Increased power collection efficiency of conventional silicon photovoltaic modules with holographic light management techniques

Author(s):  
Yuechen Wu ◽  
Benjamin Chrysler ◽  
Raymond K. Kostuk ◽  
Jianbo Zhao ◽  
Silvana Ayala Pelaez
2018 ◽  
Vol 181 ◽  
pp. 77-82 ◽  
Author(s):  
A.J. Blanker ◽  
P. Berendsen ◽  
N. Phung ◽  
Z.E.A.P. Vroon ◽  
M. Zeman ◽  
...  

2012 ◽  
Author(s):  
Negar Naghavi ◽  
Zacharie Jehl ◽  
Frederique Donsanti ◽  
Jean-François Guillemoles ◽  
Isabelle Gérard ◽  
...  

Solar RRL ◽  
2017 ◽  
Vol 1 (10) ◽  
pp. 1700084 ◽  
Author(s):  
Yuehui Lu ◽  
Zhicheng Chen ◽  
Ling Ai ◽  
Xianpeng Zhang ◽  
Jing Zhang ◽  
...  

Author(s):  
Yang Li ◽  
Chen Zhu ◽  
Jun Lv ◽  
Xueqing Zhang ◽  
Alison Lennon ◽  
...  

Author(s):  
H. Rose

The scanning transmission electron microscope offers the possibility of utilizing inelastically scattered electrons. Use of these electrons in addition to the elastically scattered electrons should reduce the scanning time (dose) Which is necessary to keep the quantum noise below a certain level. Hence it should lower the radiation damage. For high resolution, Where the collection efficiency of elastically scattered electrons is small, the use of Inelastically scattered electrons should become more and more favorable because they can all be detected by means of a spectrometer. Unfortunately, the Inelastic scattering Is a non-localized interaction due to the electron-electron correlation, occurring predominantly at the circumference of the atomic electron cloud.


Author(s):  
P.E. Batson

Use of the STEM to obtain precise electronic information has been hampered by the lack of energy loss analysis capable of a resolution and accuracy comparable to the 0.3eV energy width of the Field Emission Source. Recent work by Park, et. al. and earlier by Crewe, et. al. have promised magnetic sector devices that are capable of about 0.75eV resolution at collection angles (about 15mR) which are great enough to allow efficient use of the STEM probe current. These devices are also capable of 0.3eV resolution at smaller collection angles (4-5mR). The problem that arises, however, lies in the fact that, even with the collection efficiency approaching 1.0, several minutes of collection time are necessary for a good definition of a typical core loss or electronic transition. This is a result of the relatively small total beam current (1-10nA) that is available in the dedicated STEM. During this acquisition time, the STEM acceleration voltage may fluctuate by as much as 0.5-1.0V.


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