Ya-Jun Gao’s research while affiliated with Nanjing University and other places

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Publications (11)


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

August 2022

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95 Reads

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5 Citations

Zheng Wang

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Yue Jiang

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Ya-Jun Gao

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[...]

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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.



Metasurface design for the generation of an arbitrary assembly of different polarization states

September 2021

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68 Reads

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14 Citations

Manipulation of polarization states with metasurfaces is a compelling approach for on-chip photonics and portable information processing. Yet it remains challenging to generate different types of polarization states with a single piece of a metasurface. This paper demonstrates a metasurface to resolve this issue, which is made of L-shaped resonators with different geometrical sizes. Each resonator diffracts a right- or left-handed circularly polarized state with an additional geometrical-scaling-induced phase. The type of polarization state of each diffracted beam is determined by the enantiomorphism, size, and spatial sequence of the resonators in the unit cell. The number of the beams is modulated by the geometry and separation of the resonators. We provide examples to illustrate how to achieve the specific number of diffracted beams with the desired polarization states in experiments. We suggest that this strategy can be applied for integrated photonics and portable quantum information processing.


Fig. 1. The principle of RFMs and the visual effects in reflection and transmission. (A) shows that the RFM allows transmission like a smooth surface and reflection like a frosted surface. In (B) and (C) illustrations demonstrate the visual effects in reflection and transmission for a flat glass, a frosted glass, and an RFM, respectively. In (B), the illuminating lamp and the object are in front of the glass and metasurface, whereas in (C), they are behind the glass and metasurface.
Fig. 3. The design of an RFM and the numerical verifications. (A) Three-dimensional illustration of a double-layer RFM based on two complementary arrays of gold nanorods, which can be regarded as a random binary map (the bottom left inset) of the heads and tails. The bottom right inset shows a zoom-in view of the corner of the RFM. (B) The detailed structures of the heads and tails. (C) Transmittance and transmission phase of the heads and tails. (D) Reflectance and reflection phase of the heads and tails. (E) Transmittance at the condition of  = 180° as a function of the radius of the gold nanorods. (F) Far-field radiation power patterns for a PHM (top) and an RFM (bottom) under the illumination of a TE-polarized Gaussian beam at the incident angle (marked by white arrow) of  i = 0°, 10°, 20°, and 30°, respectively.
Fig. 4. Transmission and reflection experiments for the RFM and PHM. (A) SEM images of a part of the fabricated RFM. The inset graph shows the zoom-in view of the RFM. (B) The intensity profiles of the transmitted (left column) and reflected beams (right column) for the RFM (top) and PHM (bottom). The incident laser beam is controlled by an aperture diaphragm. The measured optical power is depicted in the corresponding panels. (C) Schematic graph of the angular distribution measurement setup. (D) The measured angular distributions of the light intensity for the RFM and PHM under the incident angles of 10°, 20°, and 30°, respectively.
Fig. 5. Imaging experiments for the RFM and PHM. (A) The schematic graphs of the measurement setups in transmission (left) and reflection (right), respectively. (B) The optical photographs of the rabbit and dog patterns, which are used as the objects in transmission and reflection, respectively. (C and D) The photo images captured with a microscope from the RFM (top) and PHM (bottom) in the transmission (C) and reflection (D) setups, respectively. (E) The photo image of a USAF 1951 resolution test chart captured from the RFM in the transmission setup. The central wavelengths of the illuminating light are 520 nm, 550 nm, 600 nm, 700 nm, 800 nm (false color), and 850 nm (false color), respectively.
Diffuse reflection and reciprocity-protected transmission via a random-flip metasurface
  • Article
  • Full-text available

September 2021

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653 Reads

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64 Citations

Science Advances

Rough surfaces lead to diffused light in both reflection and transmission, thereby blurring the reflected and transmitted images. Here, we merge the traditionally incompatible diffuse reflection and undistorted transmission by introducing the concept of random-flip metasurfaces made of randomly flipped components. These metasurfaces have a globally random phase in reflection that leads to diffuse reflection, while the local space inversion and reciprocity principle ensure distortion-free transmission. Notably, the metasurface reflects like a rough surface yet transmits like a smooth one in a broad spectrum. On the basis of complementary random arrays of gold nanorods, we verified this functionality by both optical spectroscopy and imaging experiments over a broad range of frequencies from the visible to the infrared regime. This feature, which originates from breaking the phase correlation between reflection and transmission by the metasurface, could enable a range of new optical materials and display technology.

