MONTE-CARLO SIMULATION OF LUMINESCENT SOLAR CONCENTRATORS WITH SLOPED EDGES

Author(s):  
T. Oksa ◽  
M. Hämäläinen
2013 ◽  
Vol 22 (S1) ◽  
pp. A35 ◽  
Author(s):  
S. R. Wilton ◽  
M. R. Fetterman ◽  
J. J. Low ◽  
Guanjun You ◽  
Zhenyu Jiang ◽  
...  

2013 ◽  
Vol 113 (21) ◽  
pp. 214510 ◽  
Author(s):  
Shin Woei Leow ◽  
Carley Corrado ◽  
Melissa Osborn ◽  
Michael Isaacson ◽  
Glenn Alers ◽  
...  

Energies ◽  
2021 ◽  
Vol 14 (2) ◽  
pp. 455
Author(s):  
Duncan E. Smith ◽  
Michael D. Hughes ◽  
Bhakti Patel ◽  
Diana-Andra Borca-Tasciuc

Luminescent solar concentrators enhance the power output of solar cells through wave-guided luminescent emission and have great potential as building-integrated photovoltaics. Luminescent solar concentrators with a variety of geometries and absorbing–emitting materials have been reported in the literature. As the breadth of available experimental configurations continues to grow, there is an increasing need for versatile Monte Carlo ray-tracing simulation tools to analyze the performance of these devices for specific applications. This paper presents the framework for a Monte Carlo ray-tracing simulation tool that can be used to analyze a host of three-dimensional geometries. It incorporates custom radiative transport models to consider the effects of scattering from luminescent media, while simultaneously modeling absorption and luminescent emission. The model is validated using experimental results for three-dimensional planar and wedge-shaped luminescent solar concentrators employing scattering phosphor films. Performance was studied as a function of length, wavelength, and the angle of incidence of incoming light. The data for the validation studies and the code (written using the Python programming language) associated with the described model are publically available.


2019 ◽  
Vol 40 (4) ◽  
pp. 484-490
Author(s):  
束俊鹏 SHU Jun-peng ◽  
汪鹏君 WANG Peng-jun ◽  
张晓伟 ZHANG Xiao-wei ◽  
解凯贺 XIE Kai-he ◽  
张会红 ZHANG Hui-hong ◽  
...  

Author(s):  
Ryuichi Shimizu ◽  
Ze-Jun Ding

Monte Carlo simulation has been becoming most powerful tool to describe the electron scattering in solids, leading to more comprehensive understanding of the complicated mechanism of generation of various types of signals for microbeam analysis.The present paper proposes a practical model for the Monte Carlo simulation of scattering processes of a penetrating electron and the generation of the slow secondaries in solids. The model is based on the combined use of Gryzinski’s inner-shell electron excitation function and the dielectric function for taking into account the valence electron contribution in inelastic scattering processes, while the cross-sections derived by partial wave expansion method are used for describing elastic scattering processes. An improvement of the use of this elastic scattering cross-section can be seen in the success to describe the anisotropy of angular distribution of elastically backscattered electrons from Au in low energy region, shown in Fig.l. Fig.l(a) shows the elastic cross-sections of 600 eV electron for single Au-atom, clearly indicating that the angular distribution is no more smooth as expected from Rutherford scattering formula, but has the socalled lobes appearing at the large scattering angle.


Author(s):  
D. R. Liu ◽  
S. S. Shinozaki ◽  
R. J. Baird

The epitaxially grown (GaAs)Ge thin film has been arousing much interest because it is one of metastable alloys of III-V compound semiconductors with germanium and a possible candidate in optoelectronic applications. It is important to be able to accurately determine the composition of the film, particularly whether or not the GaAs component is in stoichiometry, but x-ray energy dispersive analysis (EDS) cannot meet this need. The thickness of the film is usually about 0.5-1.5 μm. If Kα peaks are used for quantification, the accelerating voltage must be more than 10 kV in order for these peaks to be excited. Under this voltage, the generation depth of x-ray photons approaches 1 μm, as evidenced by a Monte Carlo simulation and actual x-ray intensity measurement as discussed below. If a lower voltage is used to reduce the generation depth, their L peaks have to be used. But these L peaks actually are merged as one big hump simply because the atomic numbers of these three elements are relatively small and close together, and the EDS energy resolution is limited.


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