2006
DOI: 10.1109/ted.2006.876285
|View full text |Cite
|
Sign up to set email alerts
|

Theory of electrothermal behavior of bipolar transistors: part III-impact ionization

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1
1

Citation Types

0
29
0
1

Year Published

2009
2009
2016
2016

Publication Types

Select...
5
2

Relationship

2
5

Authors

Journals

citations
Cited by 53 publications
(30 citation statements)
references
References 32 publications
0
29
0
1
Order By: Relevance
“…MC data Rickelt and Rein model [6] Rinaldi and d Alessandro model [9] New model MC data Rickelt and Rein model [6] Rinaldi and d Alessandro model [9] New model Here a represents the common-base current gain, and i à b is a normalized base critical current. As shown in [5], i à b depends only on the emitter window aspect ratio a = L E /W E (see Fig.…”
Section: Discussionmentioning
confidence: 99%
See 1 more Smart Citation
“…MC data Rickelt and Rein model [6] Rinaldi and d Alessandro model [9] New model MC data Rickelt and Rein model [6] Rinaldi and d Alessandro model [9] New model Here a represents the common-base current gain, and i à b is a normalized base critical current. As shown in [5], i à b depends only on the emitter window aspect ratio a = L E /W E (see Fig.…”
Section: Discussionmentioning
confidence: 99%
“…[6][7][8][9]). These models retain a reasonable accuracy only for a limited range of the collector voltage.…”
Section: Avalanche Multiplication Factor Modelmentioning
confidence: 99%
“…An Internet search on high-voltage FET failures revealed several papers documenting thermal effects in certain types of large-area FETs that can result in failures well below their published specifications [3,4]. Although no one paper described our problem, we concluded that we likely did have a thermal stability issue specific to large-area, high-gain, lowresistance, high-voltage FETs in linear service.…”
Section: ω 10w 1000ωmentioning
confidence: 92%
“…Impact ionization was enabled by exploiting in the cell macromodels the model for the avalanche multiplication factor proposed in [20], which was extended to account for a positive differential resistance (oI/oV > 0) of the avalanche curve (i.e., the I D -V DS characteristic corresponding to V GS = 0 V). The fitting parameters of the model were tailored by comparison with the measured UIS waveforms.…”
Section: Simulation Of Uis Testsmentioning
confidence: 99%