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Draine, B. T.; Flatau, P. J. Program DDSCAT; University of California, San Diego, and Scripps Institute of Oceanography, La Jolla, CA.
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Program DDSCAT
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Draine, B.T.1
Flatau, P.J.2
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45749136331
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DDSCAT calculation details are as follows: dipole geometry input files for me bumpy model with icosahedral symmetry at 1 nm dipole spacing were generated by a stand-alone code written in-house, available per request. By this code, three sizes of core/bump combinations were generated (diameters, in nm, 90/30, 70/24, and 37/19. For half-embedded bumps, the total dipoles were 474 982, 244 720, and 50 671, respectively. For one-third embedded bumps, they were 513 166, 244 720, and 57 017, respectively. Convenient graphical depictions of each input file (insets in the figure) were obtained by protein visualization software by labeling each dipole location as water oxygens and scaling appropriately. Peak position was obtained by cubic spline fit of data points at a 10 nm resolution near the peak. External medium is set to water, with refractive index (n, k) equal to (1.33, 0.01) for all visible wavelengths
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DDSCAT calculation details are as follows: dipole geometry input files for me bumpy model with icosahedral symmetry at 1 nm dipole spacing were generated by a stand-alone code written in-house, available per request. By this code, three sizes of core/bump combinations were generated (diameters, in nm): 90/30, 70/24, and 37/19. For half-embedded bumps, the total dipoles were 474 982, 244 720, and 50 671, respectively. For one-third embedded bumps, they were 513 166, 244 720, and 57 017, respectively. Convenient graphical depictions of each input file (insets in the figure) were obtained by protein visualization software by labeling each dipole location as water oxygens and scaling appropriately. Peak position was obtained by cubic spline fit of data points at a 10 nm resolution near the peak. External medium is set to water, with refractive index (n, k) equal to (1.33, 0.01) for all visible wavelengths.
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