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Electrically Driven Tunable Broadband Polarization States via Active Metasurfaces Based on Joule‐Heat‐Induced Phase Transition of Vanadium Dioxide

August 2021

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201 Reads

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90 Citations

Laser & Photonics Review

Broadband tuning of polarization states is pivotal yet challenging in modern photonics technologies, especially for miniaturized or integrated systems. Metasurfaces potentially provide an effective approach to resolve this challenge. However, once a metadevice is fabricated, its functionalities are determined, and it is hard to actively tune the polarization states. Here, the electrically tunable broadband polarization states by combining phase‐change material (vanadium dioxide) and dispersion‐free metasurface are demonstrated for the first time. The polarization states are modulated through the electrically driven, Joule‐heat‐induced phase transition of vanadium dioxide, where the output polarization state can be continuously tuned from horizontal one to vertical one, or from circular polarization to linear polarization. With accurate on‐chip control of the phase transition, continuous and reversible modulation of polarization is verified in a scanning display. Moreover, a proof‐of‐concept demonstration for dynamically independent control of multiple polarization display is carried out. Different images are produced by applying electrical currents in N separate channels to generate a dynamic multiplexing polarization display with 2N encoding states. Such an active metasurface can be readily integrated with electronics and has potential applications in display, encryption, camouflage, and information processing. Electrically driven tunable broadband polarization states are demonstrated by combining vanadium dioxide and dispersion‐free metasurface. The polarization states of reflected light can be continuously modulated from horizontal polarization to perpendicular polarization or from circular polarization to linear polarization through the electrically tuned phase transition of vanadium dioxide. Such an active metasurface can be applied in display, encryption, and information processing.




Simultaneous Generation of Arbitrary Assembly of Polarization States with Geometrical-Scaling-Induced Phase Modulation

August 2020

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269 Reads

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54 Citations

Physical Review X

Manipulating the polarization of light on the microscale or nanoscale is essential for integrated photonics and quantum optical devices. Nowadays, the metasurface allows one to build on-chip devices that efficiently manipulate the polarization states. However, it remains challenging to generate different types of polarization states simultaneously, which is required to encode information for quantum computing and quantum cryptography applications. By introducing geometrical-scaling-induced (GSI) phase modulations, we demonstrate that an assembly of circularly polarized (CP) and linearly polarized (LP) states can be simultaneously generated by a single metasurface made of L-shaped resonators with different geometrical features. Upon illumination, each resonator diffracts the CP state with a certain GSI phase. The interaction of these diffractions leads to the desired output beams, where the polarization state and the propagation direction can be accurately tuned by selecting the geometrical shape, size, and spatial sequence of each resonator in the unit cell. As an example of potential applications, we show that an image can be encoded with different polarization profiles at different diffraction orders and decoded with a polarization analyzer. This approach resolves a challenging problem in integrated optics and is inspiring for on-chip quantum information processing.


Simultaneous Generation of Arbitrary Assembly of Polarization States with Geometrical-Scaling-Induced Phase Modulation

May 2019

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47 Reads

Manipulating the polarization of light on the micro/nano scale is essential for integrated photonics and quantum optical devices. Nowadays, metasurface allows building on-chip devices that may efficiently manipulate polarization states. However, it remains challenging to generate different types of polarization states simultaneously, which is required for encoding information for quantum computing and quantum cryptography applications. By introducing geometrical-scaling-induced (GSI) phase modulations, we demonstrate here that an assembly of circularly polarized (CP) and linearly polarized (LP) states can be simultaneously generated by a single metasurface made of L-shaped resonators with different geometrical sizes. Upon illumination, each resonator diffracts CP state with a certain GSI phase. The interaction of these diffractions leads to the desired output beams, where the polarization state and the propagation direction can be accurately tuned by selecting the geometrical shape, size and the spatial sequence of each resonator in the unit cell. This approach resolves a challenging problem in integrated optics and is inspiring for on-chip quantum information processing.


