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硅纳米线晶体管中电离杂质散射对总迁移率影响的模拟

Simulation of the Impact of Ionized Impurity Scattering on the Total Mobility in Si Nanowire Transistors.

作者信息

Sadi Toufik, Medina-Bailon Cristina, Nedjalkov Mihail, Lee Jaehyun, Badami Oves, Berrada Salim, Carrillo-Nunez Hamilton, Georgiev Vihar, Selberherr Siegfried, Asenov Asen

机构信息

Engineered Nanosystems Group, Department of Neuroscience and Biomedical Engineering, School of Science, Aalto University, P.O. Box 12200, FI-00076 Aalto, Finland.

Device Modelling Group, School of Engineering, University of Glasgow, Glasgow G12 8LT, Scotland, UK.

出版信息

Materials (Basel). 2019 Jan 2;12(1):124. doi: 10.3390/ma12010124.

Abstract

Nanowire transistors (NWTs) are being considered as possible candidates for replacing FinFETs, especially for CMOS scaling beyond the 5-nm node, due to their better electrostatic integrity. Hence, there is an urgent need to develop reliable simulation methods to provide deeper insight into NWTs' physics and operation, and unlock the devices' technological potential. One simulation approach that delivers reliable mobility values at low-field near-equilibrium conditions is the combination of the quantum confinement effects with the semi-classical Boltzmann transport equation, solved within the relaxation time approximation adopting the Kubo⁻Greenwood (KG) formalism, as implemented in this work. We consider the most relevant scattering mechanisms governing intraband and multi-subband transitions in NWTs, including phonon, surface roughness and ionized impurity scattering, whose rates have been calculated directly from the Fermi's Golden rule. In this paper, we couple multi-slice Poisson⁻Schrödinger solutions to the KG method to analyze the impact of various scattering mechanisms on the mobility of small diameter nanowire transistors. As demonstrated here, phonon and surface roughness scattering are strong mobility-limiting mechanisms in NWTs. However, scattering from ionized impurities has proved to be another important mobility-limiting mechanism, being mandatory for inclusion when simulating realistic and doped nanostructures, due to the short range Coulomb interaction with the carriers. We also illustrate the impact of the nanowire geometry, highlighting the advantage of using circular over square cross section shapes.

摘要

纳米线晶体管(NWTs)因其更好的静电完整性,正被视为取代鳍式场效应晶体管(FinFETs)的可能候选者,特别是对于5纳米节点以下的CMOS缩放。因此,迫切需要开发可靠的模拟方法,以更深入地了解NWTs的物理特性和工作原理,并释放这些器件的技术潜力。一种在低场近平衡条件下能提供可靠迁移率值的模拟方法是将量子限制效应与半经典玻尔兹曼输运方程相结合,并在采用久保-格林伍德(KG)形式的弛豫时间近似内求解,本工作即采用此方法。我们考虑了控制NWTs带内和多子带跃迁的最相关散射机制,包括声子、表面粗糙度和电离杂质散射,其速率已直接从费米黄金定则计算得出。在本文中,我们将多切片泊松-薛定谔解与KG方法相结合,以分析各种散射机制对小直径纳米线晶体管迁移率的影响。如此处所示,声子和表面粗糙度散射是NWTs中很强的迁移率限制机制。然而,电离杂质散射已被证明是另一种重要的迁移率限制机制,在模拟实际的掺杂纳米结构时,由于与载流子的短程库仑相互作用,必须将其考虑在内。我们还说明了纳米线几何形状的影响,突出了使用圆形横截面形状优于方形的优点。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4e95/6337633/31fe36d42a1e/materials-12-00124-g001.jpg

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