Nanoscale Characterization of Active Doping Concentration in Boron-Doped Individual Si Nanocrystals

2018 ◽  
Vol 215 (23) ◽  
pp. 1800531 ◽  
Author(s):  
Jie Xu ◽  
Dongke Li ◽  
Deyuan Chen ◽  
Wei Li ◽  
Jun Xu
1998 ◽  
Vol 535 ◽  
Author(s):  
Jeff J. Petersoa ◽  
Charles E. Hunt ◽  
Stefan F. Zappe ◽  
Ernst Obeneier ◽  
Richard Westhoff ◽  
...  

AbstractMobilities in Si1-x-yGex Cy layers were measured using mesa etched Van der Pauw structures for alloy layers with 0 < x < 0.30 and 0 < y < 0.02 and doping levels of 1015 < N < 1018 cm-3. Mobilities in Si1-x-yGex Cy layers with x = 0.27 were found to approach Si mobilities for both μn and μp.While electron mobilities in phosphorous-doped SiGeC decrease with doping concentration, hole mobilities in boron-doped SiGeC increase with doping level, indicating ionized impurity scattering is not dominant for μp over the temperature range studied.


1987 ◽  
Vol 95 ◽  
Author(s):  
Jin Jang ◽  
Sung Chul Kim ◽  
Dae Bong Lee ◽  
Choochon Lee

AbstractThe electrical and optical properties of heavily boron-doped hydrogenated amorphous silicon (a-Si:H) films deposited at 100°C with a gas phase doping concentration between B2H6/SiH4=0.001 and 0.1 have been investigated. The absorption edge exhibits the characteristic Urbach form and the width of exponential absorption tail, Eo, increases with increasing doping concentration. The optical gap has a linear relationship with the Eo and it is expected to be 2.20 eV when the Eo is zero. Thus, the disorder determines the optical gap directly whether the sample is doped or undoped, the hydrogen and boron in the film change the disorder. The conversion efficiency of n-i-p cell is improved by 15% if the p-layer is deposited at 100°C after preparing the n- and i-layers ∼250°C.


2021 ◽  
Vol 106 ◽  
pp. 116-123
Author(s):  
Long Sui ◽  
Chunyu Tang ◽  
Qing Du ◽  
Ying Zhao ◽  
Kui Cheng ◽  
...  

2002 ◽  
Vol 742 ◽  
Author(s):  
T. Kimoto ◽  
K. Hashimoto ◽  
K. Fujihira ◽  
K. Danno ◽  
S. Nakamura ◽  
...  

ABSTRACTHomoepitaxial growth, impurity doping, and diode fabrication on 4H-SiC(11–20) and (03–38) have been investigated. Although the efficiency of nitrogen incorporation is higher on the non-standard faces than on (0001), a low background doping concentration of 2∼3×1014 cm-3 can be achieved. On these faces, boron and aluminum are less effectively incorporated, compared to the growth on off-axis (0001). 4H-SiC(11–20) epilayers are micropipe-free, as expected. More interestingly, almost perfect micropipe closing has been realized in 4H-SiC (03–38) epitaxial growth. Ni/4H-SiC(11–20) and (03–38) Schottky barrier diodes showed promising characteritics of 3.36 kV-24 mΩcm2 and 3.28 kV–22 mΩcm2, respectively. The breakdown voltage of 4H-SiC(03–38) Schottky barrier diodes was significantly improved from 1 kV to above 2.5 kV by micropipe closing.


2017 ◽  
Vol 47 (2) ◽  
pp. 938-943 ◽  
Author(s):  
Yu Yang ◽  
Jianqiu Guo ◽  
Balaji Raghothamachar ◽  
Xiaojun Chan ◽  
Taejin Kim ◽  
...  

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