Transparent conductive properties of TiON thin films
Titanium oxynitride (TiON) thin films were deposited on glass substrates by reactive sputtering of a Ti target under a flow of O2 and N2 gases. When the total number of O and N atoms bonded to Ti was small, the TiON films took on a nano-crystalline fcc structure primarily oriented toward the (200) d...
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Veröffentlicht in: | Journal of vacuum science & technology. A, Vacuum, surfaces, and films Vacuum, surfaces, and films, 2022-01, Vol.40 (1) |
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description | Titanium oxynitride (TiON) thin films were deposited on glass substrates by reactive sputtering of a Ti target under a flow of O2 and N2 gases. When the total number of O and N atoms bonded to Ti was small, the TiON films took on a nano-crystalline fcc structure primarily oriented toward the (200) direction. As the TiON films became more oxidized and/or nitrided, they gradually transformed into an amorphous state with their carrier concentration being between 1018 and 1019 cm−3. The efficiency of oxidization was six times higher than that of nitridation. The optical transmittance of TiON films deposited at RT under sufficient O2 and N2 flow rates reached 100% at wavelengths longer than 1000 nm. However, complete termination of Ti with N atoms failed to occur at low O2 flow rates even when the N2 flow rate was increased. The carrier concentration (n) of the TiON films could be varied in a wide range between 1018 and 3 × 1021 cm−3. The n (×10−19 cm−3) versus Hall mobility (μ) (cm2 V−1 s−1) plot scaled as log μ = 1.23 − 0.38⋅log n between 1 × 1018 and 1 × 1020 cm−3. The Hall mobility reached 20–50 cm2 V−1 s−1 at n = 1018 cm−3, which means this film is promising as an amorphous semiconductor. The log–log plot of resistivity (ρ) (mΩ cm) against n scaled as log ρ = 1.74 − 0.87⋅log n. |
doi_str_mv | 10.1116/6.0001434 |
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When the total number of O and N atoms bonded to Ti was small, the TiON films took on a nano-crystalline fcc structure primarily oriented toward the (200) direction. As the TiON films became more oxidized and/or nitrided, they gradually transformed into an amorphous state with their carrier concentration being between 1018 and 1019 cm−3. The efficiency of oxidization was six times higher than that of nitridation. The optical transmittance of TiON films deposited at RT under sufficient O2 and N2 flow rates reached 100% at wavelengths longer than 1000 nm. However, complete termination of Ti with N atoms failed to occur at low O2 flow rates even when the N2 flow rate was increased. The carrier concentration (n) of the TiON films could be varied in a wide range between 1018 and 3 × 1021 cm−3. The n (×10−19 cm−3) versus Hall mobility (μ) (cm2 V−1 s−1) plot scaled as log μ = 1.23 − 0.38⋅log n between 1 × 1018 and 1 × 1020 cm−3. The Hall mobility reached 20–50 cm2 V−1 s−1 at n = 1018 cm−3, which means this film is promising as an amorphous semiconductor. The log–log plot of resistivity (ρ) (mΩ cm) against n scaled as log ρ = 1.74 − 0.87⋅log n.</description><identifier>ISSN: 0734-2101</identifier><identifier>EISSN: 1520-8559</identifier><identifier>DOI: 10.1116/6.0001434</identifier><identifier>CODEN: JVTAD6</identifier><language>eng</language><ispartof>Journal of vacuum science & technology. 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A, Vacuum, surfaces, and films</title><description>Titanium oxynitride (TiON) thin films were deposited on glass substrates by reactive sputtering of a Ti target under a flow of O2 and N2 gases. When the total number of O and N atoms bonded to Ti was small, the TiON films took on a nano-crystalline fcc structure primarily oriented toward the (200) direction. As the TiON films became more oxidized and/or nitrided, they gradually transformed into an amorphous state with their carrier concentration being between 1018 and 1019 cm−3. The efficiency of oxidization was