Phosphorus and boron codoping of silicon nanocrystals by ion implantation: Photoluminescence properties

被引:24
|
作者
Nakamura, Toshihiro [1 ]
Adachi, Sadao [1 ]
Fujii, Minoru [2 ]
Miura, Kenta [1 ]
Yamamoto, Shunya [3 ]
机构
[1] Gunma Univ, Grad Sch Engn, Kiryu, Gunma 3768515, Japan
[2] Kobe Univ, Grad Sch Engn, Dept Elect & Elect Engn, Kobe, Hyogo 6578501, Japan
[3] Japan Atom Energy Agcy, Quantum Beam Sci Directorate, Takasaki, Gunma 3701292, Japan
来源
PHYSICAL REVIEW B | 2012年 / 85卷 / 04期
关键词
DOPED SI NANOCRYSTALS; OPTICAL-PROPERTIES; ENERGY-TRANSFER; POROUS SILICON; QUANTUM DOTS; IMPURITIES; ABSORPTION; DIFFUSION; EMISSION; LIGHT;
D O I
10.1103/PhysRevB.85.045441
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
The photoluminescence (PL) properties of P or B single-doped Si nanocrystals (Si-nc's) and P and B co-doped Si-nc's are studied. In the single-doped Si-nc samples, PL quenching occurs as a result of the Auger nonradiative recombination process between the photoexcited excitons and free carriers supplied by doped impurities. In the (P, B) co-doped sample, on the other hand, the donor-acceptor (D-A)-pair recombination emission is clearly observed on the long-wavelength side of the intrinsic Si-nc emission peak at similar to 900 nm. The D-A-pair recombination energy is found to be smaller than the band-gap energy of bulk Si and is strongly dependent on the number of P and B impurities doped in a Si-nc. PL spectra are measured at 50 and 300 K and found to indicate that strong thermal quenching occurs in a (P, B) co-doped sample at 300 K. This quenching effect is probably because of carrier migration among the donor and acceptor states. The PL decay rate is determined as a function of the emitted-light wavelength for the pure and (P, B) co-doped Si-nc samples.
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页数:7
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