2018
DOI: 10.1103/physrevapplied.10.024032
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Two-Dimensional Photonic Devices based on Bloch Surface Waves with One-Dimensional Grooves

Abstract: Both experiments and simulations show that the polarization state and propagation path of the Bloch surface waves sustained on a dielectric multilayer, can be manipulated with the grooves inscribed on this multilayer. These grooves can be easily producible, accessible and controllable. Various nano-devices for the Bloch surface waves, such as the launcher, beam splitter, reflector, polarization rotator, and even the photonic single-pole double-throw switch, were all experimentally realized with the properly de… Show more

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Cited by 26 publications
(16 citation statements)
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“…The free space wavelength of the device is λ 0 =1555 nm. The layer stack is designed to sustain a BSW with TE polarization, and an extension of our results to TM polarization is feasible 23,24 . The effective index without/with the device layer amounts to and , and this defines the wavelength of the BSW .…”
Section: Resultsmentioning
confidence: 95%
“…The free space wavelength of the device is λ 0 =1555 nm. The layer stack is designed to sustain a BSW with TE polarization, and an extension of our results to TM polarization is feasible 23,24 . The effective index without/with the device layer amounts to and , and this defines the wavelength of the BSW .…”
Section: Resultsmentioning
confidence: 95%
“…29 For practical fabrication, according to the reported works, one-dimensional multilayered con¯guration of centimeter long in the transverse directions can work for investigations within an area $ 100 Â 100 m 2 . 30,31 In addition, the graphene monolayer with a practical area of $ 0:5 Â 0:5 mm 2 has been experimentally reported. 32 Figure 2 shows the absorption (A), re°ection (R), and transmission (T ) of the two composited \atoms" (EGBC and BCBC) as well as the whole structure EG(BC) 2 with incident angle ¼ 60 under TE polarization.…”
Section: Resultsmentioning
confidence: 99%
“…The free space wavelength of the device is λ 0 =1555 nm. The layer stack is designed to sustain a BSW with TE polarization, and an extension of our results to TM polarization is feasible 23,24 . The effective index without/with the device layer amounts to n w=o eff ¼ 1:1 and n w eff ¼ 1:2, and this defines the wavelength of the BSW…”
Section: Designmentioning
confidence: 99%