six times higher than that of nitridation. The optical transmittance of TiON films deposited at RT under sufficient O2 and N2 flow rates reached 100% at wavelengths longer than 1000 nm. However, complete termination of Ti with N atoms failed to occur at low O2 flow rates even when the N2 flow rate was increased. The carrier concentration (n) of the TiON films could be varied in a wide range between 1018 and 3 × 1021 cm−3. The n (×10−19 cm−3) versus Hall mobility (μ) (cm2 V−1 s−1) plot scaled as log μ = 1.23 − 0.38⋅log n between 1 × 1018 and 1 × 1020 cm−3. The Hall mobility reached 20–50 cm2 V−1 s−1 at n = 1018 cm−3, which means this film is promising as an amorphous semiconductor. The log–log plot of resistivity (ρ) (mΩ cm) against n scaled as log ρ = 1.74 − 0.87⋅log n.</description><issn>0734-2101</issn><issn>1520-8559</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2022</creationdate><recordtype>article</recordtype><recordid>eNqdz81KAzEYheEgCtbqwjvIVmFqvvxNZilFq1DsZlyHZJJgpJ0MSSx491ZacO_qbB4OvAjdAlkAgHyQC0IIcMbP0AwEJY0SojtHM9Iy3lAgcImuSvk8IEqJnCHeZzOWyWQ_Vjyk0X0NNe49nnKafK7RF5wC7uPmDdePOOIQt7tyjS6C2RZ_c9o5en9-6pcvzXqzel0-rpuBdl1tWuItt9aZYEKwSllFhHC0VZRDxx0XoECCVVIw56lhPnADtBOh84S1Htgc3R1_h5xKyT7oKcedyd8aiP7N1VKfcg_2_mjLEKupMY3_w_uU_6CeXGA_znNiug</recordid><startdate>202201</startdate><enddate>202201</enddate><creator>Akazawa, Housei</creator><scope>AAYXX</scope><scope>CITATION</scope><orcidid>https://orcid.org/0000-0002-9807-8564</orcidid></search><sort><creationdate>202201</creationdate><title>Transparent conductive properties of TiON thin films</title><author>Akazawa, Housei</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c299t-70eb4bbdafaffb88b8055d27824194d4518161b8653de2a3ef4a1295f9e037e13</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2022</creationdate><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Akazawa, Housei</creatorcontrib><collection>CrossRef</collection><jtitle>Journal of vacuum science & technology. A, Vacuum, surfaces, and films</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Akazawa, Housei</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Transparent conductive properties of TiON thin films</atitle><jtitle>Journal of vacuum science & technology. A, Vacuum, surfaces, and films</jtitle><date>2022-01</date><risdate>2022</risdate><volume>40</volume><issue>1</issue><issn>0734-2101</issn><eissn>1520-8559</eissn><coden>JVTAD6</coden><abstract>Titanium oxynitride (TiON) thin films were deposited on glass substrates by reactive sputtering of a Ti target under a flow of O2 and N2 gases. When the total number of O and N atoms bonded to Ti was small, the TiON films took on a nano-crystalline fcc structure primarily oriented toward the (200) direction. As the TiON films became more oxidized and/or nitrided, they gradually transformed into an amorphous state with their carrier concentration being between 1018 and 1019 cm−3. The efficiency of oxidization was six times higher than that of nitridation. The optical transmittance of TiON films deposited at RT under sufficient O2 and N2 flow rates reached 100% at wavelengths longer than 1000 nm. However, complete termination of Ti with N atoms failed to occur at low O2 flow rates even when the N2 flow rate was increased. The carrier concentration (n) of the TiON films could be varied in a wide range between 1018 and 3 × 1021 cm−3. The n (×10−19 cm−3) versus Hall mobility (μ) (cm2 V−1 s−1) plot scaled as log μ = 1.23 − 0.38⋅log n between 1 × 1018 and 1 × 1020 cm−3. The Hall mobility reached 20–50 cm2 V−1 s−1 at n = 1018 cm−3, which means this film is promising as an amorphous semiconductor. The log–log plot of resistivity (ρ) (mΩ cm) against n scaled as log ρ = 1.74 − 0.87⋅log n.</abstract><doi>10.1116/6.0001434</doi><tpages>9</tpages><orcidid>https://orcid.org/0000-0002-9807-8564</orcidid></addata></record> |
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title | Transparent conductive properties of TiON thin films |
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