Electrical properties of neodymium oxide/titanium dioxide and neodymium oxide/gadolinium silicate dielectric gate stack on silicon substrate
The problem with using single layer of high dielectric constant materials is the interfacial layer growth during thermal process of fabrication. The purpose of studying bilayer dielectric gate stack is because single layer can lead to interfacial layer growth during thermal process of fabrication....
Saved in:
Main Author: | |
---|---|
Other Authors: | |
Format: | Final Year Project |
Language: | English |
Published: |
2012
|
Subjects: | |
Online Access: | http://hdl.handle.net/10356/48413 |
Tags: |
Add Tag
No Tags, Be the first to tag this record!
|
Institution: | Nanyang Technological University |
Language: | English |
id |
sg-ntu-dr.10356-48413 |
---|---|
record_format |
dspace |
spelling |
sg-ntu-dr.10356-484132023-03-04T15:42:05Z Electrical properties of neodymium oxide/titanium dioxide and neodymium oxide/gadolinium silicate dielectric gate stack on silicon substrate Lee, Vivian Sing Zhi. Alfred Tok Iing Yoong School of Materials Science and Engineering DRNTU::Engineering::Materials::Microelectronics and semiconductor materials The problem with using single layer of high dielectric constant materials is the interfacial layer growth during thermal process of fabrication. The purpose of studying bilayer dielectric gate stack is because single layer can lead to interfacial layer growth during thermal process of fabrication. Neodymium oxide will be deposited on Silicon substrate first by Pulsed laser deposition. Gadolinium silicate and Titanium dioxide will then be deposited on top of Neodymium oxide separately by Atomic layer deposition. Two different combinations dielectric gate stack are then formed: Neodymium oxide/ Titanium dioxide (Sample A) and Neodymium oxide/ Gadolinium silicate (Sample B). The thickness of each dielectric gate stack is approximately 6nm. Crystal structure of Neodymium oxide and Titanium dioxide film crystallize upon annealing, while Gadolinium silicate remains amorphous. The RMS for Sample A is approximately 0.666nm and Sample B is approximately 0.864nm. The dielectric constant of Sample A is approximately 11.9 and Sample B is 8.68. The leakage current density at -1V for Sample A is approximately 1.6x10-1 A/cm2.and Sample B is approximately 1.6x10-2 A/cm2. Result shows that, Sample A offers higher dielectric constant but higher leakage current density due to the crystallization of the Titanium dioxide film during annealing. While Sample B offers lower leakage current density but lower dielectric constant due to the silicate formation as silyl-amide based precursor was used. Bachelor of Engineering (Materials Engineering) 2012-04-17T06:56:40Z 2012-04-17T06:56:40Z 2012 2012 Final Year Project (FYP) http://hdl.handle.net/10356/48413 en Nanyang Technological University 38 p. application/pdf |
institution |
Nanyang Technological University |
building |
NTU Library |
continent |
Asia |
country |
Singapore Singapore |
content_provider |
NTU Library |
collection |
DR-NTU |
language |
English |
topic |
DRNTU::Engineering::Materials::Microelectronics and semiconductor materials |
spellingShingle |
DRNTU::Engineering::Materials::Microelectronics and semiconductor materials Lee, Vivian Sing Zhi. Electrical properties of neodymium oxide/titanium dioxide and neodymium oxide/gadolinium silicate dielectric gate stack on silicon substrate |
description |
The problem with using single layer of high dielectric constant materials is the interfacial layer growth during thermal process of fabrication. The purpose of studying bilayer dielectric gate stack is because single layer can lead to interfacial layer growth during thermal process of fabrication.
Neodymium oxide will be deposited on Silicon substrate first by Pulsed laser deposition. Gadolinium silicate and Titanium dioxide will then be deposited on top of Neodymium oxide separately by Atomic layer deposition. Two different combinations dielectric gate stack are then formed: Neodymium oxide/ Titanium dioxide (Sample A) and Neodymium oxide/ Gadolinium silicate (Sample B).
The thickness of each dielectric gate stack is approximately 6nm. Crystal structure of Neodymium oxide and Titanium dioxide film crystallize upon annealing, while Gadolinium silicate remains amorphous. The RMS for Sample A is approximately 0.666nm and Sample B is approximately 0.864nm. The dielectric constant of Sample A is approximately 11.9 and Sample B is 8.68. The leakage current density at -1V for Sample A is approximately 1.6x10-1 A/cm2.and Sample B is approximately 1.6x10-2 A/cm2.
Result shows that, Sample A offers higher dielectric constant but higher leakage current density due to the crystallization of the Titanium dioxide film during annealing. While Sample B offers lower leakage current density but lower dielectric constant due to the silicate formation as silyl-amide based precursor was used. |
author2 |
Alfred Tok Iing Yoong |
author_facet |
Alfred Tok Iing Yoong Lee, Vivian Sing Zhi. |
format |
Final Year Project |
author |
Lee, Vivian Sing Zhi. |
author_sort |
Lee, Vivian Sing Zhi. |
title |
Electrical properties of neodymium oxide/titanium dioxide and neodymium oxide/gadolinium silicate dielectric gate stack on silicon substrate |
title_short |
Electrical properties of neodymium oxide/titanium dioxide and neodymium oxide/gadolinium silicate dielectric gate stack on silicon substrate |
title_full |
Electrical properties of neodymium oxide/titanium dioxide and neodymium oxide/gadolinium silicate dielectric gate stack on silicon substrate |
title_fullStr |
Electrical properties of neodymium oxide/titanium dioxide and neodymium oxide/gadolinium silicate dielectric gate stack on silicon substrate |
title_full_unstemmed |
Electrical properties of neodymium oxide/titanium dioxide and neodymium oxide/gadolinium silicate dielectric gate stack on silicon substrate |
title_sort |
electrical properties of neodymium oxide/titanium dioxide and neodymium oxide/gadolinium silicate dielectric gate stack on silicon substrate |
publishDate |
2012 |
url |
http://hdl.handle.net/10356/48413 |
_version_ |
1759858321974624256 |