X. L. Yang’s research while affiliated with Shandong University and other places

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Publications (64)


(Color online) Transmission and phase modulation vs. the short-axis length of the Si-nanoblock at a unit period of 200 nm. The insert shows the constituent basic unit cell of the metasurface.
(Color online) (a) The super cell of Si-nanoblocks for wave front shaping with same geometric parameters except for different short-axis sizes (20, 27, 35, 45, 56, 68, 83 and 125 nm). (b) Phase distribution of the transmission y-polarized light. (c) Phase modulation of the individual nanoblock vs. short-axis length from 20 to 125 nm and incident wavelength over the spectrum range of 600–760 nm. The insert black curve shows the simulated transmittance of the gradient metasurface with incident wavelength from 600 to 760 nm.
(Color online) (a) One pixel of the polarized-multiplexed meta-hologram device with a size of nm². (b) Top-view of the unit cell, with the inserts of long axis l, short axis w and yellow unit dividing dotted line. The simulated field intensity distribution of one pixel under the illumination of (c) x-polarized and (d) y-polarized light, respectively.
(Color online) (a) Illustration of our designed metasurface hologram under two orthogonal polarized illuminations. The phase distribution of the two images “O” and “K” were encoded on the same metasurface and can be reconstructed by the linearly polarized light along the x- or y-direction, respectively. Reconstructed holographic images for (b) x-polarized, (c) y-polarized and (d) -polarizated under 632.8 nm illumination. (e) The transmission efficiency of two diffracted emissions over the bandwidth from 600 nm to 760 nm for two orthogonal polarized positions. Reconstructed holographic images for (f) x-polarized and (g) y-polarized under the 700 nm illumination.
(Color online) (a) Illustration of the experimental set-up of the polarized-selective meta-hologram. The simulated phase patterns of the required images “O” and “K” using FDTD with (b) x-polarized and (c) y-polarized incident light. (d), (e) The corresponding experimentally holographic images by illuminating the phase information in (b) and (c) recorded by SML with the (d) x-polarized and (e) y-polarized incident light, respectively.
Polarization-multiplexed broadband hologram on all-dielectric metasurface
  • Article
  • Publisher preview available

November 2018

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74 Reads

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10 Citations

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P. W. Qiao

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Metasurface is emerging as an important platform to design various functional devices due to the superior capability in controlling amplitude, phase and polarization of light through its ultrathin engineering interface. A polarized-selective hologram of all-dielectric metasurface is proposed to reconstruct multiplexed holographic images on different linear polarization status. Unlike early metasurfaces composed of plasmonic resonators with great ohmic loss at visible spectrum, the designed metasurface made of silicon nanoblocks supports a broader spectral response over the bandwidth from 600 to 760 nm with high diffraction efficiency and low crosstalk between different polarization states. Both simulation and experiment have demonstrated the feasibility and adjustability of the polarization-multiplexed metasurface hologram. We believe it will have significant technological potential in the design of optical functional devices.

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(Colour online) Band structure of the triangular lattice PhC consisting of dielectric rods. The inset shows the Brillouin zone of the triangular lattice and the corresponding high-symmetry point.
(Colour online) (a) 2D triangular lattice PhC square array with cylindrical dielectric rods embedded in the air. The arrows indicate the two directions of and . (b) The transmittance spectra in the direction (indicated by the blue solid lines) and direction (indicated by red dashed lines). The vertical gray dotted line indicates the location of the Dirac-like point. (c) Electric-field distribution at the Dirac-like point of the triangular PhC square array.
(Colour online) (a) Dependence of the Dirac-like point position on the edge length W of the PhC square array with the triangular lattice. Evolution of the transmission spectrum in the direction (indicated by the blue solid lines) and direction (indicated by red dashed lines) of the triangular lattice PhC square arrays with different sizes of (b) , (c) , (d) .
(Colour online) (a) 2D triangular lattice PhC hexagonal array with six identical surfaces (one as the input interface and five as the output interfaces from R1 to R5) composed of cylindrical dielectric rods in air background. (b) The transmittance spectra of R1 (indicated by the red dotted line), R2 (indicated by the black dotted line) and R3 (indicated by the blue solid line) with the vertical gray dotted line indicating the location of the Dirac-like point. (c) The electric-field distribution at the Dirac-like point with the upward incident beam through the PhC hexagonal array.
Effective method to identify and verify the Dirac-like point through finite photonic crystals with triangular lattice

May 2017

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62 Reads

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3 Citations

The precise location of the Dirac-like point of a finite photonic crystal array with a triangular lattice can be identified easily from the transmittance spectrum of any output interface with the characteristic of a sharp cusp embedded in the extremum spectrum near the Dirac-like point. The transmission properties of the finite triangular lattice photonic crystal arrays with square and hexagonal shapes have been investigated systematically to demonstrate that the transmittance at the Dirac-like point has a close relation with the output interface feature of the photonic crystal array and the output interfaces with the same feature will bring about the uniform transmission characteristics in different directions. These results provide us with a more accurate and convenient method to identify the Dirac-like point of a photonic crystal with different lattice structures, array sizes and shapes, and give guidelines for its use in experiments.


