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Spatial shifts of reflected light beam on black phosphorus/hexagonal boron nitride structure

•The GH-shift for s- and p-polarized incidence can reach the maximum near the ENZ.•We can control the GH-shift from positive to negative or even to zero by adjusting the performance of BP.•The IF-shift for the s- and p-polarized incidence can be excited and greatly improved. We examined Goos-Hänchen...

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Published in:Optics and laser technology 2023-04, Vol.159, p.108968, Article 108968
Main Authors: Li, Yu-bo, Song, Hao-yuan, Zhang, Yu-qi, Zhou, Sheng, Fu, Shu-fang, Zhang, Qiang, Wang, Xuan-Zhang
Format: Article
Language:English
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Summary:•The GH-shift for s- and p-polarized incidence can reach the maximum near the ENZ.•We can control the GH-shift from positive to negative or even to zero by adjusting the performance of BP.•The IF-shift for the s- and p-polarized incidence can be excited and greatly improved. We examined Goos-Hänchen (GH) and Imbert-Fedorov (IF) shifts of the reflective beam from the hexagonal boron nitride (hBN) covered by black phosphorus (BP) layers, where the BP layers are rotated by an angle with respect to the incident plane. The interaction of phonon polaritons in hBN and plasmon polaritons in BP, as well as the structure surface and interface between the two media determines the two shifts. In the common frequency–response range of the BP and hBN, the GH- and IF-shifts can be very large in the vicinity of epsilon-near-zero (ENZ) for a linearly-polarized incidence. The GH-shift can be continuously tuned from positive to negative or even to zero at a fixed frequency by adjusting the electron density and anisotropic axis-orientation of the BP. Another fascinating phenomenon is that the IF-shift can be not only excited by the linearly-polarized incidence but also greatly improved, even up to -156λ0. These conclusions are applicable to the other 2D anisotropic materials, which will become a guidance of new polarization-dependent, anisotropic optoelectronics devices.
ISSN:0030-3992
1879-2545
DOI:10.1016/j.optlastec.2022.108968