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ABSTRACT
We give new methods for calculating the time-domain response for a finite-length distributed RC line that is stimulated by a ramp input. The following are our contributions. First, we obtain the solution of the diffusion equation for a seminfinite distributed RC line with ramp input. We then present a general and, in the limit, exact approach to compute the time-domain response for finite-length RC lines under ramp input by summing distinct diffusions starting at either end of the line. Next, we obtain analytical expressions for the finite time-domain voltage response for an open-ended finite RC line and for a finite RC line with capacitive load. The delay estimates using this method are very close to SPICE-computing delays. Finally, we present a general recursive equation for computing the higher-order diffusion components due to reflections at the source and load ends. Future work extends our method to response computations in general interconnection trees by modeling both reflection and transmission coefficients at discontinuities.
REFERENCES
Note: OCR errors may be found in this Reference List extracted from the full text article. ACM has opted to expose the complete List rather than only correct and linked references.
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1
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2
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ABUELMA'ATTI, M.T. 1989. Multipole approximation of capacitively loaded VLSI interconnections. IEEE Proceedings G 136 (June), 118-120.
|
| |
3
|
ABUELMA'ATTI, M.T. 1990. The waveform degradation in VLSI interconnections. IEEE J. Solid-State Circuits 25 (Aug.), 1014-1016.
|
| |
4
|
ABUELMA'ATTI, M.T. 1991. Modeling of capacitively (resistively)-loaded uniform RC lines for computer aided-analysis. IEEE Proceedings-G 138, 463-466.
|
| |
5
|
ANTINONE, R. J. AND BROWN, G. W. 1983. The modeling of resistive interconnects for integrated circuits. IEEE J. Solid-State Circuits 18 (April), 200-203.
|
| |
6
|
BAKOGLU, H.B. 1990. Circuits, Interconnections and Packaging for VLSI. Addison-Wesley.
|
| |
7
|
CAMPBELL, G. A. AND FOSTER, R. M. 1957. Fourier Integrals for Practical Applications, Princeton, Van Nostrand.
|
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8
|
ELMORE, W. C. 1948. The transient response of damped linear networks with particular regard to wideband amplifiers. J. Appl. Phys. 19 (Jan.), 55-63.
|
| |
9
|
HEALEY, M. 1967. Tables of Laplace, Heaviside, Fourier, and Z Transforms. W & R Chambers Ltd.
|
| |
10
|
|
 |
11
|
|
| |
12
|
KAHNG, A. B. AND MUDDU, S. 1996. New diffusion-based analyses of distributed RC interconnections. IEEE International Symposium on Circuits and Systems (May). Also available as Res. Rep. UCLA CS Dept. TR-950019.
|
| |
13
|
KAHNG, A. B. AND ROBINS, a. 1994. On Optimal Interconnections for VLSI. Kluwer Academic.
|
| |
14
|
KAUFMAN, W. M. AND GARRETT, S.J. 1962. Tapered distributed filters. IRE Trans. Circuit Theor. (Dec.), 329-336.
|
| |
15
|
KAUPP, H.R. 1989. Waveform degradation in VLSI interconnections. IEEE J. Solid-State Circuits (Aug.), 1150-1153.
|
| |
16
|
KEVORKIAN, J. 1990. Partial Differential Equations: Analytical Solution Techniques. Wadsworth & Brooks/Cole.
|
| |
17
|
MATTES, H.L. 1993. Behavior of a single transmission line stimulated with a step function. Manuscript, Aug.
|
| |
18
|
Noel Menezes , Satyamurthy Pullela , Florentin Dartu , Lawrence T. Pillage, RC interconnect synthesis—a moment fitting approach, Proceedings of the 1994 IEEE/ACM international conference on Computer-aided design, p.418-425, November 06-10, 1994, San Jose, California, United States
|
| |
19
|
PEIRSON, R. C. AND BERTNOLLI, E.C. 1969. Time-domain analysis and measurement techniques for distributed RC structures. II. Impulse measurement techniques. J. Appl. Phys. (June), 118-122.
|
 |
20
|
|
| |
21
|
SAKURAI, T. 1983. Approximation of wiring delay in MOSFET LSI. IEEE J. Solid-State Circuits SC-18 (Aug.), 418-426.
|
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22
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WILNAI, A.1971. Open-ended RC line model predicts MOSFET IC response. EDN (Dec. 15). pp. 53-54.
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REVIEW
"Linda Pagli : Reviewer"
A new method is presented for computing a mathematical analysis of
the time-domain response of a distributed RC line with ramp input. The
main result is obtained by summing the contributions of distinct
diffusion starting at either end of the
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