1966
DOI: 10.1016/0038-1101(66)90095-5
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Second breakdown and current distributions in transistors

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Cited by 11 publications
(3 citation statements)
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“…Second breakdown in SOS diodes under reverse bias has been explained as an electrothermal phenomenon involving current filamentation ( 6,7,10). For diodes having a p+ -n -n+ structure , the regions of most concern in second breakdown are , for reverse bias , the p+ -n junction and the n region and , for forward bias , the n region alone .…”
Section: A Simplfied Computer Model For Current Filamentation Inmentioning
confidence: 99%
“…Second breakdown in SOS diodes under reverse bias has been explained as an electrothermal phenomenon involving current filamentation ( 6,7,10). For diodes having a p+ -n -n+ structure , the regions of most concern in second breakdown are , for reverse bias , the p+ -n junction and the n region and , for forward bias , the n region alone .…”
Section: A Simplfied Computer Model For Current Filamentation Inmentioning
confidence: 99%
“…Observations of the current distributions in transistors under various conditions of operation were made with the use of temperature-sensitive phosphors. 16 The temperature of the device will increase in areas of high current density. The current constriction associated with second breakdown was demonstrated by these experiments.…”
Section: Second Breakdownmentioning
confidence: 99%
“…Local hot spots can then be identified. These may be caused by defects in the bond between the chip and header, current hogging or secondary breakdown (Hamiter 1967, Schafft and French 1966, Agatsuma 1966.…”
Section: Introductionmentioning
confidence: 99%