Xiaoyong Hu’s research while affiliated with Peking University and other places

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Publications (255)


3D printing technology: Driving pioneering innovations in anti-cancer drug delivery systems
  • Article

March 2025

Jiayi Ma

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Youlong Hai

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Kai Ni

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Xiaoyong Hu

With the rising global incidence of cancer and the limitations of traditional treatment methods, the integration of three-dimensional (3D) printing technology with drug delivery systems offers a promising solution for precision medicine. 3D printing, with its high flexibility and precise production control, allows for the accurate modulation of drug delivery systems, particularly in terms of targeted delivery and controlled drug release rates, thus significantly enhancing therapeutic efficacy and reducing side effects. This review focuses on the applications of various drug delivery forms, such as microneedle patches, implants, and tablets, in the treatment of cancers including breast cancer, melanoma, osteosarcoma, cervical cancer, colorectal cancer, and prostate cancer. Furthermore, the review explores the synergistic effects of combination therapies, such as photothermal therapy, chemotherapy, and immunotherapy, within 3D-printed drug delivery systems, and assesses their potential in addressing tumor recurrence, drug resistance, and treatment-related side effects. Despite the substantial promise of 3D printing technology in cancer treatment, challenges remain in material selection, process optimization, and production standardization. As technology continues to evolve and multidisciplinary collaborations deepen, 3D printing is expected to play an increasingly significant role in the future of precision medicine and personalized cancer therapy.



The non‐Hermitian four‐state system and its Riemann surface in 2D parameter space. a) Schematic diagram of the four‐state system with the detuning (loss) changes in the gray (blue) site. b) Two EPs of the system, and the encircling paths generated by Equation (2,3). c,d) The Real (c) and imaginary (d) parts of the eigenvalues λ of the non‐Hermitian four‐state system as a function of γ and δ.
Dynamics of loop‐1 and loop‐2 that encircle EP‐1 and EP‐2, respectively. a) The cyan (yellow) curve shows the state trajectories of clockwise evolution along loops‐1 on the real part of the Riemann sheets with A (B) as the initial state. b) Same as (a) except that it evolves counter‐clockwise along loops‐1. The inset shows the distribution of the eigenvectors of states A and B. c–f) The absolute amplitude coefficients of the eigenstates during the encircling process along loop‐1 for different initial states and encircling directions (indicated by gray arrows in the inset). g) The cyan (yellow) curve shows state trajectories of clockwise evolution along loops‐2 with C (D) as the initial state on the real part of the Riemann sheets. h) Same as (g) except for evolving counter‐clockwise along loops‐2. The inset shows the distribution of the eigenvectors of states C and D. i–l) Same as (c–f) except for loop‐2.
Dynamics of loop‐3 that encloses both EP‐1 and EP‐2. a) The cyan (yellow) curve shows the state trajectories of clockwise evolution along loops‐3 with A (B) as the initial state on the real part of the Riemann sheets. b) Same as (a) except that it evolves counter‐clockwise along loops‐3. The inset shows the distribution of the eigenvectors of states A and B. c–f) The absolute amplitude coefficients of the eigenstates during the encircling process along loop‐3 for different initial states and encircling directions (indicated by gray arrows in the inset). g) The cyan (yellow) curve shows state trajectories of clockwise evolution along loops‐3 with E (F) as the initial state on the real part of the Riemann sheets. h) Same as (g) except for evolving counter‐clockwise along loops‐3. The inset shows the distribution of the eigenvectors of states E and F. i–l) Same as (c–f) except for initial states are E and F.
a) Section view of the waveguide array, with WG‐2 and WG‐3 possessing loss. b) Top view of the coupled waveguides, with W1 and k2varying continuously along the z‐axis, corresponding to the dynamic encirclement of EP‐2. c) The real and d) imaginary parts of the effective mode index neff of the system. The insets in (c) show the Hz field distribution of four eigenmodes at the starting/end point of the loop. The letters in parentheses indicate the corresponding theoretically calculated eigenstates. e) The loop enclosing EP‐2 is generated by the parametric equations in the numerical simulations.
a,b) |E| and Hz field distribution of photonic chiral mode converters with the initial mode A2 incident on the boundary. The final states are mode A2 for the clockwise loop and mode A1 for the counter‐clockwise loop. c,d) |E| and Hz field distribution of photonic non‐chiral mode converters with the initial mode S1 incident on the boundary. The final state is mode S1 for both clockwise and counter‐clockwise loops.
Dynamically Encircling Multiple Exceptional Points in Waveguides System: Asymmetric–symmetric Multimode Switching
  • Article
  • Full-text available

