Yue Jiang’s research while affiliated with Nanjing University and other places

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Publications (4)


Overview of metasurface polarization optics. Metasurface provides a versatile platform for desired classical and quantum polarized source, manipulation, and detection devices, which are able to control the polarization of light in terms of either uniform polarized beam or structured spatially varying polarization profiles. Typical examples for polarized light source include circular polarization laser,⁵² polarization entangled photon-pair sources⁵⁷ with efficient and on-demand uniform polarized beam generation. Metasurface polarization manipulation devices include basic uniform polarization optical elements such as meta-waveplates⁵³ and vectorial holography elements⁵⁵ in classic regime and entanglement modulation⁶² and tomography devices⁵⁸ in quantum regime. In terms of metasurface polarization detection, single-shot full-Stokes parameters detector and imager⁶³ and multi-photon quantum entanglement state tomography³⁵ are widely explored.
(a) Schematic of polarization ellipse. (b) Schematic of Poincaré sphere and the representation of a polarization state P (2  ψ, 2  χ) that located on the sphere.
(a) Schematic of solid Poincaré ball. (b) Polarization ellipses for polarization states varies from (left) fully polarized (upper panel: linear, lower panel: circular) to (right) unpolarized.
Birefringent metasurface waveplates. (a) Left panel: a schematic of a reflective metasurface HWP consisting of Si nanopillars, a PMMA spacer, and an Ag film as a highly efficient reflector. Right panel: the cross- and co-polarization reflection spectra of the designed metasurface. Reproduced with permission from Yang et al., Nano Lett. 14(3), 1394–1399 (2014). Copyright 2014 American Chemical Society.⁶⁵ (b) Left panel: schematic of the all-dielectric metasurface HWP made of Si nanopolars. Right panel: experimental and theoretical transmission spectra of the designed metasurface. Reproduced with permission from APL Photonics 1(3), 030801 (2016). Copyright 2016 AIP Publishing LLC.⁶⁷ (c) Left panel: a scheme of the reflective background-free metasurface QWP that is composed of two Au V-shaped nano-antenna unit cell. Right panel: simulated phase difference and the ratio of amplitudes between the two reflective waves with broadband performance. Reproduced with permission from Yu et al., Nano Lett. 12(12), 6328–6333 (2012). Copyright 2012 American Chemical Society.⁷⁰ (d) Left panel: schematic of the bilayer dielectric metasurface for high efficient QWP design. Right panel: simulated phase difference between cross- and co-polarization transmission coefficients under x-polarization incident beam. Reprinted with permission from Zhou et al., Light: Sci. Appl. 8(1), 80 (2019). Copyright 2019 Author(s), licensed under a Creative Commons Attribution 4.0 License.⁷¹ (e) Left panel: schematic of angle-dependent birefringent metasurface waveplate for continuous polarization conversion consisting of optimized freeform meta-atoms. Right panel: experimental retardance with eigen-polarization state incidence. Reprinted with permission from Shi et al., Sci. Adv. 6(23), eaba3367 (2020). Copyright 2020 AAAS.⁵³ (f) Left panel: a scheme of multi-channel polarization conversion based on metagrating consisting of L-shaped scalable metallic meta-atoms. Right panel: experimental intensity ratio between target polarization and its orthogonal polarization in each diffraction order within designed wavelength region. Reprinted with permission from Gao et al., Phys. Rev. X 10(3), 031035 (2020). Copyright 2020 American Physical Society.⁷³
Dichroism metasurface polarizer. (a) Gold helix nanostructure for the circular polarizer. Reprinted with permission from Gansel et al., Science 325(5947), 1513–1515 (2009). Copyright 2009 AAAS.⁷⁴ (b) Circular dichroism in planar chiral nanostructure made of copper strips arises from different conversion efficiencies of circular polarization. Reprinted with permission from Zheludev et al., Phys. Rev. Lett. 97(16), 167401 (2006). Copyright 2006 American Physical Society.⁷⁷ (c) Large chiroptical effects in L-shaped gold nanostructures based on multimode interference. Reprinted with permission from Zhang et al., Phys. Rev. Appl. 7(5), 054003 (2017). Copyright 2017 American Physical Society.⁸⁵ (d) Strong chiral response induced by the spin-dependent destructive and constructive interference in dielectric birefringent metasurface. Reprinted with permission from Kenney et al., Adv. Mater. 28(43), 9567–9572 (2016). Copyright 2016 Author(s), licensed under a Creative Commons Attribution 4.0 License.⁸⁰ (e) Giant circular polarization dichroism induced by the spin-dependent destructive and constructive interference based on planar dielectric metasurface. Reprinted with permission from Zhang et al., Adv. Funct. Mater. 27(47), 1704295 (2017). Copyright 2017 Author(s), licensed under a Creative Commons Attribution 4.0 License.⁸¹ (f) Arbitrary polarization conversion dichroism metasurfaces for surface Poincaré sphere polarizers. Reprinted with permission from Wang et al., Light: Sci. Appl. 10(1), 24 (2021). Copyright 2021 Author(s), licensed under a Creative Commons Attribution 4.0 License.⁸² (g) Metasurface manipulating both DOP and SOP for full solid Poincaré sphere polarizer. Reprinted with permission from Wang et al., Phys. Rev. Lett. 130(12), 123801 (2023). Copyright 2023 American Physical Society.⁸⁴

