8th International Symposium on Power Semiconductor Devices and ICs. ISPSD '96. Proceedings
DOI: 10.1109/ispsd.1996.509456
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High-temperature performance of SOI and bulk-silicon RESURF LDMOS transistors

Abstract: High-temperature off-state and on-state characteristics of bulk-Si and thin-SO1 RESURF LDMOS transistors were studied experimentally and theoretically. The off-state leakage current in the SO1 devices was only 1.5 n A / p at 300 OC. The increase of on-resistance with temperature in the SO1 devices is smaller than in the bulk-Si devices because of the heavier doping dictated by the RESURF principle. The reverse recovery time of the SO1 device shows only slight temperature dependence. The results of this study i… Show more

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Cited by 17 publications
(24 citation statements)
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“…7.25 shows the reverse log J vs. V of a 4H-SiC, 1100V, Al/C/B-implanted pin junction rectifier Chow 119 . At high reverse bias, some of the SiC junction rectifiers show an increase in reverse current ) that resembles a band-to-band tunneling characteristic, which has been observed in Si on insulator (Arnold, et al 1996). In another case, a space-charge-limited current flow mechanism due to deep traps is also used to explain the dependence of the reverse current on reverse bias (J R ~ V R°, where 2 < n <5) .…”
Section: Chow 117mentioning
confidence: 90%
“…7.25 shows the reverse log J vs. V of a 4H-SiC, 1100V, Al/C/B-implanted pin junction rectifier Chow 119 . At high reverse bias, some of the SiC junction rectifiers show an increase in reverse current ) that resembles a band-to-band tunneling characteristic, which has been observed in Si on insulator (Arnold, et al 1996). In another case, a space-charge-limited current flow mechanism due to deep traps is also used to explain the dependence of the reverse current on reverse bias (J R ~ V R°, where 2 < n <5) .…”
Section: Chow 117mentioning
confidence: 90%
“…Isolating the terms in (2), it is concluded that the predominance of J RTH from J RD in JTPR and LJPR, respectively, is the reason for the different J R (T ) evolution. Indeed, this effect has already been denoted, comparing bulk with thin-film silicon-on-insulator (TF-SOI) power devices [6]. Like in TF-SOI power devices, J RD vanishes when the JTPR drift volume is completely depleted, thus giving a less pronounced J R (T ) rise (56 • C/decade) than that in LJPR (25 • C/decade).…”
Section: B Reverse Characteristicsmentioning
confidence: 97%
“…The physical structure of the two active regions of the devices were initially identical, each 42 μm-long, 0.2 μm-thick and with the same "IOS" layout that sees the gate contact extend over a thick field oxide over the drift region. These are based on SOI devices originally developed by Philips in the 1990s [20]. Despite their identical origins, for both devices to support the same blocking voltage (600 V) the linear doping used in the Si/SiC had to be half that of the SOI doping.…”
Section: The Si/sic Conceptmentioning
confidence: 99%