February 2025

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21 Reads

Dynamically encircling exceptional points in non‐Hermitian systems leads to counterintuitive chiral mode conversions, which provides a new platform for implementing information processing. Previous research has shown that the position of the starting point determines whether the dynamics are chiral or non‐chiral. Photonic devices that simultaneously realize chiral and non‐chiral mode converters are yet to be investigated. In this letter, a four‐state non‐Hermitian waveguide array with two exceptional points is presented and the dynamical encirclement of each exceptional point and double exceptional points, which possess chiral and non‐chiral dynamics is studied. Encircling a single exceptional point and both exceptional points gives the same outcome but a different encircling process. During non‐chiral dynamics, the initial states are not on the Riemann sheet that forms the EPs, encircling both exceptional points produces more branch cuts than encircling a single exceptional point. An asymmetric–symmetric multimode switch at telecommunication wavelengths is demonstrated. Chiral mode converter and non‐chiral mode converter can be implemented simultaneously on one photonic device. The research enriches the exploration of the physics associated with multiple exceptional points in non‐Hermitian multistate systems and inspires wide applications in on‐chip optical systems.

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Proposal of the monolithic hetero-integration of perovskite/Si3N4 on-chip photonic system
a, Schematic of the monolithic hetero-integration of perovskite/Si3N4 on-chip photonic system. The system comprised an efficient and stable LED, a 13-layer (L1–L13) locally connected photonic network with 15 inputs and 2 outputs for photonic computing, and 2 highly sensitive and fast-response photodetectors. NL, nonlinear layer. b,c, Schematic illustrating photonic simulations (b) and computer vision tasks (c) performed using the proposed photonic system.
Characterizations of the monolithic hetero-integrated perovskite/Si3N4 on-chip photonic system
a, Schematic of a perovskite diode working in the LED mode. PeLED, perovskite LED. The inset shows an image of the electrically driven perovskite LED with an area of 1 mm × 2 mm. Ec, conduction band; Ev, valence band; EFn, electron quasi-Fermi level; EFp, hole quasi-Fermi level. b, EQE and radiance versus current density curves of the optimized perovskite LEDs. c, Frequency response of the perovskite LEDs with different bias voltages. d, Schematic of the perovskite diode working in the photodetector mode. PePD, perovskite photodetector. The inset shows the image of the perovskite photodetector with an area of 0.5 mm × 0.5 mm. e, Current–voltage (I–V) curves of the perovskite photodetector under dark and under illuminated light for different light powers. The peak wavelength of the excitation light source is 808 nm, closely matching the electroluminescent peak wavelength of the perovskite. f, TPC characteristics under zero bias of perovskite photodetectors with different device areas. a.u., arbitrary units. g, Schematic of the perovskite LED, photodetector and Si3N4 waveguide on a single chip. The inset shows an image of the monolithically integrated on-chip photonic system. h, I–V curves for different structures. JPD, output current density of the on-chip perovskite photodetector. i, Frequency response of the on-chip devices with different structures.
AMCD calculations in a 2D disordered SSH model
a, Schematic of the 2D disordered SSH model. b,c, Calculated results of the AMCD evolutions for N = 20 (b) and N = 4 (c). d–g, Calculated eigenenergies for both topological (d and f) and trivial (e and g) phases under OBC and PBC. h–k, Calculated topological states. l,m, Large (l) and small (m) network architectures for AMCD calculations. n–q, Training loss and test results for large (n and o) and small (p and q) AMCD networks. r, Experimental results of a small-scale network for AMCD calculations.
Time-dependent photonic simulations in the nonlinear topological model
a, Wave-function distribution at T = 64 with an edge input in the nonlinear SSH model. b, Proportion of wave functions across ten lattice points at the edge with changing input intensities. c, Wave-function distribution with a Gaussian envelope in the middle of the system at T = 64. d, Proportion of wave functions across ten lattice points at the centre with changing input intensities. e, Wave-function evolution transitions from bulk to edge with an increasing input intensity. f, Wave-function evolution with a Gaussian beam input, forming spatial solitons as the input intensity increases. g, Theoretical network architecture for time-dependent nonlinear photonic simulations in the SSH model. h, Training fidelity curve with colour-coded time steps. i, Fidelity distribution across the test dataset. j, Average fidelity across all the 64 time steps for the test dataset.
Edge detection and image classification tasks
a, Schematic of 3 × 3 image patches encoded into complex amplitudes in the training dataset. b, Network architecture for edge detection and trained phase distribution. c,d, Training loss (c) and training accuracy (d) curves for edge detection over four training rounds with different initializations. e, Test confusion matrices of edge detection. f, Experimental results of the confusion matrix for edge detection, based on 100 randomly selected test dataset samples (50 edge cases and 50 non-edge cases). g, Normalized network output distribution, represented as logits for edge/non-edge classification. h, Network designed for CIFAR-10 classification. i, Task for CIFAR-10 classification. j,k, Training loss (j) and training accuracy (k) curves for CIFAR-10 classification over four individual training rounds with different initializations. l, Test confusion matrix of CIFAR-10 from the first training round.
Hetero-integrated perovskite/Si3N4 on-chip photonic system

