Ordered Zinc Antimonate Nanoisland Attachment and Morphology Control of ZnO Nanobelts by Sb Doping

被引:15
作者
Cheng, Baochang [1 ,2 ]
Tian, Baixiang [1 ,2 ]
Sun, Wei [1 ,2 ]
Xiao, Yanhe [1 ,2 ]
Lei, Shuijin [1 ,2 ]
Wang, Zhanguo [3 ]
机构
[1] Nanchang Univ, Inst Adv Studying, Nanchang 330031, Peoples R China
[2] Nanchang Univ, Sch Mat Sci & Engn, Nanchang 330031, Peoples R China
[3] Chinese Acad Sci, Inst Semicond, Key Lab Semicond Mat Sci, Beijing 100083, Peoples R China
关键词
DOPED ZNO; QUANTUM DOTS; PHOTOLUMINESCENCE; GROWTH; OXIDES; NANOSTRUCTURES; SEMICONDUCTORS; RECOMBINATION; NANOPARTICLES; NANOCRYSTALS;
D O I
10.1021/jp9015504
中图分类号
O64 [物理化学(理论化学)、化学物理学];
学科分类号
070304 ; 081704 ;
摘要
Hierarchical heterostructures of zinc antimonate nanoislands on ZnO nanobelts were prepared by simple annealing of the polymeric precursor. Sb can promote the growth of ZnO nanobelts along the [552] direction because of the segregation of Sb dopants on the +(001) and (110) surfaces of ZnO nanobelts. Furthermore, the ordered nanoislands of toothlike ZnSb(2)O(6) along the [001](ZnO) direction and rodlike Zn(7)Sb(2)O(12) along the [110](ZnO) direction can be formed because of the match relation of the lattice and polar charges between ZnO and zinc antimonate. The incorporation of Sb in a ZnO lattice induces composition fluctuation, and the growth of zinc antimonate nanoislands on nanobelt sides induces interface fluctuation, resulting in dominance of the bound exciton transition in the room temperature near-band-edge (NBE) emission at relatively low excitation intensity. At high excitation intensity, however, Auger recombination makes photogenerated electrons release phonon and relax from the conduction band to the trap states, causing the NBE emission to gradually saturate and redshift with increasing excitation intensity. The green emission more reasonably originates from the recombination of electrons in shallow traps with doubly charged V(O)** oxygen vacancies. Because a V(O)** center can trap a photoactivated electron and change to a singly charged oxygen vacancy V(O)* state, its emission intensity exhibits a maximum with increasing excitation intensity.
引用
收藏
页码:9638 / 9643
页数:6
相关论文
共 47 条
[1]   Defects in quantum dots of IIB-VI semiconductors [J].
Babentsov, V. ;
Sizov, F. .
OPTO-ELECTRONICS REVIEW, 2008, 16 (03) :208-225
[2]   Photoluminescence of polycrystalline zinc oxide co-activated with trivalent rare earth ions and lithium. Insertion of rare-earth ions into zinc oxide [J].
Bachir, S ;
Azuma, K ;
Kossanyi, J ;
Valat, P ;
RonfardHaret, JC .
JOURNAL OF LUMINESCENCE, 1997, 75 (01) :35-49
[3]   Dual-mode mechanical resonance of individual ZnO nanobelts [J].
Bai, XD ;
Gao, PX ;
Wang, ZL ;
Wang, EG .
APPLIED PHYSICS LETTERS, 2003, 82 (26) :4806-4808
[4]   DOUBLE-OXIDES OF ATIMONY PENTOXIDE WITH SPINEL STRUCTURE [J].
BAYER, G .
NATURWISSENSCHAFTEN, 1961, 48 (02) :46-&
[5]   Dynamics of GaN band edge photoluminescence at near-room-temperature regime [J].
Chen, XB ;
Huso, J ;
Morrison, JL ;
Bergman, L .
JOURNAL OF APPLIED PHYSICS, 2006, 99 (04)
[6]   Zn2SiO4/ZnO Core/Shell Coaxial Heterostructure Nanobelts Formed by an Epitaxial Growth [J].
Cheng, Baochang ;
Yu, Xiaoming ;
Liu, Hongjuan ;
Wang, Zhanguo .
JOURNAL OF PHYSICAL CHEMISTRY C, 2008, 112 (42) :16312-16317
[7]   Enhanced effect of electron-hole plasma emission in Dy, Li codoped ZnO nanostructures [J].
Cheng, Baochang ;
Yu, Xiaoming ;
Liu, Hongjuan ;
Fang, Ming ;
Zhang, Lide .
JOURNAL OF APPLIED PHYSICS, 2009, 105 (01)
[8]   Controlled growth and properties of one-dimensional ZnO nanostructures with Ce as activator/dopant [J].
Cheng, BC ;
Xiao, YH ;
Wu, GS ;
Zhang, LD .
ADVANCED FUNCTIONAL MATERIALS, 2004, 14 (09) :913-919
[9]   Photoluminescence and electron paramagnetic resonance of ZnO tetrapod structure [J].
Djurisic, AB ;
Choy, WCH ;
Roy, VAL ;
Leung, YH ;
Kwong, CY ;
Cheah, KW ;
Rao, TKG ;
Chan, WK ;
Lui, HT ;
Surya, C .
ADVANCED FUNCTIONAL MATERIALS, 2004, 14 (09) :856-864
[10]  
Ezhilvalavan S, 1996, APPL PHYS LETT, V68, P2693, DOI 10.1063/1.116311