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Download e-book for iPad: An Artificial Intelligence Approach to VLSI Design by Thaddeus J. Kowalski

By Thaddeus J. Kowalski

ISBN-10: 089838169X

ISBN-13: 9780898381696

Publication through Kowalski, Thaddeus J.

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F /. 94)). t / is included ( approaches 0 from below). The parameter s is complex and is often referred to as the complex frequency. The Laplace transformation transforms a function from the time domain onto the complex frequency domain (s-domain). sp /. s/ is given. t / dies out as t approaches infinity). s/. s/j goes to infinity when s approaches sp . t / is stable. t // lim f . s/ lim f . s/: L. More details on the Laplace transformation can be found in [47]. 0/ denote the initial conditions (incremental response at t D 0) of the incremental circuit.

The noise model of a diode is more complicated. Two additional noise signals appear at the p–n junction: shot noise and flicker noise (1=f noise). Shot noise is caused by the random fluctuations of the diode current. The fluctuations occur because the current consists of a flow of discrete charges (electrons). t /). 106) where Kf is the flicker noise coefficient and Af is the flicker noise exponent. 107) Noise models of other circuit elements are similar to the diode noise model, where the noise is modeled as a noise current source with a given power spectrum density (see Fig.

5 left). 50 Fig. 4 x, Real Fig. 5 Left: identifying a curve. Right: measuring with the mouse cursor The position of the cursor is displayed in the bottom of the plot window (Fig. 5 right). It changes as you move the cursor. Now we will zoom the curve so we can measure the gain. Make the plot window active and press Z. The cursor changes shape, indicating that the box zoom mode is on. If you want to turn the zoom mode off, press Z again. If you turned the zoom mode off, turn it back on, move the cursor to the upper left part of the rectangle you wish to zoom, and press the left mouse button.

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An Artificial Intelligence Approach to VLSI Design by Thaddeus J. Kowalski


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