Citations (7)


... 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. ...

Reference:

Metasurface polarization optics: From classical to quantum
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

... Metasurfaces are two-dimensional arrays of subwavelength resonators that can interact with incident electromagnetic waves and exhibit distinct electromagnetic properties [1][2][3][4]. Since the pioneering works of metasurfaces that generalized the laws of reflection and refraction by introducing a gradient phase along a surface [5][6][7], many efforts have been devoted to exploring their potential functionalities, including controlling the polarization state [8][9][10][11][12][13], the amplitude [14][15][16][17], and the wavefront [18,19] of electromagnetic waves, etc. Nevertheless, due to the resonant nature of meta-atoms, most of the previous metasurfaces work in a relatively narrow band, except for some designs based on principles or techniques such as the Pancharatnam-Berry phase [18,20], achromatic designs [21][22][23][24][25], reciprocity protection [26][27][28][29][30] and spatial inversion [28][29][30], etc. ...

Metasurface design for the generation of an arbitrary assembly of different polarization states
  • Citing Article
  • September 2021

... To elucidate the essential role of parity transformation, we compare it with the mirror operation, i.e., upside-down flip, namely ( , , ) → ( , , − ). When the meta-structure exhibits a 4 symmetry in the xy-plane, there is no difference between ( , , ) → (− , − , − ) and ( , , ) → ( , , − ) [46,47]. However, the difference becomes huge when the meta-structure has no symmetry, which is the case here. ...

Diffuse reflection and reciprocity-protected transmission via a random-flip metasurface

Science Advances

... The reversible phase transition of VO 2 can also be triggered by electrical and optical excitations. Due to the significant change in the refractive index and conductivity, VO 2 has been integrated with metallic structures to create a range of tunable optical devices, including memory metamaterials [30], switchable absorbers [31][32][33][34], active waveplates [35], tunable chirality [36], reconfigurable wavefronts [37][38][39], reconfigurable extraordinary transmission [40], and tunable optical limiters [41]. Furthermore, the enhancement of terahertz electric fields within metallic structures can facilitate the insulator-metal transition of VO 2 [42]. ...

Electrically Driven Tunable Broadband Polarization States via Active Metasurfaces Based on Joule‐Heat‐Induced Phase Transition of Vanadium Dioxide
  • Citing Article
  • August 2021

Laser & Photonics Review

... Steering photon propagation, with the active manipulation of optical fields and high processing speed, has been successfully applied in modern signal transmission, imaging, memory, cryptography, etc. [1][2][3][4] . The evolution of photon propagation science to a practical technology promises extreme advantages for specific applications in integrated optical circuits [5][6][7] , nano-antennas [8][9][10][11][12] , nanolasers [13][14][15] , etc. In the development of photon manipulation technology, it is substantial to find a proper method with features of high-level integration and a large storage capacity, to satisfy the need for information transmission and processing applications [16][17][18][19] . ...

Simultaneous Generation of Arbitrary Assembly of Polarization States with Geometrical-Scaling-Induced Phase Modulation

Physical Review X

... VO2 shows outstanding performance in the dynamic control of reflection spectra, transmission spectra, and polarization states in surface plasmon metasurfaces [93][94][95][96][97]. Michele Cotrufo et al. [98] incorporated a thin layer of VO2 into the metasurface to dynamically tune its optical properties with temperature changes. ...

Dynamically Switching the Polarization State of Light Based on the Phase Transition of Vanadium Dioxide
  • Citing Article
  • March 2018

Physical Review Applied