Synthesis and Characterization of Cu-doped ZnO Nanorods
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作者:
Pung, S. Y.
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Univ Sains Malaysia, Sch Mat & Mineral Resources Engn, Nibong Tebal 14300, Pulau Pinang, MalaysiaUniv Sains Malaysia, Sch Mat & Mineral Resources Engn, Nibong Tebal 14300, Pulau Pinang, Malaysia
Pung, S. Y.
[1
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Ong, C. S.
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Univ Sains Malaysia, Sch Mat & Mineral Resources Engn, Nibong Tebal 14300, Pulau Pinang, MalaysiaUniv Sains Malaysia, Sch Mat & Mineral Resources Engn, Nibong Tebal 14300, Pulau Pinang, Malaysia
Ong, C. S.
[1
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Isha, K. Mohd
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SIRIM Berhad, Adv Mat Res Ctr, Kulim 09000, Kedah, MalaysiaUniv Sains Malaysia, Sch Mat & Mineral Resources Engn, Nibong Tebal 14300, Pulau Pinang, Malaysia
Isha, K. Mohd
[2
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Othman, M. H.
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SIRIM Berhad, Adv Mat Res Ctr, Kulim 09000, Kedah, MalaysiaUniv Sains Malaysia, Sch Mat & Mineral Resources Engn, Nibong Tebal 14300, Pulau Pinang, Malaysia
Othman, M. H.
[2
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机构:
[1] Univ Sains Malaysia, Sch Mat & Mineral Resources Engn, Nibong Tebal 14300, Pulau Pinang, Malaysia
[2] SIRIM Berhad, Adv Mat Res Ctr, Kulim 09000, Kedah, Malaysia
Cu-doped ZnO nanorods were synthesized by sol-gel method using zinc nitrate tetrahydrate, methenamine and cupric acetate monohydrate as precursors. The as-synthesized ZnO nanorods have a twin-rod structure. The polar (002) surface of ZnO nanorods, which could be either negatively charge (O-terminated) or positively charged (Zn-terminated), was responsible for the formation of twin-rod structure. The results showed that the size, aspect ratio, crystallinity and c-lattice parameter of Cu doped ZnO nanorods decreased with increasing of Cu dopant concentration. In fact, the presence of Cu retarded the growth of ZnO nanorods in its preferred growth direction, i.e. (0001). The XPS analysis indicates that Cu ions were oxidized (Cu2+) and substituted into the ZnO lattice at the Zn2+ site. The presence of Cu reduced the optical bandgap of ZnO from 3.34 eV (undoped ZnO nanorods) to 3.31 eV (20 mol% Cu doped ZnO). Besides, it induced a visible PL emission at 2.97 eV, which could be related to the transition of electrons from conduction band (E-c) to Cu acceptor energy level (E-v + 0.45 eV) radiatively.
机构:
Korea Atom Energy Res Inst, Radioisotope Res Div, Taejon 305353, South KoreaKorea Atom Energy Res Inst, Radioisotope Res Div, Taejon 305353, South Korea
Uhm, Young Rang
Han, Byung Sun
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Miraenanotech, Cheongwon 363911, Chungcheongbuk, South KoreaKorea Atom Energy Res Inst, Radioisotope Res Div, Taejon 305353, South Korea
Han, Byung Sun
Rhee, Chang Kyu
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Korea Atom Energy Res Inst, Nucl Mat Dev Div, Taejon 305353, South KoreaKorea Atom Energy Res Inst, Radioisotope Res Div, Taejon 305353, South Korea
Rhee, Chang Kyu
Choi, Sun Ju
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Korea Atom Energy Res Inst, Radioisotope Res Div, Taejon 305353, South KoreaKorea Atom Energy Res Inst, Radioisotope Res Div, Taejon 305353, South Korea
机构:
Al Balqa Appl Univ, Dept Appl Sci, Amman, JordanAl Balqa Appl Univ, Dept Appl Sci, Amman, Jordan
Al-heuseen, K.
Aljameel, A. I.
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Imam Mohammad Ibn Saud Islamic Univ IMSIU, Coll Sci, Dept Phys, POB 90950, Riyadh 11623, Saudi ArabiaAl Balqa Appl Univ, Dept Appl Sci, Amman, Jordan
Aljameel, A. I.
Hussein, R. K.
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Imam Mohammad Ibn Saud Islamic Univ IMSIU, Coll Sci, Dept Phys, POB 90950, Riyadh 11623, Saudi ArabiaAl Balqa Appl Univ, Dept Appl Sci, Amman, Jordan