January 2025

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401 Reads

Nature Photonics

Integrated photonic chips hold substantial potential in optical communications, computing, light detection and ranging, sensing, and imaging, offering exceptional data throughput and low power consumption. A key objective is to build a monolithic on-chip photonic system that integrates light sources, processors and photodetectors on a single chip. However, this remains challenging due to limitations in materials engineering, chip integration techniques and design methods. Perovskites offer simple fabrication, tolerance to lattice mismatch, flexible bandgap tunability and low cost, making them promising for hetero-integration with silicon photonics. Here we propose and experimentally realize a near-infrared monolithic on-chip photonic system based on a perovskite/silicon nitride photonic platform, developing nano-hetero-integration technology to integrate efficient light-emitting diodes, high-performance processors and sensitive photodetectors. Photonic neural networks are implemented to perform photonic simulations and computer vision tasks. Our network efficiently predicts the topological invariant in a two-dimensional disordered Su–Schrieffer–Heeger model and simulates nonlinear topological models with an average fidelity of 87%. In addition, we achieve a test accuracy of over 85% in edge detection and 56% on the CIFAR-10 dataset using a scaled-up architecture. This work addresses the challenge of integrating diverse nanophotonic components on a chip, offering a promising solution for chip-integrated multifunctional photonic information processing.


Tamsulosin ameliorates bone loss by inhibiting the release of Cl − through wedging into an allosteric site of TMEM16A

December 2024

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24 Reads

Proceedings of the National Academy of Sciences

TMEM16A, a key calcium-activated chloride channel, is crucial for many physiological and pathological processes such as cancer, hypertension, and osteoporosis, etc. However, the regulatory mechanism of TMEM16A is poorly understood, limiting the discovery of effective modulators. Here, we unveil an allosteric gating mechanism by presenting a high-resolution cryo-EM structure of TMEM16A in complex with a channel inhibitor that we identified, Tamsulosin, which is resolved at 2.93 Å. Tamsulosin wedges itself into a pocket within the extracellular domain of TMEM16A, surrounded by α1-α2, α5-α6, and α9-α10 loops. This binding stabilizes a transient preopen conformation of TMEM16A, which is activated by Ca ²⁺ ions while still preserving a closed pore to prevent Cl ⁻ permeation. Validation of this binding site through computational, electrophysiological, and functional experiments, along with site-directed mutagenesis, confirmed the pivotal roles of the pocket-lining residues R605 and E624 on α5-α6 loop in modulating Tamsulosin binding and pore activity. Tamsulosin induces significant positional shifts in extracellular loops, particularly the α5-α6 loop, which moves toward the extracellular exit of the pore, leading to noticeable structural rearrangements in pore-lining helices. The hinges induced by P595 in α5 and G711 in α7 introduce flexibility to the transmembrane helices, orienting Y593 to collaborate with I641 in effectively gating the preopening pore. Notably, Tamsulosin demonstrates significant antiosteoporotic effects by inhibiting TMEM16A, suggesting potential for its repurposing in new therapeutic indications. Our study not only enhances our understanding of the gating mechanism of TMEM16A inhibition but also facilitates structure-based drug design targeting TMEM16A.



