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通过无衬底加热的电子回旋共振氩等离子体增强化学气相沉积法生长的硼原子层掺杂硅薄膜的载流子特性。

Carrier properties of B atomic-layer-doped Si films grown by ECR Ar plasma-enhanced CVD without substrate heating.

作者信息

Sakuraba Masao, Sugawara Katsutoshi, Nosaka Takayuki, Akima Hisanao, Sato Shigeo

机构信息

Laboratory for Nanoelectronics and Spintronics, Research Institute of Electrical Communication, Tohoku University, Sendai, Japan.

出版信息

Sci Technol Adv Mater. 2017 Apr 27;18(1):294-306. doi: 10.1080/14686996.2017.1312520. eCollection 2017.

DOI:10.1080/14686996.2017.1312520
PMID:28567175
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC5439406/
Abstract

The atomic-layer (AL) doping technique in epitaxy has attracted attention as a low-resistive ultrathin semiconductor film as well as a two-dimensional (2-D) carrier transport system. In this paper, we report carrier properties for B AL-doped Si films with suppressed thermal diffusion. B AL-doped Si films were formed on Si(100) by B AL formation followed by Si cap layer deposition in low-energy Ar plasma-enhanced chemical-vapor deposition without substrate heating. After fabrication of Hall-effect devices with the B AL-doped Si films on unstrained and 0.8%-tensile-strained Si(100)-on-insulator substrates (maximum process temperature 350°C), carrier properties were electrically measured at room temperature. Typically for the initial B amount of 2 × 10 cm and 7 × 10 cm, B concentration depth profiles showed a clear decay slope as steep as 1.3 nm/decade. Dominant carrier was a hole and the maximum sheet carrier densities as high as 4 × 10 cm and 2 × 10 cm (electrical activity ratio of about 7% and 3.5%) were measured respectively for the unstrained and 0.8%-tensile-strained Si with Hall mobility around 10-13 cm V s. Moreover, mobility degradation was not observed even when sheet carrier density was increased by heat treatment at 500-700 °C. There is a possibility that the local carrier (ionized B atom) concentration around the B AL in Si reaches around 10 cm and 2-D impurity-band formation with strong Coulomb interaction is expected. The behavior of carrier properties for heat treatment at 500-700 °C implies that thermal diffusion causes broadening of the B AL in Si and decrease of local B concentration.

摘要

外延中的原子层(AL)掺杂技术作为一种低电阻超薄半导体薄膜以及二维(2-D)载流子传输系统已受到关注。在本文中,我们报告了具有抑制热扩散的B原子层掺杂Si薄膜的载流子特性。通过在低能Ar等离子体增强化学气相沉积中形成B原子层然后沉积Si帽层,在不进行衬底加热的情况下,在Si(100)上形成了B原子层掺杂的Si薄膜。在未应变和0.8%拉伸应变的绝缘体上硅(Si(100)-on-insulator)衬底(最高工艺温度350°C)上制备了具有B原子层掺杂Si薄膜的霍尔效应器件后,在室温下对载流子特性进行了电学测量。对于初始B量为2×10¹⁹cm⁻³和7×10¹⁹cm⁻³的情况,B浓度深度分布显示出明显的衰减斜率,陡至1.3nm/十倍程。主导载流子为空穴,对于未应变和0.8%拉伸应变的Si,分别测量到高达4×10¹³cm⁻²和2×10¹³cm⁻²的最大面载流子密度(电学活性比约为7%和3.5%),霍尔迁移率约为10⁻¹³cm²V⁻¹s。此外,即使通过在500 - 700°C下热处理增加面载流子密度,也未观察到迁移率退化。Si中B原子层周围的局部载流子(电离B原子)浓度有可能达到约10²¹cm⁻³,预计会形成具有强库仑相互作用的二维杂质带。在500 - 700°C下热处理时载流子特性的行为表明,热扩散会导致Si中B原子层变宽以及局部B浓度降低。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/678e/5439406/e2e96c5801e5/tsta_a_1312520_f0012_oc.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/678e/5439406/719e0e790e7f/tsta_a_1312520_uf0001_oc.jpg
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https://cdn.ncbi.nlm.nih.gov/pmc/blobs/678e/5439406/b3cf87886cc1/tsta_a_1312520_f0007_oc.jpg
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https://cdn.ncbi.nlm.nih.gov/pmc/blobs/678e/5439406/05216a10e0b9/tsta_a_1312520_f0010_oc.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/678e/5439406/21f243d4ba6f/tsta_a_1312520_f0011_oc.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/678e/5439406/e2e96c5801e5/tsta_a_1312520_f0012_oc.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/678e/5439406/719e0e790e7f/tsta_a_1312520_uf0001_oc.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/678e/5439406/edf4a0fc683d/tsta_a_1312520_f0001_oc.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/678e/5439406/9c8ea7fff828/tsta_a_1312520_f0002_oc.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/678e/5439406/5714376376d0/tsta_a_1312520_f0003_oc.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/678e/5439406/1af502f9c3c2/tsta_a_1312520_f0004_oc.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/678e/5439406/538bc939d26e/tsta_a_1312520_f0005_oc.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/678e/5439406/dae1b4c39122/tsta_a_1312520_f0006_oc.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/678e/5439406/b3cf87886cc1/tsta_a_1312520_f0007_oc.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/678e/5439406/cc09a50e25f9/tsta_a_1312520_f0008_oc.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/678e/5439406/2bac44824e8d/tsta_a_1312520_f0009_oc.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/678e/5439406/05216a10e0b9/tsta_a_1312520_f0010_oc.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/678e/5439406/21f243d4ba6f/tsta_a_1312520_f0011_oc.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/678e/5439406/e2e96c5801e5/tsta_a_1312520_f0012_oc.jpg

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