功率mosfet中轻掺杂电阻区的载流子动力学

T. Iizuka
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引用次数: 0

摘要

通过二维器件仿真,分析了横向双扩散MOS (LDMOS)晶体管中轻掺杂电阻区的二维电流流动。在保留其理论支柱HiSIM_HV的同时,探索了概念上的扩展。HiSIM_HV是工业标准的基于表面电位的高压mosfet紧凑模型。由于电流流线从沟道平滑地过渡到LDMOS本特性MOSFET部分沟道附近的轻掺杂区域,因此发生在轻掺杂电阻区栅极重叠表面的表面积累被视为扩展沟道而不是扩展漏极。通道偏移长度(ΔL)可以在漂移-扩散模型的框架内表示,并且可以与特征准费米电压Vdive相关,其中积累电流流线已经完全脱离表面。HiSIM_HV的内部漏极节点(DP或d ')被认为放置在一个由栅极控制的横向和漏极控制的横向扩展的耗尽区边界的开口上,而许多紧凑模型将DP放置在通道和轻掺杂区域之间的边界上。本征MOSFET的有效漏极电压(Vdseff)与栅极控制的漏极电压有关,而不是与DP处的准费米电压(Vdp)有关。因此,固有MOSFET的漏极电压在关断状态下几乎保持与外部施加的漏极电压一样高,而它在固有MOSFET部分的导通状态开始时突然下降的困难有望得到缓解。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Carrier Dynamics in Lightly-doped Resistance Region in Power MOSFETs
Two-dimensional current flow in the lightly-doped resistive region in a lateral double-diffused MOS (LDMOS) transistor was analyzed through 2D device simulation. While retaining its theoretical backbone of HiSIM_HV, the industry-standard surface-potential-based compact model for high-voltage MOSFETs, a conceptual extension is explored. Owing to a smooth transit of current flowlines from the channel to the lightly doped region adjacent to the channel of the intrinsic MOSFET part of LDMOS, the surface accumulation occurring at the gate-overlapped surface of the lightly doped resistive region is regarded as an extended channel rather than an extended drain. The channel offset length (ΔL) can be expressed within the framework of the drift-diffusion model and can be related with a characteristic quasi-Fermi voltage Vdive where accumulation current flowlines have already completely dived away from the surface. The HiSIM_HV’s internal drain node (DP or alternatively d’) is regarded as being placed at an opening bounded by the gate-controlled transverse and the drain-controlled lateral extension of depletion region, while many compact models place DP at the boundary between the channel and the lightly doped region. The intrinsic MOSFET’s effective drain voltage (Vdseff) is related to gate controlled Vdive rather than the quasi-Fermi voltage (Vdp) at DP. Hence, a difficulty in that the intrinsic MOSFET’s drain voltage stays almost as high as externally applied drain voltage at the off-state, while it suddenly drops at the onset of on-state of the intrinsic MOSFET part is expected to be mitigated.
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