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Broadband and omnidirectional absorption in heterostructures with a highly absorptive metallic film and a dielectric Bragg reflector
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10.1063/1.3562173
/content/aip/journal/jap/109/6/10.1063/1.3562173
http://aip.metastore.ingenta.com/content/aip/journal/jap/109/6/10.1063/1.3562173
View: Figures

Figures

Image of FIG. 1.
FIG. 1.

Dispersion diagram of (CD)N for both TE and TM waves. In the region between the two dashed lines, an omnidirectional gap exists. , , nm, nm.

Image of FIG. 2.
FIG. 2.

(Color online) (a), (b) and (c) show the reflectance, transmittance and absorbance of M(CD)10, respectively. nm. (d) The simulated distributions of (blue lines) and (black lines) in M(CD)10 at a wavelength of 551.0 nm. For clearer presentation, layer M is drawn with a thickness 10 times greater than its true scaled value. All the other parameters are the same as those in Fig. 1.

Image of FIG. 3.
FIG. 3.

(Color online) Absorbance (solid lines) of BM(CD)10 and reflectance (dashed lines) of (CD)10 as a function of wavelength for TM and TE modes at 0°, 50°, and 75° incident angles. B is the protection film with nm and . nm. All the other parameters are the same as those in Fig. 1.

Image of FIG. 4.
FIG. 4.

(Color online) (a) The average values of fields () in the metallic layer of BM(CD)10 as a function of wavelength at normal incidence. (b), (c) and (d) give the distributions of in BM(CD)10 at different wavelengths of 407.5 nm, 539.1 nm and 816.3 nm, respectively. For clearer presentation, layer M is drawn with a thickness 6 times greater than its true scaled value. All the parameters are the same as those in Fig. 3.

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/content/aip/journal/jap/109/6/10.1063/1.3562173
2011-03-22
2014-04-17
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752b84549af89a08dbdd7fdb8b9568b5 journal.articlezxybnytfddd
Scitation: Broadband and omnidirectional absorption in heterostructures with a highly absorptive metallic film and a dielectric Bragg reflector
http://aip.metastore.ingenta.com/content/aip/journal/jap/109/6/10.1063/1.3562173
10.1063/1.3562173
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