Development of /spl delta/B/i-Si//spl delta/Sb and /spl delta/B/i-Si//spl delta/Sb/i-Si//spl delta/B resonant interband tunnel diodes for integrated circuit applications
S. Rommel, Niu Jin, T. Dillon, S. Di Giacomo, J. Banyai, B. Cord, C. D'Imperio, D. J. Hancock, N. Kirpalani, V. Emanuele, P. R. Berger, P. Thompson, K. Hobart, R. Lake
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引用次数: 1
Abstract
Recent developments in Si based tunnel diode technologies have made the realization of circuits incorporating both tunnel diodes and transistors feasible. A recent study by the authors presented the design of an n-on-p Si RITD layer with a peak-to-valley current ratio (PVCR) of 2.15 at a current density of 3 kA/cm/sup 2/ which was grown by molecular beam epitaxy (MBE) (Thompson et al, Appl. Phys. Lett. vol. 75, pp. 1308-1310, 1999). Further studies of this structure investigated additional tunnel barrier thicknesses of 4 nm, 8 nm, and 10 nm. In all samples, room temperature NDR was observed comparable to that of the baseline 6 nm RITD. Simple adjustments to the tunnel barrier thickness can be made to tailor the performance for a particular circuit application. However, growth of a complimentary p-on-n tunnel diode is problematic due to Sb segregation through the intrinsic tunneling spacer. The solution is to control the Sb segregation by employing multiple substrate temperatures during MBE growth. Following the success of the complementary p-on-n growth strategy, it was now possible to demonstrate the integration of two tunnel diodes in a single growth. The basic flow and design presented here follow that of III-V RITDs (Yang et al, 1995), presenting a symmetric pnp RITD structure. The motivation for developing this structure was to mimic the I-V characteristic of III-V RITDs which have NDR regions under forward and reverse bias. A Si-based structure with these properties would facilitate the development of a Goto-type memory cell (Goto et al, 1960).
基于硅的隧道二极管技术的最新发展使得隧道二极管和晶体管集成电路的实现成为可能。作者最近的一项研究提出了一种n-on-p Si RITD层的设计,其峰谷电流比(PVCR)为2.15,电流密度为3 kA/cm/sup 2/,该层是通过分子束外延(MBE)生长的(Thompson等,苹果)。理论物理。列托人。第75卷,第1308-1310页,1999年)。对该结构的进一步研究考察了额外的4 nm、8 nm和10 nm的隧道势垒厚度。在所有样品中,观察到的室温NDR与基线6 nm RITD相当。对隧道阻挡层厚度的简单调整可以为特定的电路应用量身定制性能。然而,互补的p-on-n隧道二极管的生长是有问题的,因为Sb通过固有的隧道间隔隔离。解决方案是通过在MBE生长过程中采用多种衬底温度来控制Sb偏析。在互补p-on-n增长战略取得成功之后,现在有可能在单一增长中展示两个隧道二极管的集成。本文介绍的基本流程和设计遵循III-V型RITD (Yang et al ., 1995),呈现对称的pnp RITD结构。开发这种结构的动机是模仿在正向和反向偏置下具有NDR区域的III-V型ritd的I-V特征。具有这些特性的硅基结构将促进Goto型记忆细胞的发展(Goto等人,1960)。