2013
DOI: 10.1088/2040-8978/15/10/105101
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On the limits of the effective description of hyperbolic materials in the presence of surface waves

Abstract: Here, we address the question of the validity of an effective description for hyperbolic metamaterials in the near-field region. We show that the presence of localized modes such as surface waves drastically limits the validity of the effective description and requires revisiting the concept of homogenization in near-field. We demonstrate from exact calculations that one can find surface modes in spectral regions where the effective approach predicts hyperbolic modes only. Hence, the presence of surface modes … Show more

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Cited by 55 publications
(43 citation statements)
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“…As was shown in Ref. 31 materials which have a broad hyperbolic frequency band as predicted from effective medium theory can support surface modes inside these frequency bands as well which will compete with the hyperbolic modes 31,32 . In particular, we will show that for the realization of a hyperbolic metamaterial as studied in Ref.…”
mentioning
confidence: 61%
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“…As was shown in Ref. 31 materials which have a broad hyperbolic frequency band as predicted from effective medium theory can support surface modes inside these frequency bands as well which will compete with the hyperbolic modes 31,32 . In particular, we will show that for the realization of a hyperbolic metamaterial as studied in Ref.…”
mentioning
confidence: 61%
“…As will become clear in the following the such calculated frequency bands ∆ 1 and ∆ 2 can also support surface modes, which are not taken into account in the effective description 31 . In order to study super-Planckian radiation we consider the geometry depicted in Fig.…”
mentioning
confidence: 96%
“…By comparing EMT to the exact results in Figure 7b, it can be seen that the EMT results are actually not so far off from the exact results for most frequencies when SiC is topmost layer, but they lack of course the surface mode contribution of the first SiC layer as could already be observed in the transmission coefficients. This finding has important consequences for the LDOS and heat flux as discussed in [25,81,96]. Compared to the mixed configuration and the configuration with Ge as topmost layer EMT overestimated the heat flux inside the reststrahlen band for most frequencies, whereas compared to the configuration with SiC as topmost layer EMT underestimates the heat flux especially around ω SPhP .…”
Section: Radiative Heat Fluxmentioning
confidence: 91%
“…one period of the structure, are strictly speaking only meaningful when the periodicity Λ of the meta-material structure is much smaller than the wavelength but even for Λ much smaller than the wavelength the EMT results can lead to wrong predictions [25,[76][77][78][79][80][81] so that some care needs to be exercised when using these EMT expressions. Nonetheless, they are quite helpful for determinig the hyperbolic frequency bands of a meta-material structure in a simple way.…”
Section: Hyperbolic Mediamentioning
confidence: 99%
“…It should be noted that the effective medium approach used in Eqn. (5), (6) does not describe the effects of the spatial dispersion in the metamaterial [27,28], however in planar hyperbolic metamaterials studied in this work the resulting corrections can be neglected [29]. The permittivity of AlInAs in mid-IR is approximately constant ( AlInAs ≈ 10.23), and the permittivity of n + -doped InGaAs can be expressed as [14] …”
mentioning
confidence: 92%