Asymetric multiple-image authentication based on complex amplitude information multiplexing and RSA algorithm

June 2015

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180 Reads

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2 Citations

Acta Physica Sinica

By combining the iterative phase retrieval algorithm in the Fresnel domain with the shift rotation permutation operations of row vectors and column vectors, a new kind of asymmetric multiple-image authentication based on complex amplitude information multiplexing and RSA algorithm is proposed, where multiple complex amplitude information in the input plane is retrieved and generated by the phase retrieval algorithm in the Fresnel domain. In original binary amplitude mask, the row vector and column vectors random numbers are randomly generated in advance, such that each sampling mask for each authenticator is obtained by the shift rotation permutation operations of corresponding row vector and column vectors random numbers for original binary amplitude mask. Thus, one synthesized complex amplitude is generated by the operations of sampling, overlap and multiplexing, and then sent to the certification center for authentication use. At the same time, the row vector and column vectors random numbers are encoded to ciphers by the public keys of RSA algorithm, and then delivered to the corresponding authenticators. During the authentication process, the row vector and column vectors random numbers are first decoded by the private keys possessed by the authenticator; second, the authenticator's sampling mask is reconstructed by the shift rotation permutation operations of the above decoded random numbers for original binary amplitude mask. Finally, the authenticator with other additional authentication keys is prompted to place the synthesized complex amplitude information and its sampling mask at the corresponding positions, when the system is illuminated by a plane wave with the correct wavelength. A recovered image is then recorded in the output plane, by calculating and displaying the nonlinear correlation coefficient between the recovered image and the certification image, if there exists a remarkable peak in its nonlinear correlation coefficient distributions, indicating that the authentication is successful. On the contrary, if there is no remarkable peak but uniformly distributed white noise in the map, the authentication process is a failure attempt. Any intruder with randomly generated forged authentication keys will end up with a failure which enhances the security of the system to some extent.


A novel beam splitter based on graded photonic crystals

September 2014

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24 Reads

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1 Citation

This study proposes a novel beam splitter system based on graded photonic crystals, wherein the GPCs are part of a circular PC. A self-collimating PC structure with a square lattice is added to improve transmissivity. The total transmissivity is increased by extending the defect of the self-collimating PC. This study presents a beam splitter system with low energy loss and the best total transmissivity of almost 90%. Furthermore, the relationship between the beam-splitting ratio and the light position is discovered, and the beam-splitting ratio may be changed discretionarily and expediently. Numerical results are obtained using finite-difference time domain and plane wave methods. The proposed structure has significant application potential in optical integration.


Realization of optical coupling based on semi-circular photonic crystals

July 2014

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25 Reads

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3 Citations

Optik

In this paper, a new structure used to realize optical coupling is proposed. This structure is made up of half of a two-dimensional circular photonic crystal and a photonic crystal waveguide. It is shown that the peak value of the transmissivity shifts by choosing appropriate parameters of SCPC. This structure has great potential in optical integration and other areas.


Simultaneous measurement of optical inhomogeneity and thickness variation by using dual-wavelength phase-shifting photorefractive holographic interferometry

March 2014

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38 Reads

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13 Citations

Optics & Laser Technology

A method to measure thickness variation and optical inhomogeneity simultaneously with a dual-wavelength phase-shifting photorefractive holographic interferometer is proposed. This method has no special requirements on the sample surfaces, and additional operations such as coating refractive index matching liquid on surfaces is not needed. With the help of photorefractive holographic interferometry, the wavefront distortion caused by the interferometer system is compensated automatically. Compared with other methods, this method is simpler and more accurate. Computer simulation and optical experiment have verified its feasibility and reliability.


Software realization of optical information hiding system based on phase-shifting interferometry

December 2012

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103 Reads

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1 Citation

Acta Physica Sinica

Combining the techniques of double random phase encoding and phase-shifting interferometry, an information hiding system is proposed, in which the information to be hidden can be encrypted into multiple interferograms. By choosing the appropriate weighting factor, the interferograms can be embedded in the host image. The secrete information can be successfully extracted and decrypted by special phase-shifting reconstruction formula and inverse Fresnel diffraction transform. A software of information hiding system is designed by mixed programming between Visual C++ and Matlab based in the Matcom software environments. By testing the software interface, the designed software can successfully realize the main functions, such as image reading and displaying, input of basis geometrical parameters, information encrypting and embedding, information extracting, decrypting, robustness testing, etc..


