</strong>Transfer Characteristic (STC) is lowered due to the parallelconnection <strong>of</strong> the conducting access transistor and the loadPMOS transistor. This severely degrades the cell immunity tonoise. The side <strong>of</strong> the possible maximum square nestedbetween the normal and inverse VTC during the read accessthus equals the read SNM <strong>of</strong> the cell. It is represented by thesolid line in Fig. 3.In the Fig. 7 (a), a conceptual setup measuring for the cellwrite margin is shown. Let’s assume that the inv-1 side in thecell initially holds a data ‘0’ and the inv-2 side holds a data‘1’, respectively. When the cell is in the write access, theword-line is connected to V dd , while the bitline pairs aredriven to V dd and the ground to flip the cell state. Then, thedata storage node <strong>of</strong> inverter-2 side will be falling down from305

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