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Metasurface polarization optics: From classical to quantum
  • Article
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December 2024

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387 Reads

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4 Citations

Feng-Jun Li

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Rui Zhong

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Metasurface polarization optics, manipulating polarization using metasurfaces composed of subwavelength anisotropic nanostructure array, has enabled a lot of innovative integrated strategies for versatile and on-demand polarization generation, modulation, and detection. Compared with conventional bulky optical elements for polarization control, metasurface polarization optics provides a feasible platform in a subwavelength scale to build ultra-compact and multifunctional polarization devices, greatly shrinking the size of the whole polarized optical system and network. Here, we review the recent progresses of metasurface polarization optics in both classical and quantum regimes, including uniform and spatially varying polarization-manipulating devices. Basic polarization optical elements such as meta-waveplate, meta-polarizer, and resonant meta-devices with polarization singularities provide compact means to generate and modulate uniform polarization beams. Spatial-varying polarization manipulation by employing the pixelation feature of metasurfaces, leading to advanced diffraction and imaging functionalities, such as vectorial holography, classic and quantum polarization imaging, quantum polarization entanglement, quantum interference, and modulation. Substituting conventional polarization optics, metasurface approaches pave the way for on-chip classic or quantum information processing, flourishing advanced applications in displaying, communication, imaging, and computing.

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Implement quantum tomography of polarization-entangled states via nondiffractive metasurfaces

August 2022

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95 Reads

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5 Citations

Traditional optical elements, such as waveplates and polarization beam splitters, are essential for quantum state tomography (QST). Yet, their bulky size and heavy weight are prejudicial for miniaturizing quantum information systems. Here, we introduce nondiffractive silicon metasurfaces with high transmission efficiency to replace the traditional optical elements for QST of polarization-entangled states. Two identical silicon metasurfaces are employed, and each metasurface comprises four independent districts on a micrometer scale. The unit cell of each district consists of two silicon nanopillars with different geometrical sizes and orientation angles, and the interference of the scattered waves from the nanopillars leads to a single output beam from the district with a specific polarization state with a transmission efficiency above 92%. When the two-photon polarization-entangled state shines on different districts of two metasurfaces, each photon of the photon pair interacts with the local nanopillars within the district, and the two-photon state is projected onto 16 polarization bases for state reconstruction. We experimentally demonstrate the reconstruction of four input Bell states with high fidelities. This approach significantly reduces the number of conventional optical components in the QST process and is inspiring for advancing quantum information technology.


