Nitrogen doped ZnO thin films prepared by anode layer ion source reactive ion beam sputter deposition

碩士 === 國立臺灣科技大學 === 電子工程系 === 100 === Nitrogen doped ZnO (ZnO:N) thin films have been deposited by reactive ion beam sputter deposition utilizing an anode layer ion source. Both argon and nitrogen were passed simultaneously through the ion source to act as sputtering and reactive ion species, respe...

Full description

Bibliographic Details
Main Authors: Han-chen Peng, 彭翰晨
Other Authors: Liang-chiun Chao
Format: Others
Language:zh-TW
Published: 2012
Online Access:http://ndltd.ncl.edu.tw/handle/qtya6e
id ndltd-TW-100NTUS5428036
record_format oai_dc
spelling ndltd-TW-100NTUS54280362019-05-15T20:43:22Z http://ndltd.ncl.edu.tw/handle/qtya6e Nitrogen doped ZnO thin films prepared by anode layer ion source reactive ion beam sputter deposition 陽極層離子源反應式濺鍍沉積摻氮氧化鋅薄膜之特性 Han-chen Peng 彭翰晨 碩士 國立臺灣科技大學 電子工程系 100 Nitrogen doped ZnO (ZnO:N) thin films have been deposited by reactive ion beam sputter deposition utilizing an anode layer ion source. Both argon and nitrogen were passed simultaneously through the ion source to act as sputtering and reactive ion species, respectively. The plasma spectrum of the anode layer ion source shows distinctive atomic nitrogen emission lines suggesting that the incorporation of atomic nitrogen into ZnO may be improved. Experimental results show that all the film exhibit a preferred orientation along the (002) direction. A 20 nm un-doped ZnO was first deposited at 200?aC and subsequently annealed at 700?aC to act as buffer layers. Higher annealing temperature causes decomposition of the ZnO film and results in increased deep level green emission. ZnO:N was deposited on the buffer layer at 25 ~ 300?aC. Micro-Raman spectroscopy analysis shows Raman peaks at 275 and 582 cm-1, which is due to the local vibration mode of nitrogen in ZnO. All the nitrogen doped ZnO exhibit n-type conductivity. Conversion from n-type to p-type was not observed regardless of nitrogen flow rates or post-growth annealing. This is likely due to the formation of molecular nitrogen occupying oxygen sites (N2)O that act as double donors. Variable temperature Hall effect measurement shows that at temperatures above 165 K, the transport is governed by thermally activated carriers. The activation energy for conduction in this temperature range is 73 meV. The bandgap of ZnO:N is 3.158 eV, while the transmittance is larger than 80% in the visible region. Liang-chiun Chao 趙良君 2012 學位論文 ; thesis 70 zh-TW
collection NDLTD
language zh-TW
format Others
sources NDLTD
description 碩士 === 國立臺灣科技大學 === 電子工程系 === 100 === Nitrogen doped ZnO (ZnO:N) thin films have been deposited by reactive ion beam sputter deposition utilizing an anode layer ion source. Both argon and nitrogen were passed simultaneously through the ion source to act as sputtering and reactive ion species, respectively. The plasma spectrum of the anode layer ion source shows distinctive atomic nitrogen emission lines suggesting that the incorporation of atomic nitrogen into ZnO may be improved. Experimental results show that all the film exhibit a preferred orientation along the (002) direction. A 20 nm un-doped ZnO was first deposited at 200?aC and subsequently annealed at 700?aC to act as buffer layers. Higher annealing temperature causes decomposition of the ZnO film and results in increased deep level green emission. ZnO:N was deposited on the buffer layer at 25 ~ 300?aC. Micro-Raman spectroscopy analysis shows Raman peaks at 275 and 582 cm-1, which is due to the local vibration mode of nitrogen in ZnO. All the nitrogen doped ZnO exhibit n-type conductivity. Conversion from n-type to p-type was not observed regardless of nitrogen flow rates or post-growth annealing. This is likely due to the formation of molecular nitrogen occupying oxygen sites (N2)O that act as double donors. Variable temperature Hall effect measurement shows that at temperatures above 165 K, the transport is governed by thermally activated carriers. The activation energy for conduction in this temperature range is 73 meV. The bandgap of ZnO:N is 3.158 eV, while the transmittance is larger than 80% in the visible region.
author2 Liang-chiun Chao
author_facet Liang-chiun Chao
Han-chen Peng
彭翰晨
author Han-chen Peng
彭翰晨
spellingShingle Han-chen Peng
彭翰晨
Nitrogen doped ZnO thin films prepared by anode layer ion source reactive ion beam sputter deposition
author_sort Han-chen Peng
title Nitrogen doped ZnO thin films prepared by anode layer ion source reactive ion beam sputter deposition
title_short Nitrogen doped ZnO thin films prepared by anode layer ion source reactive ion beam sputter deposition
title_full Nitrogen doped ZnO thin films prepared by anode layer ion source reactive ion beam sputter deposition
title_fullStr Nitrogen doped ZnO thin films prepared by anode layer ion source reactive ion beam sputter deposition
title_full_unstemmed Nitrogen doped ZnO thin films prepared by anode layer ion source reactive ion beam sputter deposition
title_sort nitrogen doped zno thin films prepared by anode layer ion source reactive ion beam sputter deposition
publishDate 2012
url http://ndltd.ncl.edu.tw/handle/qtya6e
work_keys_str_mv AT hanchenpeng nitrogendopedznothinfilmspreparedbyanodelayerionsourcereactiveionbeamsputterdeposition
AT pénghànchén nitrogendopedznothinfilmspreparedbyanodelayerionsourcereactiveionbeamsputterdeposition
AT hanchenpeng yángjícénglíziyuánfǎnyīngshìjiàndùchénjīcàndànyǎnghuàxīnbáomózhītèxìng
AT pénghànchén yángjícénglíziyuánfǎnyīngshìjiàndùchénjīcàndànyǎnghuàxīnbáomózhītèxìng
_version_ 1719104717869547520