2016
DOI: 10.1088/1674-1056/25/11/114216
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Plasmon–phonon coupling in graphene–hyperbolic bilayer heterostructures

Abstract: Polar dielectrics are important optical materials enabling the subwavelength manipulation of light in infrared due to their capability to excite phonon polaritons. In practice, it is highly desired to actively modify these hyperbolic phonon polaritons (HPPs) to optimize or tune the response of the device. In this work, we investigate the plasmonic material, a monolayer graphene, and study its hybrid structure with three kinds of hyperbolic thin films grown on SiO 2 substrate. The inter-mode hybridization and t… Show more

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Cited by 4 publications
(5 citation statements)
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References 39 publications
(47 reference statements)
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“…These bounded surface modes carry high density of state of photons and can largely raise the evanescent wave tunneling and thus overall thermal radiation efficiency, as found in the measurement. This effect will be more obvious at smaller gaps or replacing Si with a low-index substrate that will enhance the bandwidth and intensity of the bounded modes 45 .…”
Section: Resultsmentioning
confidence: 99%
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“…These bounded surface modes carry high density of state of photons and can largely raise the evanescent wave tunneling and thus overall thermal radiation efficiency, as found in the measurement. This effect will be more obvious at smaller gaps or replacing Si with a low-index substrate that will enhance the bandwidth and intensity of the bounded modes 45 .…”
Section: Resultsmentioning
confidence: 99%
“…It needs to be pointed out that silicon may not be the best choice to host grapheme if one wants to maximize the heat flux and for this aim polar materials such as silica or BN may be used where the occurrence of plasmon–phonon hybridization can further strengthen the tunneling of evanescent waves 20 , 45 . However, the Si/Gr heterostructure proposed here can provide a promising framework to harvest thermal energy.…”
Section: Resultsmentioning
confidence: 99%
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“…In the investigation of the performance of the BSW sensor, the reflectance, sensitivity, field distribution as well as figure of merit (FOM) are analyzed through the transfer-matrix method (TMM). [34,35] The EM fields of the transfer-matrix polarized wave (H x = H z = 0, E y = 0) in each layer ( j) can be described as…”
Section: Theoretical Background and Modelmentioning
confidence: 99%
“…x . [35] The propagation matrix that propagates freely through a given material is given by The dynamic matrix that propagates through the boundary of two dielectrics is defined as…”
Section: Theoretical Background and Modelmentioning
confidence: 99%