Anisotropic topological quantum transport on a programmable topological photonic chip. (a) Quantum transport in TIs in the presence of anisotropy, disorder, and topological invariants simultaneously. (b) Schematic of a programmable topological photonic chip. It bases on a FTI with a square lattice with $6 \times 6$ 6 × 6 unit cells of coupled microrings, in total 96 microrings. Inset: zoom-in view of a single unit cell (blue lines are silicon nanophotonic waveguide circuits, and yellow parts are thermo-optical phase shifters). The resonant phase $\varphi$ φ of each microring and the coupling parameter $\theta$ θ between nearest microrings can be arbitrarily controlled. Note that $\theta$ θ is negatively correlated with the coupling strength. The lattice is accessed by 24 input and 24 output optical ports connected to the lattice boundary. Anisotropic topological transport can be experimentally characterized by real-field imaging (top-view imaging with individual cell resolution), and by bandstructure-like measurement (spectral measurement readout at output ports). (c) Horizontal-vertical anisotropic TIs. Phase transition from topological phase to Anderson phase occurs as disorder increases. In between, a quasi-diffusive phase can be observed, where edge modes remain robust in one direction but the distribution becomes diffusive in another. (d) Diagonal-antidiagonal anisotropic TIs. Transport in bulk modes can exhibit unconventionally greater robustness than edge states in lossy, disordered, and anisotropic TIs. (e) Anisotropic TIs with gradient anisotropy that emulates stretched topological TIs in reality. The new transport channels can have greater robustness than old ones along boundaries, and the new transport channels can be reconfigured by controlling the gradient anisotropy. In (c), (d), gray lines indicate anisotropy in the FTI lattice; pink background represents disorders in each unit, where disorders represent random resonant phases $\delta \in$ δ ∈ (0, $2\pi$ 2 π ).
Basic properties of anisotropic topological insulators. (a) Lattice configuration of a horizontal-vertical anisotropic TI. Coupling parameters between nearest microrings in the horizontal ( $x$ x ) and vertical ( $y$ y ) directions are denoted as ${\theta _a}$ θ a and ${\theta _b}$ θ b , respectively. The pink square indicates a three-microring unit cell. (b) Phase diagram. FTI-3 (FTI-2) indicates the presence of three (two) edge states within one free spectral range (FSR). Under TPT, the edge state near $\varepsilon = \pi /{T_R}$ ε = π / T R vanishes into a trivial bandgap. (c) Projected bands in two directions as anisotropy increases (we fix ${\theta _a}$ θ a and tune ${\theta _b}$ θ b ). For edge states, ${\cal W}$ W near $\varepsilon = \pi /{T_R}$ ε = π / T R transitions from one to zero, leading to the disappearance of the corresponding edge state ❸. For bulk bands, they tend to be more compressed and curved (enhanced transport properties) in the $x$ x direction, but flat (localization) in the $y$ y direction. Experimentally imaged real-space distributions of light field for (d) bulk states and (e) edge states. In (e), TPT for the edge state ❸ occurs. In (d), anisotropy transforms initially randomly distributed bulk states in isotropic TIs into directional bulk states in anisotropic TIs that predominantly transport along the $x$ x direction. Green and blue arrows in (a), (d), and (e) indicate the input and output ports. (f) One-dimensional IPR for non-degenerate bulk eigenstates along different directions. Higher IPR signifies greater localization.
