2016
DOI: 10.1364/oe.24.006749
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Ultracompact high-efficiency polarising beam splitter based on silicon nanobrick arrays

Abstract: Since the transmission of anisotropic nano-structures is sensitive to the polarisation of an incident beam, a novel polarising beam splitter (PBS) based on silicon nanobrick arrays is proposed. With careful design of such structures, an incident beam with polarisation direction aligned with the long axis of the nanobrick is almost totally reflected (~98.5%), whilst that along the short axis is nearly totally transmitted (~94.3%). More importantly, by simply changing the width of the nanobrick we can shift the … Show more

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Cited by 42 publications
(18 citation statements)
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“…The advanced anisotropy manipulation of metasurfaces indicates the capability of achieving dual polarization multiplexing for two beams of orthogonal LP light. For example, by changing the arm length of a cross-shaped nanostructure 18,19 or the dimensions of a nanoscale pillar [20][21][22][23][24] , the phase or amplitude of orthogonal LP light can be independently controlled, and then, polarizing beam splitters 18,20 , dualchannel nanoprinting devices 19,21,22 , step-zoom lenses 23 , 3D holograms 24 , and devices with other functionalities can be realized. Furthermore, the phase of orthogonal CP light 25 , any orthogonal polarized light 26 , or even nonorthogonal polarized light 27 can be independently modulated in two polarization modes by simultaneously elaborately designing the dimensions and orientations of nanostructures.…”
Section: Introductionmentioning
confidence: 99%
“…The advanced anisotropy manipulation of metasurfaces indicates the capability of achieving dual polarization multiplexing for two beams of orthogonal LP light. For example, by changing the arm length of a cross-shaped nanostructure 18,19 or the dimensions of a nanoscale pillar [20][21][22][23][24] , the phase or amplitude of orthogonal LP light can be independently controlled, and then, polarizing beam splitters 18,20 , dualchannel nanoprinting devices 19,21,22 , step-zoom lenses 23 , 3D holograms 24 , and devices with other functionalities can be realized. Furthermore, the phase of orthogonal CP light 25 , any orthogonal polarized light 26 , or even nonorthogonal polarized light 27 can be independently modulated in two polarization modes by simultaneously elaborately designing the dimensions and orientations of nanostructures.…”
Section: Introductionmentioning
confidence: 99%
“…The polarization efficiency, defined as 71 , is evaluated as η = 97%, η = 99% and η = 96% in the visible region for the 533, 600 and 750 nm polarizing beam splitters, respectively, and η = 88% in the near-IR region for the λ 0 = 900 nm polarizer. Transmission/reflection flat-optics polarizers reaching polarization efficiencies of this high have only been reported in the near-IR around λ = 1500 nm 72,73 , where silicon has no losses. The approach presented in this work obtained similar results in the visible range at wavelengths at which Si is highly absorbing, proving to be a successful path to address the loss problem of high refractive index semiconductors in the design of highly efficient flat optics in the visible region.…”
Section: Resultsmentioning
confidence: 99%
“…Although the phase manipulation of GEMS is independent of the dimensions of nanostructures, the combination of geometric phase and Mie resonance can provide a new approach for lightwave manipulation. In 2016, Zheng et al designed a dielectric nanostructure acting as nanopolarizer [78]. As Mie resonance occurs along the long axis of the nanostructure, it can reflect and transmit most of incident light polarized along the long and short axes, respectively.…”
Section: P-b Phase With Dielectricsmentioning
confidence: 99%