2001
DOI: 10.1016/s0026-2692(01)00023-4
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A new generation of power lateral and vertical floating islands MOS structures

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Cited by 11 publications
(4 citation statements)
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“…These are available as commercial products on silicon but only as prototypes on 4H-SiC. Sophisticated silicon structures include alternate P-type and N-type zones in the active layer for getting higher voltage handling (11), so called Mesh-MOS by STM (4), and Cool-MOS by Infineon (6). Bipolar IGBT has very similar structure, but with P+ substrate.…”
Section: Optionnal P-type Inclusionsmentioning
confidence: 99%
“…These are available as commercial products on silicon but only as prototypes on 4H-SiC. Sophisticated silicon structures include alternate P-type and N-type zones in the active layer for getting higher voltage handling (11), so called Mesh-MOS by STM (4), and Cool-MOS by Infineon (6). Bipolar IGBT has very similar structure, but with P+ substrate.…”
Section: Optionnal P-type Inclusionsmentioning
confidence: 99%
“…V br in the area between two adjacent buried oxide layer can be expressed by (2) Where E s is the electric field of the drift region. The electric filed is almost uniform due to the modulation effect of Qs when y <= D], therefore, V br2 enhances by 0.5D]E s in comparison with the conventional PSOI VDMOS.…”
Section: Vdmosmentioning
confidence: 99%
“…The main weakness of this device is that the specific on-resistance (Ron-sp) increases drastically with the increase of the breakdown voltage (V br ) [I] . The floating island MOSFET (FLIMOS) [2][3], oppositely doped buried regions MOSFET [4], power devices with dielectric charge traps [5] , super junction MOSFET [6] and the partial silicon-on-insulator VDMOS (PSOI VDMOS) [7] have been proposed to enhance the V br while keeping a low R on • sr…”
mentioning
confidence: 99%
“…This P buried layer is located under the PsBody/N' plane junction in order to divide, under reverse bias conditions, the maximal electric field into two parts (Fig. 2), allowing the improvement of the breakdown voltage for the same N' epitaxial layer doping concentration [3]. This basically happens due to the fact that the negative charges in the depleted P floating layer tend to terminate a large part of the flux induced by the positive charges of the depleted N' drift region so that the field intensity is not allowed to accumulate throughout the entire thickness of the epitaxial layer, and a larger doping density can be used without producing a high peak field [7].…”
mentioning
confidence: 99%