Multichannel Distribution and Transformation of Entangled Photons with Dielectric Metasurfaces

July 2022

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151 Reads

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31 Citations

Physical Review Letters

Photonic quantum information processing relies on operating the quantum state of photons, which usually involves bulky optical components unfavorable for system miniaturization and integration. Here, we report on the transformation and distribution of polarization-entangled photon pairs with multichannel dielectric metasurfaces. The entangled photon pairs interact with metasurface building blocks, where the geometrical-scaling-induced phase gradients are imposed, and are transformed into two-photon entangled states with the desired polarization. Two metasurfaces, each simultaneously distributing polarization-entangled photons to spatially separated multiple channels M (N), may accomplish M×N channels of entanglement distribution and transformation. Experimentally we demonstrate 2×2 and 4×4 distributed entanglement states, including Bell states and superposition of Bell states, with high fidelity and strong polarization correlation. We expect this approach paves the way for future integration of quantum information networks.


The THz photonic crystal and its bulk band diagram. (a) Schematic of the THz photonic crystal, which was composed of metal cylinders. The red dashed line denotes a unit cell. The diameter of the cylinder was d = 250 μm, the distance between adjacent cylinders was t = 300 μm, and the lattice constant was a = 750 μm. The rotation angle θ of metal cylinder location is the angle between one of principal axes of the unit cell and the x-axis. (b) Bulk band structure of the photonic crystals with θ = 0° (black dashed line), and θ = ±30° (solid red line). (c) Phase profiles at the K valley of the two lowest bulk bands for VPC1 (θ = 30°) and VPC2 (θ = -30°). The color scale shows z-oriented magnetic field Hz, and the blue and red arrows respectively denote LCP and RCP states. (d) Calculated eigenfrequencies of LCP (red curve) and RCP (blue curve) states at the K valley when θ varied.
Topologically protected edge waves with different valley polarization. (a) Distribution of Berry curvature of VPC1 (left panel) and distribution of Berry curvature of VPC2 (right panel). (b) Dispersion relation for the ribbon-shaped supercell comprising 20 unit cells with domain walls in the center. The shaded regions represent the projected bulk dispersions, and the solid/dashed lines represent Type-A/Type-B interfaces. (c) Schematics of supercells with different interfaces. The magnified area shows the intensity distribution of |Hz| near the interface at the K valley and the Poynting power flow denoted by the black arrows.
Transmission measurements for THz VPCs. (a) Photograph of a fabricated sample, where the inset is a magnification to show the detailed structure. (b) Assembled experimental sample, where the inset is a partial enlargement of the sample. (c) Experimental setup used to perform transmittance measurements. (d) The magnified photograph corresponds to the red dotted frame in (c). (e) Calculated dispersion relation for the bulk VPC1 sample along with k//; the light-blue shadowed region corresponds to the bulk bandgap, and the red line are artificially labeled light cone. (f) Measured dispersion map for VPC1, the gray dotted area represents the bulk bandgap, and the black line represents the light cone.
Simulated and experimental results for the evaluation of topological transport robustness. (a)–(c) Simulated intensity distribution results for |Hz| field at 0.21 THz for a straight interface (a), disordered interface (b), and bending interface (c); each inset shows a top view of each of the three topologically distinct interfaces. (d) Measured time-domain spectra for THz radiation transmitted through a straight interface (red curve) and through the bulk, which did not contain an interface (black curve). (e) Measured transmittance results for the four different interface conditions, i.e., the straight interface (red curve), disordered interface (blue curve), bending interface (green curve), and no interface (black curve). (f) The phase shift results were measured for the four different configurations with respect to waves that were freely propagating through air.
Simulated and experimental topological results for the valley-dependent edge states. (a) Schematic of the topological multi-channel intersections; the black and green arrows respectively denote the direction of THz wave propagation at the K and K’ valleys. (b) The simulated intensity distribution of |Hz| field. (c) The measured time-domain spectral results for THz radiation transmission by different ports; the red, black, and blue curves respectively correspond to the time-domain spectra measured from Port 1, 2, and 3. (d) The measured transmittance from Port 1, 2, and 3; the blue shaded region denotes the bulk bandgap.
Direct observation of terahertz topological valley transport

