Clocking Optimization and Distribution in Digital Systems with Scheduled Skews

Hsieh, Hong-Yean; Liu, Wentai; Franzon, Paul D.; Cavin, Ralph K.

doi:10.1007/978-1-4684-8440-3_3

Cited by 2 publications

(3 citation statements)

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“…The MEI boundary condition is based on a finite difference equation to describe how the electromagnetic field distribution on a boundary element relates to the field distribution on the neighboring elements. The finite difference equation is given as (1) where corresponds to the boundary element and correspond to the neighboring elements.…”

Section: Theory and Modelingmentioning

confidence: 99%

“…1521-3323/99$10.00 © 1999 IEEE Let and the coefficients are determined by applying distributions (called metrons) [2] of surface current density on the conductor. The field distribution on the boundary element is determined by equation (1) instead of by the mesh equation from finite element method. The theory of MEI boundary condition is based on three postulates:…”

Section: Theory and Modelingmentioning

confidence: 99%

“…W ITH rapid improvement in transistor switching speeds, the interconnections within and between integrated circuits (IC's) are increasingly limiting the performance of very large scale integration (VLSI) systems [1]. These fine interconnect lines are often complex structures containing multiple layers of dielectric and/or conductor materials.…”

Section: Introductionmentioning

confidence: 99%

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High frequency loss and electromagnetic field distribution for striplines and microstrips [MCM packages]

Lo¹,

Kauffman

Franzon

1999

IEEE Trans. Adv. Packag.

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A new three-component measured equation of invariance (MEI) boundary condition is developed and applied to the hybrid edge/nodal vector finite element method. The electric field distribution on the cross section of various lossy transmission lines is calculated. The propagation constant of a lossy transmission line with coated conductor strip is also calculated. The three-component MEI boundary condition simulates the field distribution on the artificial boundary for electromagnetic field excited by the surface charge density and the three vector components of the electric current density. Numerical experiments are performed to test the method by comparing calculated transmission loss with the measured data.

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Section: Theory and Modelingmentioning

confidence: 99%

Section: Theory and Modelingmentioning

confidence: 99%

Section: Introductionmentioning

confidence: 99%

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