scholarly journals Excimer laser annealing of p-type perovskite thin films

Author(s):  
X. Du ◽  
J. J. Dubowski ◽  
M. Post ◽  
D. Wang ◽  
J. Tunney
2006 ◽  
Vol 45 (5B) ◽  
pp. 4344-4346 ◽  
Author(s):  
Shinji Munetoh ◽  
Takahide Kuranaga ◽  
Byoung Min Lee ◽  
Teruaki Motooka ◽  
Takahiko Endo ◽  
...  

2006 ◽  
Vol 958 ◽  
Author(s):  
Shinji Munetoh ◽  
Takanori Mitani ◽  
Takahide Kuranaga ◽  
Teruaki Motooka

ABSTRACTWe have performed molecular-dynamics simulations of heating, melting and recrystallization processes in amorphous silicon (a-Si) thin films deposited on glass during excimer laser annealing. By partially heating the a-Si surface region with 2 nm depth and removing thermal energy from the bottom of the glass substrate, a steady-state temperature profile was obtained in the a-Si layer with the thickness of 15 nm and only the surface region was melted. It was found that nucleation predominantly occurred in the a-Si region as judged by the coordination numbers and diffusion constants of atoms in the region. The results suggest that nucleation occurs in unmelted residual a-Si region during the laser irradiation and then crystal growth proceeds toward liquid Si region under the near-complete melting condition.


2015 ◽  
Vol 424 ◽  
pp. 38-41 ◽  
Author(s):  
Daishi Shiojiri ◽  
Ryosuke Yamauchi ◽  
Daiji Fukuda ◽  
Nobuo Tsuchimine ◽  
Satoru Kaneko ◽  
...  

2002 ◽  
Vol 46 (8) ◽  
pp. 1085-1090 ◽  
Author(s):  
Chang-Ho Tseng ◽  
Ching-Wei Lin ◽  
Teh-Hung Teng ◽  
Ting-Kuo Chang ◽  
Huang-Chung Cheng ◽  
...  

1999 ◽  
Author(s):  
Seung-Jae Moon ◽  
Ming-Hong Lee ◽  
Mutsuko Hatano ◽  
Kenkichi Suzuki ◽  
Constantine P. Grigoropoulos

1992 ◽  
Vol 281 ◽  
Author(s):  
Nallan Padmapani ◽  
G. F. Neumark ◽  
N. Taskar ◽  
D. Dorman

ABSTRACTThe recent success in obtaining blue-green diode lasers using ZnSe-based heterostructures has been mainly due to the successful p-doping of ZnSe using a N plasma source in an MBE system. P-type ZnSe can also be grown by MOCVD, using NH3 as the dopant source. Dopant concentrations of up to 1018 cm−3 have been obtained but net acceptor concentrations are in the range of only about 1015 cm−3 Activation of the remaining N has been achieved to some extent (NA -ND∼3*1016cm−3 ) by rapid thermal annealing. However, this has had limited success. We have used fast surface annealing by an excimer laser to activate the N. We have observed an increase in the ratio of Acceptor Bound Exciton peak intensity to Free Exciton peak intensity on annealing and this effect increases as we increase the laser power density from 10 to 30 MW/cm2. Electrical measurements ( C-V ) give a net acceptor concentration of ∼2*1016 cm−3 and thus confirm the increase in carrier concentration after annealing.


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