Electronic, magnetic and optical properties of Co(II) doped and (Al, Co) co-doped CdS nanowires: An ab initio study

被引:8
|
作者
Khan, Muhammad Sheraz [1 ]
Zou, Bingsuo [2 ]
Luo, Jun [2 ]
Yao, Shangfei [1 ]
Bukhtiar, Arfan [1 ]
Huang, WeiGuo [1 ]
Zheng, Biling [1 ]
Ullah, Sami [3 ]
Cao, JiaJun [1 ]
机构
[1] Guangxi Univ, Sch Phys Sci & Technol, Nanning 530004, Peoples R China
[2] Guangxi Univ, Sch Resources Environm & Mat, Guangxi Key Lab Proc Nonferrous Met & Featured Mat, Nanning 530004, Peoples R China
[3] King Fahd Univ Petr & Minerals KFUPM, KA Care Energy Res & Innovat Ctr ERIC, Dhahran 31261, Saudi Arabia
关键词
First principles calculations; Dilute magnetic semiconductor; Nanowires; Electronic properties; Magnetic properties; Optical properties; SEMICONDUCTOR; FERROMAGNETISM; ZNO; DEPOSITION; SCATTERING; POLARON;
D O I
10.1016/j.mssp.2023.108019
中图分类号
TM [电工技术]; TN [电子技术、通信技术];
学科分类号
0808 ; 0809 ;
摘要
In this work, we have carried out first-principles calculations for understanding the optoelectronic and magnetic properties of Co(II)-doped and (Al, Co) co-doped CdS nanowires. In the free carrier Co(II)-doped CdS NW, the spin-down Co(II)-ta state is completely empty, leading to a super-exchange process. The exchange coupling of the electron carrier (provided by Al co-doping) with the spin-down Co(II)-ta state promote a ferromagnetic ordering via double exchange interactions with a Curie temperature above room temperature. From the optical analysis, we found that Co(II) doping causes a blue-shift of the fundamental energy gap of CdS nanowire. The observed d -d spin-allowed transition peak of the Co(II) ion at 1.97 eV in the visible region is consistent with the experiments. The n-type Al co-doping not only generates an exciton-magnetic polaron (EMP) peak next to the fundamental bandgap but also exhibits the red-shift of the fundamental energy gap and Co(II)'s d-level-to-d -level transition bands. The correlation between spin-spin interaction and optical absorption shows that the d-d spin-allowed transition and optical energy gap both exhibit a blue-shift (red-shift) in the AFM (FM), supporting the experimental observation. Due to the paramagnetic behavior of the Co ions in the far configuration, there is no shift in the d-d transition peak or optical bandgap in the AFM and FM.
引用
收藏
页数:12
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