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具有氧化铪-氧化铝纳米层的硅SIS结构中的类二极管电流泄漏和铁电开关

Diode-Like Current Leakage and Ferroelectric Switching in Silicon SIS Structures with Hafnia-Alumina Nanolaminates.

作者信息

Popov Vladimir P, Tikhonenko Fedor V, Antonov Valentin A, Tyschenko Ida E, Miakonkikh Andrey V, Simakin Sergey G, Rudenko Konstantin V

机构信息

Rzhanov Institute of Semiconductor Physics SB RAS, 630090 Novosibirsk, Russia.

Valiev Institute of Physics and Technology RAS, 117218 Moscow, Russia.

出版信息

Nanomaterials (Basel). 2021 Jan 22;11(2):291. doi: 10.3390/nano11020291.

DOI:10.3390/nano11020291
PMID:33499413
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC7912112/
Abstract

Silicon semiconductor-insulator-semiconductor (SIS) structures with high-k dielectrics are a promising new material for photonic and CMOS integrations. The "diode-like" currents through the symmetric atomic layer deposited (ALD) HfO/AlO/HfO… nanolayers with a highest rectification coefficient 10 are observed and explained by the asymmetry of the upper and lower heterointerfaces formed by bonding and ALD processes. As a result, different spatial charge regions (SCRs) are formed on both insulator sides. The lowest leakages are observed through the stacks, with total AlO thickness values of 8-10 nm, which also provide a diffusive barrier for hydrogen. The dominant mechanism of electron transport through the built-in insulator at the weak field E < 1 MV/cm is thermionic emission. The Poole-Frenkel (PF) mechanism of emission from traps dominates at larger E values. The charge carriers mobility 100-120 cm/(V s) and interface states (IFS) density 1.2 × 10 cm are obtained for the n-p SIS structures with insulator HfO:AlO (10:1) after rapid thermal annealing (RTA) at 800 °C. The drain current hysteresis of pseudo-metal-oxide-semiconductor field effect transistor (MOSFET) with the memory window 1.2-1.3 V at the gate voltage |V| < ±2.5 V is maintained in the RTA treatment at T = 800-900 °C for these transistors.

摘要

具有高介电常数电介质的硅半导体-绝缘体-半导体(SIS)结构是用于光子和CMOS集成的一种很有前景的新型材料。通过对称原子层沉积(ALD)的HfO/AlO/HfO…纳米层观察到了“类二极管”电流,其最高整流系数为10,并通过键合和ALD工艺形成的上下异质界面的不对称性进行了解释。结果,在绝缘体两侧形成了不同的空间电荷区(SCR)。通过总AlO厚度值为8 - 10 nm的堆叠结构观察到最低泄漏电流,这也为氢提供了扩散阻挡层。在弱场E < 1 MV/cm时,电子通过内置绝缘体传输的主要机制是热电子发射。在较大E值时,陷阱发射的普尔-弗伦克尔(PF)机制占主导。对于在800°C进行快速热退火(RTA)后的具有绝缘体HfO:AlO(10:1)的n-p SIS结构,获得了载流子迁移率100 - 120 cm²/(V·s)和界面态(IFS)密度1.2×10¹² cm⁻²。对于这些晶体管,在800 - 900°C的RTA处理中,在栅极电压|V| < ±2.5 V时,具有1.2 - 1.3 V记忆窗口的伪金属氧化物半导体场效应晶体管(MOSFET)的漏极电流滞后得以保持。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2b50/7912112/20c3aee12886/nanomaterials-11-00291-g009.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2b50/7912112/23ec3208c371/nanomaterials-11-00291-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2b50/7912112/b35a7bb7ac76/nanomaterials-11-00291-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2b50/7912112/8d363ee26d73/nanomaterials-11-00291-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2b50/7912112/cfb9ae7cdae7/nanomaterials-11-00291-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2b50/7912112/353236571288/nanomaterials-11-00291-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2b50/7912112/6b4520df0088/nanomaterials-11-00291-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2b50/7912112/90b2ce5c41e6/nanomaterials-11-00291-g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2b50/7912112/1282dcdc0e02/nanomaterials-11-00291-g008.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2b50/7912112/20c3aee12886/nanomaterials-11-00291-g009.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2b50/7912112/23ec3208c371/nanomaterials-11-00291-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2b50/7912112/b35a7bb7ac76/nanomaterials-11-00291-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2b50/7912112/8d363ee26d73/nanomaterials-11-00291-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2b50/7912112/cfb9ae7cdae7/nanomaterials-11-00291-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2b50/7912112/353236571288/nanomaterials-11-00291-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2b50/7912112/6b4520df0088/nanomaterials-11-00291-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2b50/7912112/90b2ce5c41e6/nanomaterials-11-00291-g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2b50/7912112/1282dcdc0e02/nanomaterials-11-00291-g008.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2b50/7912112/20c3aee12886/nanomaterials-11-00291-g009.jpg

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