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AN601 Datasheet(PDF) 3 Page - Vishay Siliconix |
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AN601 Datasheet(HTML) 3 Page - Vishay Siliconix |
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3 / 8 page ![]() AN601 Vishay Siliconix Document Number: 70572 15-Feb-94 www.vishay.com S FaxBack 408-970-5600 3 DRAIN GATE SOURCE Rb DRAIN GATE SOURCE RP n+ RP RP RB Pp+ epi n– IA IA SUBSTRATE n+ FIGURE 3. Equivalent Circuit and Cross Section Examination of Figure 3 suggests that the current necessary to trigger this series of events might be closely approximated if both the VBE of the parasitic npn bipolar transistor and Rp were known.[7] Test patterns available on the semiconductor wafer during manufacture make it possible to examine such parameters of the parasitic npn bipolar transistor. Measurement results of VBE, beta, and Rp+ from the test pattern are shown in Figure 4. Because of the deep p+ diffusion that forms the Zener structure, the region beneath the n+ diffusion — where Rp is critical—resembles a graded junction. This—in concert with the dramatic temperature rise that together reduces VBE, raises Rp, and increases beta—com- complicates any effort to calculate the critical avalanche current required to excite the parasitic bipolar transistor. Blackburn[8] derived a worst-case calculation; however, the actual performance is substantially better than predicted due to second-order effects. Today’s MOSPOWER devices can safely withstand over two times the 25 _C rated current even at junction temperatures approaching 150 _C. The “active” form of failure is no longer the prevalent mode under normal operating conditions. The limiting mechanism is now usually a thermal failure caused by the large temperature increase during avalanche. The Thermal Effect — The “Passive” Mode. During UIS, as the MOSFET is subjected to increasing energy, the internal chip temperature rises dramatically (equation 4) and is thought to generate a mesoplasma. Such mesoplasmas (regenerative heating) lead to the irreversible damage generally associated with thermal runaway.[1] * The swiftness of this temperature rise, see equation (3), tends to make heat sinks irrelevant for UIS testing. 0 50 100 150 200 250 0.6 0.5 0.4 0 0.3 0.2 0.1 900 800 700 300 600 500 400 120 100 80 0 60 40 20 BETA VBE W/V Temperature ( _C) (BETA) (VBE) ( W/V) FIGURE 4. Parasitic Bipolar Transistor Characteristics During this avalanche period, as defined by equation (3), energy is dissipated in the device equation (2), resulting in a dramatic increase in chip temperature. Blackburn[8] derived the following one-dimensional thermal model to calculate the maximum temperature rise, DTM. *The increasing temperature during mesoplasma formation results in a decreasing thermal conductivity of silicon (see Figure 5a) which, in turn, results in a further increase in the localized temperature. Thermal runaway is thus encouraged. |
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