(a) Schematic of the 2D triangular PhC with hexagonal dielectric rods in air; (b) Lowest four bands of this PhC for TM polarization. The black line marks the normalized frequency a/λ = 0.32.
EFC plots of (a) TM2 and (b) TM3 bands in the PhC. (c) Wave vector diagram for TM2 and TM3 bands at the frequency of 0.32 with different incident angles of 10°, 20° and 30°.
Ray tracing of the point source at the frequency of 0.32 placed in front of the PhC slab.
The FDTD simulations of electric field distributions with different incident angles of (a) θi = 10°; (b) θi = 20°; (c) θi = 30° at the frequency of 0.32.
Electric field patterns of double focusing imaging for the PhC slab with (a) a/λ = 0.32, f = 82.2%, (b) a/λ = 0.28, f = 82.2%, (c) a/λ = 0.35, f = 59.1%.
Dual-negative refraction in photonic crystals with hexagonal lattices

June 2011

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35 Reads

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15 Citations

We present a dual-negative refraction effect based on the overlapping bands in a two-dimensional triangular photonic crystal formed by holographic lithography. Under certain conditions, one incident plane wave launched into this photonic crystal can be dispersed into two negative refracted waves at the same frequency and the same perpendicular polarization state with different phase velocities and group velocities. We find that this dual-negative refraction behavior can be easily manipulated by adjusting the incident angle, the frequency of incident wave and the filling ratio of the PhC. This special effect can be applied to realize wave-front division and optical interference in optical holography. Based on this effect, a double focusing imaging phenomenon has been achieved by the PhC slab. These unique features may show great impacts on both fundamental physics and optical device applications.


Holographic Fabrication of Photonic Crystals by Double-Beam Exposure Method for Improving the Extraction Efficiency of LED

May 2011

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12 Reads

Light Emitting Diode (LED) has been developing rapidly in recent years because of its various characteristics, such as small size, long life, high brightness, low calorific power and so on. But the poor efficiency of light extraction is the major factor which constrains the development of LED. The two-dimensional (2D) photonic crystals (PhCs) are very suitable for improving the efficiency of light extraction. The PhCs whose size is centimeter level can be fabricated by holographic lithography. It is low cost and easier for the industrialization of production. To research the condition of making 2D PhCs for improving the efficiency of light extraction, we use 532nm laser as the light source and SU-8 negative photoresist as the mask. The 2D PhCs whose duty cycle is 1:1 are created by double-beam double exposure method. It is verified that the PhCs can be used to improve the efficiency of light extraction.


Anomalous refractive effects in honeycomb lattice photonic crystals formed by holographic lithography

July 2010

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20 Reads

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23 Citations

We have investigated for the first time the anomalous refractive effects of a photonic crystal (PhC) formed by holographic lithography (HL) with triangular rods arranged in a honeycomb lattice in air. Possibilities of left-handed negative refraction and superlens are discussed for the case of TM2 band with the index contrast n = 3.4:1. In contrast to the conventional honeycomb PhC made of regular rods in air, the HL PhCs show left-handed negative refraction over a wider and higher frequency range with high transmissivity (>90%), and the effective indices quite close to −1 for a wide range of incident angles with a larger all-angle left-handed negative refraction (AALNR) frequency range (Δω/ω ≈14.8%). Calculations and FDTD simulations demonstrate the high-performance negative refraction properties can happen in the holographic structures for a wide filling ratio and can be modulated by changing the filling ratio easily.


Citations (52)


... To meet the growing demands for enhanced data transmission rates and capacities, multifunctional metasurfaces have been proposed, integrating multiple functionalities into a single metasurface. This integration can be achieved through various multiplexing strategies, such as polarization multiplexing, [22][23][24][25][26] where designed metaatoms produce distinct amplitude-phase responses for different polarization states of electromagnetic waves. By elaborately arranging these meta-atoms within the metasurfaces, various functionalities can be realized for different polarization states. ...

Reference:

Chirality‐Assisted Spin‐Decoupled Metasurface Implemented by Simple Geometrical Rotation
Polarization-multiplexed broadband hologram on all-dielectric metasurface

... Using computer control, the "printed materials" are layered on top of each other until the physical object replicates the design on the computer. Common materials used for 3D printing include tough nylon, gypsum, aluminum, textiles, and polylactic acid [37,38]. The future of 3D printing appears to involve creating more lifelike models using a variety of materials [39]. ...

Novel oral fast-disintegrating drug delivery devices with predefined inner structure fabricated by Three-Dimensional Printing
  • Citing Article
  • March 2009

Journal of Pharmacy and Pharmacology

... There have been extensive studies on the propagation effects of structured light beams using various scalar diffraction theories, which can be divided into four categories: the Fresnel diffraction integral [14][15][16][17], the Collins formula [18][19][20][21][22][23][24], the angular spectrum representation [25][26][27][28][29][30], and the Rayleigh-Sommerfeld diffraction integral [31][32][33][34][35][36][37][38][39][40]. The Fresnel diffraction integral, which is an approximation of the Kirchhoff diffraction formula, is usually used to study the propagation of paraxial light beams in a homogeneous medium. ...