Asynchronous Anderson transitions in anisotropic topological insulators. (a) Calculated real-space winding numbers $\overline {{{\cal W}_x}}$ W x ¯ and $\overline {{{\cal W}_y}}$ W y ¯ . The TI is set with configurations of ${\theta _a} = 0.25\pi$ θ a = 0.25 π and ${\theta _b} = 0.5\pi$ θ b = 0.5 π under different levels of uniformly distributed resonant phase disorder $\delta \in$ δ ∈ (0, $2\pi$ 2 π ). $\overline {{{\cal W}_x}}$ W x ¯ and $\overline {{{\cal W}_y}}$ W y ¯ are calculated with quasi-1D geometries ${L_x} = 60,{L_y} = 6$ L x = 60 , L y = 6 and ${L_x} = 6,{L_y} = 60$ L x = 6 , L y = 60 , respectively, where ${L_{x/y}}$ L x / y is the number of unit cells in its corresponding direction. Yellow bars indicate the quasi-diffusive phase, characterized by $\overline {{{\cal W}_x}}$ W x ¯ near one and $\overline {{{\cal W}_y}}$ W y ¯ near zero. Dashed lines denote the disorder values chosen for experiments. (b), (c) Experimental spectra of horizontal and vertical transmission under varying $\delta$ δ . The input and output ports for (b) and (c) are indicated by arrows in the upper left panels of (e) and (f), respectively. Edge states ❶ and ❷ sandwiching degenerate bulk bands in the clean limit within one FSR are highlighted within blue boxes. In each panel in (b) and (c), gray background represents a collection of $N$ N data, colored lines represent their mean, and ${\pm}1\sigma$ ± 1 σ is shown in the top. When $\delta = 0.9\pi$ δ = 0.9 π , the $\sigma$ σ values clearly show that edge states in the $x$ x direction remain robust against disorder, whereas edge states in the $y$ y direction become diffusive. (d) Calculated IPRs. Transition from the ballistic (top 90% diamonds) to the diffusive (bottom 10% diamonds) states occurs at $\delta = 1.16\pi$ δ = 1.16 π and $0.9\pi$ 0.9 π for the edge states in $x$ x and $y$ y directions. An anisotropy-induced $\delta$ δ delay in between two dashed lines indicates the quasi-diffusive state. Shaded area refers to ${\pm}1\sigma$ ± 1 σ and lines refer to mean. (e), (f) Experiment (upper) and simulation (lower) results for field distributions, from robust edge states ( $\delta = 0.2\pi$ δ = 0.2 π ) to quasi-diffusive states ( $\delta = 0.9\pi$ δ = 0.9 π ) and ultimately, to an Anderson insulator ( $\delta = 1.9\pi$ δ = 1.9 π ). Light wavelength in (e), (f) corresponds to the marked circles in spectra in (b), (c). Statistical analysis with $N = 100$ N = 100 are simulated in (a), (d), (e), (f), and statistical measurement with $N = 100$ N = 100 are implemented in (b), (c), (e), (f).
