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Working with S, Y, Z Parameters<br />

Applications<br />

reasons: the model-evaluation time in CPF is less by a factor of 5-7 than that for the<br />

equivalent circuit built from the same poles.<br />

Due to the very nature of fitting, the CPF method always results in a causal solution. It<br />

also has a delay-extraction capability useful when simulating transmission lines or<br />

connectors.<br />

• Digital Signal Processing (DSP) technique is an alternative approach that transforms the<br />

frequency-domain data into time domain parameters via inverse FFT, Hilbert transform<br />

and convolution. Important modifications were made to these basic algorithms to enable<br />

both periodic and non-periodic dependencies, to ensure the causality of the system, to<br />

account for singularities in matrix representation and to ensure high-speed convolution.<br />

If the circuit frequency response is naturally periodic (as for delay-containing operators)<br />

and is given only in a fraction of a single period, the DSP method is recommended to<br />

ensure accurate simulation. In this case, the last point given in the input data file should<br />

correspond to the half-period of the dependence.<br />

• System identification (SI) technique is a third method that represents S parameters in the<br />

form of a rational function in ‘s’ (Laplace variable). These functions are then converted<br />

into systems of linear differential equations so that Eldo can solve them during the<br />

transient analysis.<br />

With the above three methods, Eldo can efficiently solve a wide variety of problems. Frequency<br />

dependencies can be either quite smooth or with a large number of sharp resonant peaks (up to<br />

many hundred). The <strong>user</strong> may specify input data either with equidistant frequency points,<br />

starting from zero or not; or give them in any other way, (for example, logarithmically spaced)<br />

relevant to the method of data acquisition.<br />

Of course, one can expect accurate simulations only if the original data is complete and<br />

accurate. The frequency dependence given should completely encompass the range of interest,<br />

from the lowest to the highest operation frequency. For example, high accuracy at DC is<br />

unlikely if the data starts from non-zero frequency. Similarly, accurate simulation of short<br />

transitions, lasting for hundred ps, is impossible if the highest point is far below tens of GHz.<br />

Also, the data points should be given with good resolution, sufficient to reproduce the shape of<br />

the dependencies. For example, many more points are needed to describe a dependence with<br />

many sharp peaks than for a smooth one, even if they are both defined in the same frequency<br />

range. Finally, the input data should be causal, so that the real and imaginary parts of the<br />

frequency dependence satisfy the dispersion Kronig-Kramers relation. In reality, data becomes<br />

slightly non-causal due to unavoidable measurement/simulation errors, especially (typically) at<br />

higher frequencies. However, serious measurement errors (like taking the negated phase) cause<br />

catastrophic non-causality that will lead to improper simulation results.<br />

Applications<br />

S parameters can originate from the following:<br />

696<br />

Eldo® User's Manual, 15.3

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