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However the hollow nanosphere presents only slight fluctuations of the maximal absorption efficiency.
Finally a design tolerance analysis for the size parameters, reveals that the current fabrication precision is sufficient to guarantee 90% of maximal absorption efficiency.
The maximal absorption efficiency of nanorods increases of less than 10% as the wavelength increases, showing that a higher wavelength ensures higher efficiency of optimized nanorods.
We consider a threshold of 90% of the maximal absorption efficiency for each nanoparticle, and report results in Tab. 2 as well as Fig. 8.
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Their maximal absorption efficiencies are shown in Fig. 7.
This maximum absorption efficiency max(Q abs) is corresponding to the theoretical maximum best absorption efficiency obtained for the optimized size and materials parameters.
This random orientation prevents to achieve the maximum absorption efficiency.
The results reported in Tab. 1 show that the maximum absorption efficiency depends on the polarization.
Furthermore, the absorption efficiency and the associated maximal temperature rise vary for different nanoparticle sizes (see Table 2 and Fig. 2).
To enhance the light absorption efficiency, considerable effort has been conducted for the maximal absorption of sunlight, such as chemical doping[2 8], dye sensitization[9 11], material design[12 14], defect engineering[15 17], and structure engineering[18 20].
The parameter space for diameters of NWs ranges from 50 to 200 nm whereas the FR is from 0.05 to the possible maximal values for squarely and hexagonal NWs. Figure 3a shows the light absorption efficiency for single diameter InP NW arrays when FR is 0.05 with the optical constants provided in the inset.
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