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Results: 12

1.
Figure 1

Figure 1. From: Plasmonics of 3-D Nanoshell Dimers Using Multipole Expansion and Finite Element Method.

3-D Nanoshell Dimer schematic

Christopher G. Khoury, et al. ACS Nano. 2009 September 22;3(9):2776-2788.
2.
Figure 7

Figure 7. From: Plasmonics of 3-D Nanoshell Dimers Using Multipole Expansion and Finite Element Method.

3-D illustration of E-field behavior surrounding Gold Dimer ND[20nm,5nm,20%]@λpeak = 660nm

Christopher G. Khoury, et al. ACS Nano. 2009 September 22;3(9):2776-2788.
3.
Figure 11

Figure 11. From: Plasmonics of 3-D Nanoshell Dimers Using Multipole Expansion and Finite Element Method.

FE(λ) using ε(λ)corrected v.s. nanoshell diameter D, for ND[∆D,5nm,20%] of (a) Au and (b) Ag

Christopher G. Khoury, et al. ACS Nano. 2009 September 22;3(9):2776-2788.
4.
Figure 2

Figure 2. From: Plasmonics of 3-D Nanoshell Dimers Using Multipole Expansion and Finite Element Method.

FE(λ) v.s. shell thickness s for ND[20nm,5nm,∆s] of (a) Au (b) Ag

Christopher G. Khoury, et al. ACS Nano. 2009 September 22;3(9):2776-2788.
5.
Figure 4

Figure 4. From: Plasmonics of 3-D Nanoshell Dimers Using Multipole Expansion and Finite Element Method.

FE(λ) v.s. nanoshell diameter D for ND[∆D,5nm,20%] of (a) Au (b) Ag

Christopher G. Khoury, et al. ACS Nano. 2009 September 22;3(9):2776-2788.
6.
Figure 3

Figure 3. From: Plasmonics of 3-D Nanoshell Dimers Using Multipole Expansion and Finite Element Method.

FE(λ) v.s. dimer separation d for ND[20nm,∆d,20%] of (a) Au (b) Ag

Christopher G. Khoury, et al. ACS Nano. 2009 September 22;3(9):2776-2788.
7.
Figure 12

Figure 12. From: Plasmonics of 3-D Nanoshell Dimers Using Multipole Expansion and Finite Element Method.

Error between models employing ε(λ)uncorrected and ε(λ)corrected. The error is evaluated as follows: ∆var = varCOMSOLuncorrectedvarCOMSOLcorrected, where var represents variables |Ez|, ∆λmax or FWHM

Christopher G. Khoury, et al. ACS Nano. 2009 September 22;3(9):2776-2788.
8.
Figure 10

Figure 10. From: Plasmonics of 3-D Nanoshell Dimers Using Multipole Expansion and Finite Element Method.

FE(λ) using ε(λ)uncorrected and ε(λ)corrected as a function of shell thickness s for ND [20nm,5nm,∆s] of (a) Au and (b) Ag

Christopher G. Khoury, et al. ACS Nano. 2009 September 22;3(9):2776-2788.
9.
Figure 5

Figure 5. From: Plasmonics of 3-D Nanoshell Dimers Using Multipole Expansion and Finite Element Method.

Matrix of Error plots between COMSOL and ME for 3 scenarios of interest: ND[20nm,5nm,∆s], ND[20nm,∆d,20%] and ND[∆D,5nm,20%]. Error computed as ∆var = varCOMSOLvarME, where var represents variables |Ez|, ∆λmax or FWHM

Christopher G. Khoury, et al. ACS Nano. 2009 September 22;3(9):2776-2788.
10.
Figure 6

Figure 6. From: Plasmonics of 3-D Nanoshell Dimers Using Multipole Expansion and Finite Element Method.

Analysis of 20nm Au Nanoshell Monomer v.s. shell thickness s, interrogated at 2.5nm from shell surface (a) FE(λ) (b) Relative Error between ME and COMSOL

Christopher G. Khoury, et al. ACS Nano. 2009 September 22;3(9):2776-2788.
11.
Figure 9

Figure 9. From: Plasmonics of 3-D Nanoshell Dimers Using Multipole Expansion and Finite Element Method.

Comparison between the size-correction models , and for Au ND[20nm,5nm,20%]; (a) Leff v.s. shell thickness s, (b) Au Dielectric Function, εAu(λ) and (c) Comparison of three Leff models

Christopher G. Khoury, et al. ACS Nano. 2009 September 22;3(9):2776-2788.
12.
Figure 8

Figure 8. From: Plasmonics of 3-D Nanoshell Dimers Using Multipole Expansion and Finite Element Method.

Spatial plots for Au ND[20nm,5nm,20%]: (a) Slice plot along x–z plane, represented in 3-D with |Ez| as the third dimension. Inset is 2-D slice plot for reference. (b) Spatial resolution comparison of x- and z-line plots as a function of shell thickness s.

Christopher G. Khoury, et al. ACS Nano. 2009 September 22;3(9):2776-2788.

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