Crystal Structure And Optical Properties Of TiO2 Thin Films Prepared By Reactive RF Magnetron Sputtering
In sputtering deposition process of TiO2, metal Ti or sintered TiO2 target is used as deposition source. In this study, we have compared the characteristic of target materials. When TiO2 target was used, stoichiometric TiO2 films was deposited under the Ar atmosphere containing 1.0% of oxygen. The h...
Main Authors: | , , , |
---|---|
Format: | Article |
Language: | English |
Published: |
Polish Academy of Sciences
2015-06-01
|
Series: | Archives of Metallurgy and Materials |
Subjects: | |
Online Access: | http://www.degruyter.com/view/j/amm.2015.60.issue-2/amm-2015-0240/amm-2015-0240.xml?format=INT |
_version_ | 1811285929851092992 |
---|---|
author | Goto S. Adachi Y. Matsuda K. Nose M. |
author_facet | Goto S. Adachi Y. Matsuda K. Nose M. |
author_sort | Goto S. |
collection | DOAJ |
description | In sputtering deposition process of TiO2, metal Ti or sintered TiO2 target is used as deposition source. In this study, we have compared the characteristic of target materials. When TiO2 target was used, stoichiometric TiO2 films was deposited under the Ar atmosphere containing 1.0% of oxygen. The highest sputtering rate under this atmosphere was 3.9nm/min at 3.4W/cm2. But, sintered TiO2 target is fragile and cannot endure higher density of input power than 3.4W/cm2. On the other hand, Ti target needs higher oxygen concentration (8%) in sputtering gas atmosphere for obtaining rutile/anatase. Even though Ti target can be input twice power density of 7.9W/cm2, the highest deposition rate for Ti target was 1.4/nm, which was ~35% of the highest rate for TiO2 target. Then we have study out the composite target consisting of Ti plate and TiO2 chips. Using the composite target, stoichiometric TiO2 films were prepared in the rate of 9.6nm/min at 6.8 W/cm2 under the atmosphere of Ar/2.5%O2. Furthermore, we have found that the TiO2 films obtained from the composite target consisted of about 100% anatase, whereas TiO2 films obtained from other target have rutile dominant structure. The optical band gap energy of the film is determined by using the Tauc plot. The calculated band gap energies for the films deposited by Ti target and composite target were 2.95 and 3.24eV, which are equivalent to that of rutile and anatase structure, respectively. |
first_indexed | 2024-04-13T02:51:07Z |
format | Article |
id | doaj.art-3bb931919d944f698a5fc64be090aa84 |
institution | Directory Open Access Journal |
issn | 2300-1909 |
language | English |
last_indexed | 2024-04-13T02:51:07Z |
publishDate | 2015-06-01 |
publisher | Polish Academy of Sciences |
record_format | Article |
series | Archives of Metallurgy and Materials |
spelling | doaj.art-3bb931919d944f698a5fc64be090aa842022-12-22T03:05:50ZengPolish Academy of SciencesArchives of Metallurgy and Materials2300-19092015-06-0160296596710.1515/amm-2015-0240amm-2015-0240Crystal Structure And Optical Properties Of TiO2 Thin Films Prepared By Reactive RF Magnetron SputteringGoto S.0Adachi Y.1Matsuda K.2Nose M.3 GRADUATE SCHOOL OF SCIENCE AND ENGINEERING FOR EDUCATION, UNIVERSITY OF TOYAMA, 3190, GOFUKU, TOYAMA, JAPAN GRADUATE SCHOOL OF SCIENCE AND ENGINEERING FOR EDUCATION, UNIVERSITY OF TOYAMA, 3190, GOFUKU, TOYAMA, JAPAN GRADUATE SCHOOL OF SCIENCE AND ENGINEERING FOR RESEARCH, UNIVERSITY OF TOYAMA, 3190, GOFUKU, TOYAMA, JAPAN FACULTY OF ART AND DESIGN, UNIVERSITY OF TOYAMA, TAKAOKA 933-8588, JAPANIn sputtering deposition process of TiO2, metal Ti or sintered TiO2 target is used as deposition source. In this study, we have compared the characteristic of target materials. When TiO2 target was used, stoichiometric TiO2 films was deposited under the Ar atmosphere containing 1.0% of oxygen. The highest sputtering rate under this atmosphere was 3.9nm/min at 3.4W/cm2. But, sintered TiO2 target is fragile and cannot endure higher density of input power than 3.4W/cm2. On the other hand, Ti target needs higher oxygen concentration (8%) in sputtering gas atmosphere for obtaining rutile/anatase. Even though Ti target can be input twice power density of 7.9W/cm2, the highest deposition rate for Ti target was 1.4/nm, which was ~35% of the highest rate for TiO2 target. Then we have study out the composite target consisting of Ti plate and TiO2 chips. Using the composite target, stoichiometric TiO2 films were prepared in the rate of 9.6nm/min at 6.8 W/cm2 under the atmosphere of Ar/2.5%O2. Furthermore, we have found that the TiO2 films obtained from the composite target consisted of about 100% anatase, whereas TiO2 films obtained from other target have rutile dominant structure. The optical band gap energy of the film is determined by using the Tauc plot. The calculated band gap energies for the films deposited by Ti target and composite target were 2.95 and 3.24eV, which are equivalent to that of rutile and anatase structure, respectively.http://www.degruyter.com/view/j/amm.2015.60.issue-2/amm-2015-0240/amm-2015-0240.xml?format=INTTiO2RutileAnatasesputteringXRD |
spellingShingle | Goto S. Adachi Y. Matsuda K. Nose M. Crystal Structure And Optical Properties Of TiO2 Thin Films Prepared By Reactive RF Magnetron Sputtering Archives of Metallurgy and Materials TiO2 Rutile Anatase sputtering XRD |
title | Crystal Structure And Optical Properties Of TiO2 Thin Films Prepared By Reactive RF Magnetron Sputtering |
title_full | Crystal Structure And Optical Properties Of TiO2 Thin Films Prepared By Reactive RF Magnetron Sputtering |
title_fullStr | Crystal Structure And Optical Properties Of TiO2 Thin Films Prepared By Reactive RF Magnetron Sputtering |
title_full_unstemmed | Crystal Structure And Optical Properties Of TiO2 Thin Films Prepared By Reactive RF Magnetron Sputtering |
title_short | Crystal Structure And Optical Properties Of TiO2 Thin Films Prepared By Reactive RF Magnetron Sputtering |
title_sort | crystal structure and optical properties of tio2 thin films prepared by reactive rf magnetron sputtering |
topic | TiO2 Rutile Anatase sputtering XRD |
url | http://www.degruyter.com/view/j/amm.2015.60.issue-2/amm-2015-0240/amm-2015-0240.xml?format=INT |
work_keys_str_mv | AT gotos crystalstructureandopticalpropertiesoftio2thinfilmspreparedbyreactiverfmagnetronsputtering AT adachiy crystalstructureandopticalpropertiesoftio2thinfilmspreparedbyreactiverfmagnetronsputtering AT matsudak crystalstructureandopticalpropertiesoftio2thinfilmspreparedbyreactiverfmagnetronsputtering AT nosem crystalstructureandopticalpropertiesoftio2thinfilmspreparedbyreactiverfmagnetronsputtering |