Characteristics of point defects in the green luminescence from Zn- and O-rich ZnO
Cathodoluminescence spectra have been measured to determine the characteristics of ubiquitous green luminescence (GL) in nonstoichiometric zinc oxide (ZnO). Zn- and O-rich ZnO were found to exhibit characteristic emissions at 2.53 eV [full width at half-maximum (FWHM) 340 meV] and 2.30 eV (FWHM 450...
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Veröffentlicht in: | Physical review. B, Condensed matter and materials physics Condensed matter and materials physics, 2012-09, Vol.86 (11), Article 115205 |
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description | Cathodoluminescence spectra have been measured to determine the characteristics of ubiquitous green luminescence (GL) in nonstoichiometric zinc oxide (ZnO). Zn- and O-rich ZnO were found to exhibit characteristic emissions at 2.53 eV [full width at half-maximum (FWHM) 340 meV] and 2.30 eV (FWHM 450 meV), respectively. Hydrogen was used to probe the physical nature of GL centers. The Zn-rich GL is enhanced upon H incorporation, whereas the O-rich GL is completely quenched as its underlying acceptor-like V sub(Zn) centers are passivated by H. The GL emission bands each exhibit remarkably different excitation-power dependencies. The Zn-rich GL follows a close to linear relationship with excitation power, while the O-rich GL exhibits a square-root dependence. Calculations based on bimolecular recombination equations show the defect concentration in Zn-rich ZnO is three orders of magnitude greater than that in O-rich ZnO, indicating V sub(O) is more readily formed than V sub(Zn) in thermochemical treatments of ZnO. |
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B, Condensed matter and materials physics</title><description>Cathodoluminescence spectra have been measured to determine the characteristics of ubiquitous green luminescence (GL) in nonstoichiometric zinc oxide (ZnO). Zn- and O-rich ZnO were found to exhibit characteristic emissions at 2.53 eV [full width at half-maximum (FWHM) 340 meV] and 2.30 eV (FWHM 450 meV), respectively. Hydrogen was used to probe the physical nature of GL centers. The Zn-rich GL is enhanced upon H incorporation, whereas the O-rich GL is completely quenched as its underlying acceptor-like V sub(Zn) centers are passivated by H. The GL emission bands each exhibit remarkably different excitation-power dependencies. The Zn-rich GL follows a close to linear relationship with excitation power, while the O-rich GL exhibits a square-root dependence. Calculations based on bimolecular recombination equations show the defect concentration in Zn-rich ZnO is three orders of magnitude greater than that in O-rich ZnO, indicating V sub(O) is more readily formed than V sub(Zn) in thermochemical treatments of ZnO.</description><subject>Bands</subject><subject>Condensed matter</subject><subject>Excitation</subject><subject>Luminescence</subject><subject>Mathematical analysis</subject><subject>Spectra</subject><subject>Zinc</subject><subject>Zinc oxide</subject><issn>1098-0121</issn><issn>1550-235X</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2012</creationdate><recordtype>article</recordtype><recordid>eNo1kE1LxDAQhoMouK7-AU85eumaNEmTHnXxCxZWFgXxEtJkYiNtuiZdYf-9ldXTO-_wMAwPQpeULCgl7Pq53ecNfN8uVDUtREnEEZpRIUhRMvF2PM2kVgWhJT1FZzl_EkJ5zcsZ2ixbk4wdIYU8Bpvx4PF2CHHEDjzYMeMQ8dgC_kgAEXe7PkTIFqIF7NPQ4_dYYBMdXhcp2Haq63N04k2X4eIv5-j1_u5l-Vis1g9Py5tVYRmvxgIsKNkw4ppSCaKcN9wDgLSkocCZM5JbxVldKlozp6gzjgkmhZcSeNUINkdXh7vbNHztII-6D9NnXWciDLusqSS1ZJJROqHlAbVpyDmB19sUepP2mhL9K1D_C9Sq0geB7AcZFmWb</recordid><startdate>20120910</startdate><enddate>20120910</enddate><creator>Ton-That, C.</creator><creator>Weston, L.</creator><creator>Phillips, M. 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R.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c346t-ece87b30db28508dfa4feee7c0b1e43da74c843928193d81dad35375f77e46b53</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2012</creationdate><topic>Bands</topic><topic>Condensed matter</topic><topic>Excitation</topic><topic>Luminescence</topic><topic>Mathematical analysis</topic><topic>Spectra</topic><topic>Zinc</topic><topic>Zinc oxide</topic><toplevel>online_resources</toplevel><creatorcontrib>Ton-That, C.</creatorcontrib><creatorcontrib>Weston, L.</creatorcontrib><creatorcontrib>Phillips, M. R.</creatorcontrib><collection>CrossRef</collection><collection>Engineered Materials Abstracts</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>METADEX</collection><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Materials Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Physical review. B, Condensed matter and materials physics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Ton-That, C.</au><au>Weston, L.</au><au>Phillips, M. R.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Characteristics of point defects in the green luminescence from Zn- and O-rich ZnO</atitle><jtitle>Physical review. B, Condensed matter and materials physics</jtitle><date>2012-09-10</date><risdate>2012</risdate><volume>86</volume><issue>11</issue><artnum>115205</artnum><issn>1098-0121</issn><eissn>1550-235X</eissn><abstract>Cathodoluminescence spectra have been measured to determine the characteristics of ubiquitous green luminescence (GL) in nonstoichiometric zinc oxide (ZnO). Zn- and O-rich ZnO were found to exhibit characteristic emissions at 2.53 eV [full width at half-maximum (FWHM) 340 meV] and 2.30 eV (FWHM 450 meV), respectively. Hydrogen was used to probe the physical nature of GL centers. The Zn-rich GL is enhanced upon H incorporation, whereas the O-rich GL is completely quenched as its underlying acceptor-like V sub(Zn) centers are passivated by H. The GL emission bands each exhibit remarkably different excitation-power dependencies. The Zn-rich GL follows a close to linear relationship with excitation power, while the O-rich GL exhibits a square-root dependence. Calculations based on bimolecular recombination equations show the defect concentration in Zn-rich ZnO is three orders of magnitude greater than that in O-rich ZnO, indicating V sub(O) is more readily formed than V sub(Zn) in thermochemical treatments of ZnO.</abstract><doi>10.1103/PhysRevB.86.115205</doi></addata></record> |
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subjects | Bands Condensed matter Excitation Luminescence Mathematical analysis Spectra Zinc Zinc oxide |
title | Characteristics of point defects in the green luminescence from Zn- and O-rich ZnO |
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