Collins formulae in both space and frequency domains for ABCD optical systems with small deformations
  • Citing Article
  • July 2001

Journal of Modern Optics

... At this point we would like to emphasize that the aim of this article is to provide a detailed overview over the experiments which where performed in our group with normal and superconducting microwave photonic crystals until the laboratory was closed in 2015. Since then there has been a tremendous development regarding experimental studies of various aspects related to the hexagonal structure of graphene like, e.g. with dielectric photonic crystals [15,36,[97][98][99][100]. Such systems have the great advantage with respect to superconducting microwave photonic crystals that their shape can be varied, e.g. in order to introduce strain [31], realize disordered graphene [97] and hexagonal lattices formed by two different types of atoms [101], or to perform experiments on quantum search [102]. ...

Effective method to identify and verify the Dirac-like point through finite photonic crystals with triangular lattice

... 70 Implantable dosage forms for sustained release, cyclic release, multiphase release, pulse release, CR of multiple drugs in a single DDD have been reported in literature. 9,15,71,72 Traditionally, the most common method for manufacturing implants is to blend the drug with the excipients and then use a compression or injection molding technique to fabricate the devices, which may have some disadvantages in the optimal control of the structure and internal architecture of DDD. 73,74 The strategies and methods offered by 3DP for conceiving and manufacturing implantable DDD are the same as those for developing ODFs. ...

Design and fabrication of drug delivery devices with complex architectures based on three-dimensional printing technique
  • Citing Article
  • December 2005

... Since the tablet's height remained relatively constant over time, the drug release rate also remained relatively stable. Moreover, Yu et al. [68] used binder jet 3D printing to create an API gradient oral controlled-release drug delivery system and dissolved diclofenac sodium in the binder. The top and bottom layers were intended for release inhibition in the axial direction, while the middle layer powder was a mixture of lactose, HPMC, and PVP. ...

Studies on preparation of controlled-release delivery systems with drug gradients using three dimensional printing technique
  • Citing Article
  • July 2006

... When using the visual acquisition model to analyze the physical features of moving objects [14], an extraction algorithm is needed. Combining the conversion, quantization, and modification of the prediction difference, it can achieve feature analysis, determine the error point of the serve action, and take the feature partition model [15]. ...

Asymetric multiple-image authentication based on complex amplitude information multiplexing and RSA algorithm

Acta Physica Sinica

... Figure 4 indicates the relations of relative band gap Δω/ω with maximum peak value to filling ratio f for different dielectric contrasts. Computations show that the peak value of optimum relative PBG not always augments with the increase of dielectric constant ε for normal structure, instead, the peak value reaches the maximum at about ε = 8.9, such as 9.9% with f = 15.9% for ε = 8.9 and c = 1.2, which is larger than the result (8.8%) of best designed pincushion columns with the same dielectric constant [27]. Specially, in this kind of normal structures, the required minimum permittivity to open a complete photonic band gap with Δω/ω > 1% is near 3.8, which is much lower than the value of 6.4 in the case of pincushion columns [27] and lower than all the results of 2D photonic crystals ever reported before. ...

Holographic design of a two-dimensional photonic crystal of square lattice with pincushion columns and large complete band gaps

... Most schemes employ diffraction for the spectral discrimination, which inevitably brings a trade-off between size and resolution. Integrated spectrometer implementations [10][11][12][13][14][15] are mostly based on arrays of filter elements, which limit the resolution, and rely on external detectors, resulting in a much increased packaging complexity and cost. In principle, the combination of a tuneable optical cavity and a photodetector can lead to an extremely compact spectrometer, particularly if the detector is integrated inside the cavity 16,17 . ...

Realization of optical coupling based on semi-circular photonic crystals
  • Citing Article
  • July 2014

Optik

... gr. reflectometry (Lu et al. 2014), ellipsometry (McCrackin et al. 1963), or light attenuation (Flournoy et al. 1972;Utaka et al. 2013;Zhang et al. , 2009Liu et al. 2019;Nogueira et al. 2005;Li et al. 2006Li et al. , 2014Borgetto et al. 2010;Kavehpour et al. 2002). In Table 1 (see supplementary material) a summary of the main of them is displayed, highlighting their measurement range, and some interesting characteristics of the employed method. ...

Simultaneous measurement of optical inhomogeneity and thickness variation by using dual-wavelength phase-shifting photorefractive holographic interferometry
  • Citing Article
  • March 2014

Optics & Laser Technology