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ACM-SIGDA's ACM-SIGDA Physical Design Workshop #5 1996: Proceedings PDF

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Let the rise times of the signals be much larger than the propagation delays, so that a lumped RC model is adequate[3]. As the noise pulse is essentially a small signal, linearity and time-invariance can Clearly, the proof holds even if the input has non-zero rise time. 28 The possibility of using overlaps with nets switching slowly to decrease the overall crosstalk on a victim net. Note that overlap is never used to advantage by any of the previous routing methods. Our expression shows that increasing overlap length increases the crosstalk contribution of that particular aggressor.

Maximum noise amplitude Noise pulse width X Figure 9. Transforming the A-W plot to a Ei vs. 5. Channel routing results In this sub-section we describe the experimental results obtained using our channel router. We compare the greedy channel router oblivious to coupled noise with the algorithm outlined in the previous sub-section, both implemented in C. The implementation in [11] was not available[19] and therefore could not be compared. The average normalized (to the supply voltage) coupled noise results are presented in Table 1.

Section III uses these expressions to show that routing driven by the new model could be significantly better than routing driven by the charge sharing model. A new algorithm is also proposed and experimental results are presented. Section IV concludes with a discussion on the likely impact of this paper. to C2 Figure 2. Equivalent circuit for calculating coupled noise The following two theorems lead to expressions for the coupled noise pulse amplitude and width. Both the expressions are derived from the differential equations characterizing the system and no explicit time-domain solution is necessary.

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