An LDMOS with large SOA and low specific on-resistance
An LDMOS with nearly rectangular-shape safe operation area (SOA) and low specific on-resistance is proposed. By utilizing a split gate, an electron accumulation layer is formed near the surface of the n-drift region to improve current conduction capability during on-state operation. As a result, the...
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Published in | Journal of semiconductors Vol. 37; no. 5; pp. 52 - 55 |
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Main Author | |
Format | Journal Article |
Language | English |
Published |
01.05.2016
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Subjects | |
Online Access | Get full text |
ISSN | 1674-4926 |
DOI | 10.1088/1674-4926/37/5/054006 |
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Summary: | An LDMOS with nearly rectangular-shape safe operation area (SOA) and low specific on-resistance is proposed. By utilizing a split gate, an electron accumulation layer is formed near the surface of the n-drift region to improve current conduction capability during on-state operation. As a result, the specific on-resistance can be low- ered down to 74.7 m~2.cm2 for a 600 V device from simulation. Furthermore, under high-voltage and high-current conditions, electrons and holes flow as majority carriers in the n-drift region and p-type split gate, respectively. Due to charge compensation occurring between holes and electrons, the local electric field is reduced and impact ion- ization is weakened in the proposed device. Therefore, a higher on-state breakdown voltage at large V6s is obtained and snap-back is suppressed as well. |
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Bibliography: | 11-5781/TN LDMOS; safe operation area (SOA); snap-back; split gate An LDMOS with nearly rectangular-shape safe operation area (SOA) and low specific on-resistance is proposed. By utilizing a split gate, an electron accumulation layer is formed near the surface of the n-drift region to improve current conduction capability during on-state operation. As a result, the specific on-resistance can be low- ered down to 74.7 m~2.cm2 for a 600 V device from simulation. Furthermore, under high-voltage and high-current conditions, electrons and holes flow as majority carriers in the n-drift region and p-type split gate, respectively. Due to charge compensation occurring between holes and electrons, the local electric field is reduced and impact ion- ization is weakened in the proposed device. Therefore, a higher on-state breakdown voltage at large V6s is obtained and snap-back is suppressed as well. ObjectType-Article-1 SourceType-Scholarly Journals-1 ObjectType-Feature-2 content type line 23 |
ISSN: | 1674-4926 |
DOI: | 10.1088/1674-4926/37/5/054006 |