Recent progress of the native defects and p-type doping of zinc oxide<xref rid="cpb_26_4_047702_fn1" ref-type="fn">*</xref> <fn id="cpb_26_4_047702_fn1"> <label>*</label> <p>Project supported by the State Key Program for Basic Research of China (Grant No. 2011CB302003), the National Natural Science Foundation of China (Grant Nos. 61274058, 61322403, 61504057, and 61574075), the Natural Science Foundation of Jiangsu Province, China (Grant Nos. BK20130013 and BK20150585), and the Six Talent Peaks Project in Jiangsu Province, China (Grant No. 2014XXRJ001).</p> </fn>

Recent progress of the native defects and p-type doping of zinc oxide* *

Project supported by the State Key Program for Basic Research of China (Grant No. 2011CB302003), the National Natural Science Foundation of China (Grant Nos. 61274058, 61322403, 61504057, and 61574075), the Natural Science Foundation of Jiangsu Province, China (Grant Nos. BK20130013 and BK20150585), and the Six Talent Peaks Project in Jiangsu Province, China (Grant No. 2014XXRJ001).

Tang Kun, Gu Shu-Lin^†, Ye Jian-Dong, Zhu Shun-Ming, Zhang Rong, Zheng You-Dou

(color online) Partial densities of states (pDOSs) of (a) V and (b) (2V–V that can be attributed to V (red) and V (blue), respectively. The DOS for bulk ZnO is also shown as shaded regions. The VBM is set to be zero value of energy. The bulk conduction band DOS and the partial DOS of the V are magnified by factors of 10 and 5, respectively. (c) A schematic drawing of the level repulsion between V and V. The pDOSs are obtained by projection onto the most adjacent Zn atoms for the V level and onto the most adjacent O atoms for the V level, respectively.^[17]