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Frontiers of Optoelectronics

ISSN 2095-2759

ISSN 2095-2767(Online)

CN 10-1029/TN

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Front. Optoelectron.    2019, Vol. 12 Issue (1) : 88-96    https://doi.org/10.1007/s12200-017-0730-8
REVIEW ARTICLE
Detection of photonic orbital angular momentum with micro- and nano-optical structures
Chenhao WAN1,2, Guanghao RUI3, Jian CHEN2,4, Qiwen ZHAN2,5()
1. School of Optical and Electronic Information, Huazhong University of Science and Technology, Wuhan 430074, China
2. Department of Electro-Optics and Photonics, University of Dayton, 300 College Park, Dayton, Ohio 45469, USA
3. Advanced Photonics Center, Southeast University, Nanjing 210096, Jiangsu, China
4. School of Electronic Engineering, University of Electronic Science and Technology of China, Chengdu 611731, China
5. School of Optical-Electrical and Computer Engineering, University of Shanghai for Science and Technology, Shanghai 200093, China
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Abstract

Light with an optical orbital angular momentum (OAM) has attracted an increasing amount of interest and has found its way into many disciplines ranging from optical trapping, edge-enhanced microscopy, high-speed optical communication, and secure quantum teleportation to spin-orbital coupling. In a variety of OAM-involved applications, it is crucial to discern different OAM states with high fidelity. In the current paper, we review the latest research progress on OAM detection with micro- and nano-optical structures that are based on plasmonics, photonic integrated circuits (PICs), and liquid crystal devices. These innovative OAM sorters are promising to ultimately achieve the miniaturization and integration of high-fidelity OAM detectors and inspire numerous applications that harness the intriguing properties of the twisted light.

Keywords orbital angular momentum (OAM)      optical vortices      singular optics      spatial light modulator      surface plasmon polariton (SPP)      holography      photonic integrated circuit (PIC)     
Corresponding Author(s): Qiwen ZHAN   
Just Accepted Date: 17 August 2017   Online First Date: 12 September 2017    Issue Date: 29 April 2019
 Cite this article:   
Chenhao WAN,Guanghao RUI,Jian CHEN, et al. Detection of photonic orbital angular momentum with micro- and nano-optical structures[J]. Front. Optoelectron., 2019, 12(1): 88-96.
 URL:  
https://academic.hep.com.cn/foe/EN/10.1007/s12200-017-0730-8
https://academic.hep.com.cn/foe/EN/Y2019/V12/I1/88
Fig.1  (a) Schematic of light with spiral phase. The insets are the transverse intensity profiles of Laguerre-Gaussian (LG) modes with different |l|. (b) Schematic of experimental setup. The plasmonic lens is excited by LG modes from the SiO2 substrate side and imaged by a NSOM probe working on collection mode. Inset 1 is the diagram of a single ring plasmonic lens and the coordinates used in analytical derivation. The illumination is along the z-direction. Inset 2 is the scanning electronic microscope micrograph of the plasmonic lens fabricated in gold film on SiO2 substrate. Adapted from Ref. [19]
Fig.2  Intensity distributions of the optical field near the plasmonic lens surface excited by photons with different OAMs. (a)−(e) are the NSOM images for l = 0, +1, −1, +2 and −2, respectively. (f)−(j) are the corresponding numerical simulation results. The excitation polarization is shown by the white arrow in (a). The scale bar in (f) and the color bar in (j) are also applicable to the other images of intensity distributions. Adapted from Ref. [19]
Fig.3  (a) Schematic of the metahologram. The holographic pattern has four sectors, which are designed by considering the interference between a converging SP wave with a vortex beam carrying different OAMs. The inset corresponds to the designed TC for each sector. (b) Binary version of the interferogram. Adapted from Ref. [20]
Fig.4  Numerical simulations of the SP intensity distribution of the metahologram for circularly polarized illumination with a TC of 1. Adapted from Ref. [20]
Fig.5  Lookup table for identifying incident OAM by encoding the OAM mode with discretized signal levels. Adapted from Ref. [20]
Fig.6  Diagram of the proposed OAM receiver. The circular resonator with angular gratings patterned along the inner wall couples the normally incident azimuthally polarized vortex beam to an access waveguide. Adapted from Ref. [26]
Fig.7  Receiving spectrum of the OAM receiver. Adapted from Ref. [26]
Fig.8  Resonant wavelengths for vortex beam with different SAMs. Adapted from Ref. [26]
Fig.9  Diagram of the composite OAM receiver that has a (a) GeSe annular film and (b) GeSe gratings consist of alternate states on top of the resonator as the cladding layer. The duty cycle of the gratings is 0.5. Adapted from Ref. [26]
Fig.10  Receiving spectrum of the composited device shown in Fig. 5(a) when the GeSe is in (a) amorphous state and (b) crystal state, respectively. Adapted from Ref. [26]
Fig.11  Comparison of two high-resolution OAM sorters. (a) Previous demonstrations with four custom refractive/diffractive elements (log-polar mapper, mapper corrector, fan-out element, fan-out corrector) and three lenses in between. (b) The novel scheme with only two custom phase elements (quadratic fan-out mapper, dual-phase corrector) and no lens in between. Adapted from Ref. [39]
Fig.12  Numerical simulation and experimental results for the three-copy fan-out case of OAM sorting. (a) Simulation results show that different OAM modes (l = −2, −1, 0, 1 and 2) are sorted into a set of parallel lines with various vertical positions. (b) Experimental results verify the simulation results. All experimental images use the same scale bar and coordinates. Adapted from Ref. [39]
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