Self‐trapped state and phonon localization in TiO2quantum dot with a dipole layer

1993 ◽  
Vol 73 (9) ◽  
pp. 4689-4690 ◽  
Author(s):  
Bingsuo Zou ◽  
Yan Zhang ◽  
Liangzhi Xiao ◽  
Tiejin Li
Author(s):  
Yu Fang ◽  
Wen-Jay Lee ◽  
An-Chen Yang ◽  
Guan-Peng Chen ◽  
Nan-Yow Chen ◽  
...  

Author(s):  
Yuxiang Ni ◽  
Honggang Zhang ◽  
Song Hu ◽  
Hongyan Wang ◽  
Sebastian Volz ◽  
...  

1972 ◽  
Vol 34 (2) ◽  
pp. 151-172 ◽  
Author(s):  
Richard A. Arndt ◽  
James D. Bond ◽  
L. David Roper

2015 ◽  
Vol 5 (17) ◽  
pp. n/a-n/a ◽  
Author(s):  
Shunmian Lu ◽  
Xing Guan ◽  
Xinchen Li ◽  
Wei E. I. Sha ◽  
Fengxian Xie ◽  
...  

2017 ◽  
Vol 8 (1) ◽  
Author(s):  
Michael E. Manley ◽  
Douglas L. Abernathy ◽  
John D. Budai
Keyword(s):  

1994 ◽  
Vol 50 (2) ◽  
pp. 1297-1300 ◽  
Author(s):  
Silvia Rubini ◽  
Pietro Ballone

2005 ◽  
Vol 336 (2-3) ◽  
pp. 259-263 ◽  
Author(s):  
E.L. Albuquerque ◽  
E.B. Barros ◽  
V.N. Freire ◽  
J. Mendes-Filho

1993 ◽  
Vol 297 ◽  
Author(s):  
P.H Pfleiderer H

The buffer of standard solar cells restricts the "surface recombination" at the front side. Some typical cell properties linked to the buffer are exposed by numerical simulations: The "blue snake" appearing in small-signal photocharacteristics, the electron inversion layer, the reverse field peak and the satellite space-charge dipole layer. It is possible to base a simulation on the roots of an algebraic equation.


2012 ◽  
Vol 51 ◽  
pp. 081303 ◽  
Author(s):  
Shinya Hibino ◽  
Tomonori Nishimura ◽  
Kosuke Nagashio ◽  
Koji Kita ◽  
Akira Toriumi

1992 ◽  
Vol 02 ◽  
pp. C2-279-C2-283
Author(s):  
S. R. ELLIOTT

The anomalous vibrational behaviour exhibited by non-crystalline materials - a peak in the vibrational density of states, and in the Raman spectrum (the boson peak) at low frequencies, and a peak in the heat capacity and a plateau in the thermal conductivity at low temperatures - is ascribed ta phonon localization associated with the strong scattering of phonons by density-fluctuation domains in the structure. Within such domains, short-range and medium-range arder is maintained, and outside them the material is structurally homogeneous and isotropie. This model can also explain the correlation between the boson-peak frequency and the position of the first sharp diffraction peak in the structure factor observed in a number of inorganie and polymerie amorphous solids.


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