2018
DOI: 10.1109/ted.2018.2802485
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Improvement of Deep-Trench LDMOS With Variation Vertical Doping for Charge-Balance Super-Junction

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Cited by 18 publications
(5 citation statements)
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“…DT SJ LDMOS, some other reported structures [12−18] and DC DT SJ LDMOS proposed in this paper. From the figure it can be seen that the electrical performance of the device breaks through the "silicon limit" [11] .…”
Section: Results Of the Simulationmentioning
confidence: 99%
“…DT SJ LDMOS, some other reported structures [12−18] and DC DT SJ LDMOS proposed in this paper. From the figure it can be seen that the electrical performance of the device breaks through the "silicon limit" [11] .…”
Section: Results Of the Simulationmentioning
confidence: 99%
“…Based on the common structure of T-LDMOS, many improved structures are proposed [4]- [12], such as the ones with vertical field plates in the trench [7]- [9], and the ones with variable-k trench-dielectric [10]- [12]. Recently, many studies start applying a well-known technique of super junction (SJ) to the LDMOS [13]- [16], as well as to the T-LDMOS [17]- [20], such as the T-LDMOS with a quasi vertical (QV) SJ structure [17], [19], [20] and that with a lateral SJ structure at the trench bottom [18]. However, because the trench acts as a capacitor in the off-state and disturbs the surface electric-field (e-field) distribution [19], a QVSJ structure in T-LDMOS is hard to satisfy the important charge-balanced condition and, therefore, cannot be fully used to improve the device performance.…”
Section: Introductionmentioning
confidence: 99%
“…Recently, many studies start applying a well-known technique of super junction (SJ) to the LDMOS [13]- [16], as well as to the T-LDMOS [17]- [20], such as the T-LDMOS with a quasi vertical (QV) SJ structure [17], [19], [20] and that with a lateral SJ structure at the trench bottom [18]. However, because the trench acts as a capacitor in the off-state and disturbs the surface electric-field (e-field) distribution [19], a QVSJ structure in T-LDMOS is hard to satisfy the important charge-balanced condition and, therefore, cannot be fully used to improve the device performance. Although some studies have paid attention to deal with that, they mostly rely on some costly process to realize the complex structures, such as the drift region with the variation vertical doping [19] and the trapezoidal trench [20].…”
Section: Introductionmentioning
confidence: 99%
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“…The BV of the power device is limited by the low lateral BV for the poor surface electric field distribution, and some work has been carried out, such as the variable lateral doping (VLD), [4][5][6][7] super junction, [8,9] and charge islands. [10] Enhancing the electric field (ENDIF) of the dielectric buried layer is a feasible method to increase the vertical BV and several new structures have been developed [11][12][13][14][15] in which introducing self-adaptive interface charges are effective and attractive.…”
Section: Introductionmentioning
confidence: 99%