Diagonal-antidiagonal anisotropic topological insulators with superior robust bulk transport. (a) Configuration. Coupling strengths are uniform along the antidiagonal direction and staggered on the diagonal direction. We chose TI with ${\theta _a} = 0.1\pi$ θ a = 0.1 π and ${\theta _b} = 0.6\pi$ θ b = 0.6 π . The pink square indicates a six-microring unit cell. (b) Calculated bulk bandstructures. The right panels display four perspectives: horizontal ( $x$ x ), vertical ( $y$ y ), diagonal ( $d$ d ), and antidiagonal ( $a$ a ). It indicates efficient transport along the antidiagonal direction and poor transport in all other directions for modes in the yellow and blue bulk bands. (c) Transmission spectra at the two antidiagonal ports in (a) and corresponding projected bands in ${k_{x,y}}$ k x , y . The trivial bandgap, edge states, and directional bulk within one FSR are highlighted in red, blue, and green, respectively. (d) Statistical measurements of transmission spectra (experiment and simulation) with disorder. Gray background represents a collection of $N$ N data, colored lines represent their mean, and ${\pm}1\sigma$ ± 1 σ is plotted in the top. Counterintuitively, the bulk states exhibit less variations in transmission compared to the edge states. (e) Numerical analysis of spectral $\sigma$ σ in TIs with different lattice losses. (f), (g) Experimental and simulated real-space field distributions of the edge state and bulk state, in the absence (presence) of disorders. The edge state becomes more diffusive while the bulk state remains almost unchanged. A uniform distribution of phase disorder $\delta = 0.7\pi$ δ = 0.7 π is applied in all plots in (d), (e), (g). Light wavelength in (f), (g) corresponds to the markers in spectra in (c), (d). Statistical analysis or experiments with $N = 100$ N = 100 are conducted in (d)–(g).
Anisotropic topological insulators with gradient anisotropy. (a) Lattice configuration. It emulates a stretched isotropic TI that undergoes stretching in the upper left and lower right corners, inducing gradient coupling strengths along the diagonal direction. Two sets of coupling parameters $({\theta _a},{\theta _b},{\theta _c},{\theta _d},{\theta _e})$ ( θ a , θ b , θ c , θ d , θ e ) are used in experiments: small strain $(0\pi ,0.06\pi ,0.12\pi ,0.18\pi ,0.24\pi)$ ( 0 π , 0.06 π , 0.12 π , 0.18 π , 0.24 π ) and large strain $(0\pi ,0.18\pi ,0.36\pi ,0.54\pi ,0.72\pi)$ ( 0 π , 0.18 π , 0.36 π , 0.54 π , 0.72 π ) . The TPT critical point for isotropic TI is $0.272\pi$ 0.272 π . Therefore, for large strain, domain walls (indicated by yellow lines) separate the FTI-3 region (before TPT) and FTI-2 region (after TPT). Small black arrows denote input and output ports. (b) Experimental and simulated field distributions of different edge states under small and large strain. These edge states near $\varepsilon = 0$ ε = 0 (❶/❷) tend to transport along the lattice boundary, while the edge state near $\varepsilon = \pi /{\rm T}$ ε = π / T (❸) instead transports along the new anisotropic domain wall formed under large strain. (c) Statistical measurements of transmission spectra under small strain (upper) and large strain (lower). Under large strain, only the edge state ❸ exhibits topological protection against disorders. Gray background represents a collection of $N$ N data, colored lines represent their mean, and ${\pm}1\sigma$ ± 1 σ is plotted in the top. A uniform distribution of phase disorder $\delta = 0.5\pi$ δ = 0.5 π is applied in all plots. Statistical analysis and statistical measurement with $N = 100$ N = 100 are implemented in (b), (c).
Anisotropic quantum transport in a programmable photonic topological insulator

