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Carrier Dynamics in Lightly-doped Resistance Region in Power MOSFETs

机译:功率MOSFET中轻掺杂电阻区域的载流子动力学

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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.
机译: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中的二维电流。在保留其HiSIM_HV的理论主干的基础上,HiSIM_HV是用于高压MOSFET的行业标准,基于表面电势的紧凑型模型,但仍在探索概念扩展。由于电流流线从沟道平滑过渡到与LDMOS的本征MOSFET部分的沟道相邻的轻掺杂区域,因此在轻掺杂电阻区域的栅极重叠表面上发生的表面累积被视为扩展沟道而不是延长排水时间。通道偏移长度(ΔL)可以在漂移扩散模型的框架内表达,并且可以与准费米电压V相关 潜水 那里的累积电流流线已经完全脱离了地面。 HiSIM_HV的内部漏极节点(DP或d')被视为位于由耗尽区的栅极控制的横向和漏极控制的横向延伸所界定的开口处,而许多紧凑模型将DP置于沟道之间的边界处和轻掺杂区。本征MOSFET的有效漏极电压(V dseff )与门控V有关 潜水 而不是准费米电压(V dp )。因此,可以缓解本征MOSFET的漏极电压几乎保持与外部施加的漏极电压处于截止状态一样高的困难,而在本征MOSFET部件的导通状态开始时突然下降,这是很难解决的。

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