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Development of a New Electro-thermal Simulation Tool for RF circuits

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10 1.2. The limitations <strong>of</strong> present simulation codes<br />

Figure 1.12: <strong>Electro</strong>-<strong>thermal</strong> simulation with ADS from Agilent. Both self and mutual<br />

interactions are included.<br />

ity to activate the self-heating option (see e.g., the model MEXTRAM 504 <strong>for</strong> bipolar<br />

junction transistors). Such models are equipped with a supplementary terminal, namely<br />

a "<strong>thermal</strong> node", and include a default value <strong>for</strong> the <strong>thermal</strong> self-resistance. Hence,<br />

the temperature increase above ambient is evaluated from the dissipated power and<br />

considered, in turn, as a further input that modifies the <strong>thermal</strong>ly-sensitive parameters<br />

(electro-<strong>thermal</strong> feedback). However, <strong>thermal</strong> interactions between active devices<br />

integrated in the chip are not accounted <strong>for</strong>, which represents a considerable limitation<br />

<strong>for</strong> the electro-<strong>thermal</strong> simulation <strong>of</strong> high-density ICs.<br />

The possible solution to the problem could be the development <strong>of</strong> new schematic components,<br />

so called <strong>Electro</strong>-<strong>thermal</strong> Feedback Blocks (ETFBs), as shown in Fig. 1.12.<br />

Correctly constructed ETFB could take into account both types <strong>of</strong> electro-<strong>thermal</strong><br />

interactions that is <strong>for</strong> self and mutual ones.

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