November 2024

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61 Reads

Quantum transport in materials describes the behavior of particles at the quantum level. Topological materials exhibit nontrivial transport properties with topological invariants, leading to the emergence of protected states that are immune against disorders at the material boundaries. In many real-world materials, especially those with anisotropic crystal structures, the transport properties can vary significantly along different directions within the material bulk. Here, we experimentally observe counterintuitive quantum transport phenomena in anisotropic topological insulators with controllable anisotropy and disorder, implemented on a programmable topological photonic chip. We examine phase transition from the topological phase to the Anderson phase, between which a new quasi-diffusive phase emerges. Anisotropic topological transport demonstrates unconventional superior robustness in the bulk mode compared to the edge mode, in the presence of disorder and loss in realistic systems. Peculiar topological transport with sophisticated gradient anisotropy, emulating stretched topological materials, occurs at the gradient domain wall that can be reconfigured. Our findings provide fresh insights into the intricate interplay between anisotropy within the bulk and robustness at the boundary of topological materials, which could lead to advancements in the field of topological material science and the development of topological devices with tailored functionalities.


(a) TE (blue curves) and TM (red curves) polarization band structure of PhC; (b) schematic diagram of the proposed defective resonant cavity; (c) structure of the optical convolution kernel based on the PhC.
Conceptual diagram of a PhC photonic convolution kernel. Convolution operations within the CNN model can be realized at the speed of light throughout the system. The data from the input image is encoded in the intensity of each frequency line through electro-optical modulation, which serves as input to the PhC weights bank. The PD receives the output from the PhC weights bank and performs a weighted summation operation. DeMUX, wave-decomposition multiplexer.
Tensor convolution results achieved by PhC kernel-based. The standard test image is convolved with nine different kernels, including classical image processing (blur, motion blur, relief, contour, sharpening), and edge extraction using the lower/upper/left/right Sobel operators.
(a) Process and structure of the CNN model used for predicting the MNIST dataset and the Fashion-MNIST dataset. (b) Loss and accuracy functions for both the training and test sets. (c) Confusion matrix for classifying the dataset using an optical convolution kernel.
Integrated convolutional kernel based on two-dimensional photonic crystals

October 2024

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87 Reads

Optical neural networks (ONNs) exhibit significant potential for accelerating artificial intelligence task processing due to their low latency, high bandwidth, and parallel processing capabilities. Photonic crystals (PhCs) are extensively utilized in integrated optoelectronics because of their unique photonic bandgap properties and precise control of light waves. In this study, we propose an optical reconfigurable convolutional kernel based on PhCs. This kernel can perform convolutional operations on weights by constructing a PhC weight bank. The convolutional kernel demonstrates exceptional performance within the developed optical convolutional neural network framework, successfully realizing various image edge processing tasks. It achieves blind recognition accuracies of 97.81% for the MNIST dataset and 80.31% for the Fashion-MNIST dataset. This study not only demonstrates the feasibility of constructing optical neural networks based on PhCs but to our knowledge, also offers new avenues for the future development of optical computing


Fig. 2 a Schematic diagram of the experimental device. b Schematics of mesh electrodes with different structures. In b, the yellow color indicates the metal electrode, while the grey color denotes the PTFE layer that covers the mesh electrode
Fig. 5 Manipulation of different Moiré lattices with increasing voltage. a PPCs obtained by rotating two striped mesh electrodes. The ratio of Ar to Air in the mixture gas is 2:3, p = 190 Torr, f = 50 kHz, d = 2.0 mm. The lattice constant of the striped metal array a = 10 mm. b PPCs obtained by rotating two square mesh electrodes. The ratio of Ar to Air in the mixture gas is 1:1, p = 152 Torr, f = 50 kHz, d = 2.0 mm. The lattice constant of the square metal array a = 8 mm. c PPCs obtained by rotating two honeycomb mesh electrodes. The ratio of Ar to Air in the mixture gas is 1:1, p = 152 Torr, f = 50 kHz, d = 2.0 mm. The lattice constant of the honeycomb metal array a = 8.66 mm
Fig. 6 Robustness of topological edge states. a-c Snapshots of Line-type, Z-type and Ω-type interface topological PPCs. U = 3.6 kV, 3.6 kV, 3.6 kV, respectively. The ratio of Ar to Air in the mixture gas is 3:2, p = 135 Torr, f = 50 kHz, d = 2.0 mm, the exposure time Δt = 1/10 s. The green and yellow triangles denote the triangular plasma elements of opposite orientations at the interface, the triangle side length is 3.0 mm. d-f Unidirectional propagation of the edge states localized at the interface. The inset in a shows the positions of plasma elements on the mesh electrode
Fig. 7 Photonic band structures and the vortex properties of eigenmodes. a and b Band diagrams of type-A and type-B triangular PPCs. c The frequency variation of K valley during a cycle. d Phase distribution and Poynting vector at K valley for type-A PPCs and type-B PPCs. e The project band structure of supercell. f E z distribution at the wave vector k x = 0.35π∕a and k x = 0.65π∕a , respectively. The electron density of plasma n e = 2.0 × 10 14 cm −3 , v m = 34 GHz
Fig. 8 Triangular PPC and its band structure. a Snapshot of the triangular PPC composed of circular plasma elements (defined as type-C PPC). U = 3.8 kV. The ratio of Ar to Air in the mixture gas is 3:2, p = 135 Torr, f = 50 kHz, d = 2.0 mm, the exposure time Δt = 1/10 s. The diameter of the circular filaments is 1.2 mm. b and c 3D photonic bands of type-A (or B) PPC and type-C PPC, respectively. The average electron density n e = 2.7 × 10 14 cm −3 , v m = 34 GHz. d Experimental transmittance spectra of millimeter waves for type-A (or B) PPC and type-C PPC. e Simulated E z distribution for type-A (or B) PPC and type-C PPC with the frequency of incident microwave f = 34.7 GHz. A normalized colorbar is adopted
Plasma photonic crystal 'kaleidoscope' with flexible control of topology and electromagnetism