April 2022

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67 Reads

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16 Citations

Topological photonics offers the possibility of robust transport and efficiency enhancement of information processing. Terahertz (THz) devices, such as waveguides and beam splitters, are prone to reflection loss owing to their sensitivity to defects and lack of robustness against sharp corners. Thus, it is a challenge to reduce backscattering loss at THz frequencies. In this work, we constructed THz photonic topological insulators and experimentally demonstrated robust, topologically protected valley transport in THz photonic crystals. The THz valley photonic crystal (VPC) was composed of metallic cylinders situated in a triangular lattice. By tuning the relevant location of metallic cylinders in the unit cell, mirror symmetry was broken, and the degenerated states were lifted at the K and K’ valleys in the band structure. Consequently, a bandgap of THz VPC was opened, and a nontrivial band structure was created. Based on the calculated band structure, THz field distributions, and valley Berry curvature, we verified the topological phase transition in such type of THz photonic crystals. Further, we showed the emergence of valley-polarized topological edge states between the topologically distinct VPCs. The angle-resolved transmittance measurements identified the bulk bandgap in the band structure of the VPC. The measured time-domain spectra demonstrated the topological transport of valley edge states between distinct VPCs and their robustness against bending and defects. Furthermore, experiments conducted on a topological multi-channel intersectional device revealed the valley-polarized characteristic of the topological edge states. This work provides a unique approach to reduce backscattering loss at the THz regime. It also demonstrates potential high-efficiency THz functional devices such as topologically protected beam splitters, low-loss waveguides, and robust delay lines.

Citations (4)


... Utilizing this unique functionality, a miniaturized and simplified two-photon polymerization (TPP) system was developed and demonstrated efficient multi-focus parallel processing [13] . Wavelength and polarization information can be independently encoded into each focal point, enabling the development of compact spectrometer [14] and polarization-resolved device [15] . More importantly, metalensbased optical trapping arrays have emerged as a powerful platform for the preparation and manipulation of ultracold atoms [16,17] , enabling multifunctional control in complex quantum information experiments. ...

Reference:

Scalable manufacturing of polarization-insensitive metalenses with high-uniform focal arrays in the visible
Metasurface polarization optics: From classical to quantum

... Typical examples for polarized light source include circular polarization laser, 52 polarization entangled photon-pair sources 57 with efficient and on-demand uniform polarized beam generation. Metasurface polarization manipulation devices include basic uniform polarization optical elements such as meta-waveplates 53 and vectorial holography elements 55 in classic regime and entanglement modulation 62 and tomography devices 58 in quantum regime. In terms of metasurface polarization detection, singleshot full-Stokes parameters detector and imager 63 and multi-photon quantum entanglement state tomography 35 are widely explored. ...

Implement quantum tomography of polarization-entangled states via nondiffractive metasurfaces
  • Citing Article
  • August 2022

... They enable precise manipulation and control over the amplitude, phase, and polarization of light, allowing for the realization of complex optical functions using ultrathin devices [35][36][37][38][39][40][41][42] . The ability of metasurfaces to simultaneously perform multi-DOFs manipulation makes them particularly advantageous for quantum applications, as they can be tailored to generate specific quantum states with high fidelity [43][44][45][46][47][48][49][50][51][52][53] . However, the full potential of metasurfaces in the context of quantum entanglement can be further explored. ...

Multichannel Distribution and Transformation of Entangled Photons with Dielectric Metasurfaces
  • Citing Article
  • July 2022

Physical Review Letters

... Potential applications of topological quantum states [15,16], such as quantum computing, have also been proposed. Topological photonic crystals have great potential for development in topological angular states [17][18][19], topological valley states [20][21][22], and brittle topologies [23]. In 2008, Haldane and Raghu [24] opened the Dirac point by breaking the timereversal symmetry (TRS) of the system and realized the first topological phase transition in an optical system. ...

Direct observation of terahertz topological valley transport