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Univ New S Wales, Ctr Mat Res Energy Convers, Sch Mat Sci & Engn, Sydney, NSW 2052, AustraliaUniv New S Wales, Ctr Mat Res Energy Convers, Sch Mat Sci & Engn, Sydney, NSW 2052, Australia
Bak, T.
[1
]
Nowotny, M. K.
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Univ New S Wales, Ctr Mat Res Energy Convers, Sch Mat Sci & Engn, Sydney, NSW 2052, AustraliaUniv New S Wales, Ctr Mat Res Energy Convers, Sch Mat Sci & Engn, Sydney, NSW 2052, Australia
Nowotny, M. K.
[1
]
Sheppard, L. R.
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Univ New S Wales, Ctr Mat Res Energy Convers, Sch Mat Sci & Engn, Sydney, NSW 2052, AustraliaUniv New S Wales, Ctr Mat Res Energy Convers, Sch Mat Sci & Engn, Sydney, NSW 2052, Australia
Sheppard, L. R.
[1
]
Nowotny, J.
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Univ New S Wales, Ctr Mat Res Energy Convers, Sch Mat Sci & Engn, Sydney, NSW 2052, AustraliaUniv New S Wales, Ctr Mat Res Energy Convers, Sch Mat Sci & Engn, Sydney, NSW 2052, Australia
Nowotny, J.
[1
]
机构:
[1] Univ New S Wales, Ctr Mat Res Energy Convers, Sch Mat Sci & Engn, Sydney, NSW 2052, Australia
The present work reports the effect of chromium on the mobility terms for electrons and electron holes for TiO2 at 1273 K. These data were determined by using the concentration data from the defect disorder diagram derived by the authors and the electrical conductivity data for Cr-doped TiO2 reported by Carpentier et al. [J. Phys. Chem. Solids 1989, 50, 145]. It is shown that chromium incorporates into the TiO2 lattice according to two different mechanism depending on chromium concentration. In the concentration range 1-3 atom %, chromium incorporation leads to the formation of acceptors, which are compensated by tri-valent titanium interstitials. However, in the range 4-5 atom %, the acceptor-type defects formed by chromium incorporated in the titanium sites are compensated by oxygen vacancies. The incorporation of chromium results in a relatively insignificant increase of the mobility of electrons from mu(n) = 0.5 x 10(-5) m(2) V-1 s(-1) for undoped TiO2 to mu(n) = 1.3 x 10(-5) m(2) V-1 s(-1). The incorporation of Cr results in a drop of the mobility of electron holes from mu(p) = 2.95 x 10-5 m(2) V-1 s(-1) for undoped TiO2 to mu(p) = 0.6 x 10-5 m(2) V-1 s(-1) for Cr-doped TiO2. The observed mobility changes are considered in terms of the Cr-induced structural changes of the TiO2 lattice.
机构:
Univ Kebangsaan Malaysia, Inst Microengn & Nanoelect IMEN, Bangi 43600, Selangor, MalaysiaUniv Kebangsaan Malaysia, Inst Microengn & Nanoelect IMEN, Bangi 43600, Selangor, Malaysia
Al-Hardan, N. H.
Abdullah, M. J.
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Univ Sains Malaysia, Sch Phys, George Town 11800, MalaysiaUniv Kebangsaan Malaysia, Inst Microengn & Nanoelect IMEN, Bangi 43600, Selangor, Malaysia
Abdullah, M. J.
Aziz, A. Abdul
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Univ Sains Malaysia, Sch Phys, George Town 11800, MalaysiaUniv Kebangsaan Malaysia, Inst Microengn & Nanoelect IMEN, Bangi 43600, Selangor, Malaysia