October 2024

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81 Reads

Frontiers of Optoelectronics

Continuous development of photonic crystals (PCs) over the last 30 years has carved out many new scientific frontiers. However, creating tunable PCs that enable flexible control of geometric configurations remains a challenge. Here we present a scheme to produce a tunable plasma photonic crystal (PPC) ‘kaleidoscope’ with rich diversity of structural configurations in dielectric barrier discharge. Multi-freedom control of the PPCs, including the symmetry, dielectric constant, crystal orientation, lattice constant, topological state, and structures of scattering elements, has been realized. Four types of lattice reconfigurations are demonstrated, including transitions from periodic to periodic, disordered to ordered, non-topological to topological, and striped to honeycomb Moiré lattices. Furthermore, alterations in photonic band structures corresponding to the reconstruction of various PPCs have been investigated. Our system presents a promising platform for generating a PPC ‘kaleidoscope’, offering benefits such as reduced equipment requirements, low cost, rapid response, and enhanced flexibility. This development opens up new opportunities for both fundamental and applied research. Graphical Abstract



Citations (65)


... All of these factors may substantially impact the detailed energetics of nearly degenerate states in doped materials, particularly when the system is excited or coupled to phonons/magnons [60][61][62][63][64][65], which would require further generalization of the current models. The influence of phonons is expected to enhance the charge modulation via a pure Peierls distortion and thus enhance the CDW. ...

Reference:

Theory of interaction-induced charge order in CrSBr
Ultrafast Electron Dynamics Dominated by Electron–Phonon Coupling in CrSBr Revealed by Photoemission Electron Microscopy
  • Citing Article
  • December 2024

The Journal of Physical Chemistry C

... This independence causes critical interaction-specific features to be overlooked, as the representations of each protein sequence are generated in isolation. Furthermore, this approach becomes increasingly impractical for PPIs that involve complex multi-sequence (2+) interactions, such as those seen in antibody-antigen or TCR-epitope-MHC complexes [17,18]. While concatenating input sequences has been proposed as a workaround, it risks degrading embedding quality by treating all sequences as a single unified entity, potentially masking distinct sequence-specific features [19]. ...

Sliding-attention transformer neural architecture for predicting T cell receptor–antigen–human leucocyte antigen binding

Nature Machine Intelligence

... Light has multiple dimensions, including wavelength, amplitude, phase, mode, and polarization, which are suitable as a multi-dimensional channel for information transmission. Recently, numerous innovative hardware architectures for optical computing have emerged, including coherent architectures based on on-chip Mach-Zehnder interferometer (MZI) grids [9-10], incoherent architectures based on micro-ring resonator (MRR) arrays in wavelength-divisionmultiplexing (WDM) technology [11], and diffractive optical frameworks [12][13][14][15]. Optical computing network architectures require the integration of multiple photonic components. ...

Polarization and wavelength routers based on diffractive neural network

Frontiers of Optoelectronics

... We attribute the deviation between the experiment and the fitting results to fabrication imperfections, because each directional coupler could have slightly different transmission coefficient and the arm path length in each interferometer could be slightly different. The effect of fabrication imperfections, however, can potentially be mitigated by integrating phase shifters to the directional coupler matrix [38]. ...

Ultracompact and multifunctional integrated photonic platform

Science Advances

... EPs catalyze many interesting phenomena, including unconventional transmission or reflection [9][10][11][12] , enhanced sensing [13][14][15] , and unusual quantum criticality [16][17][18][19][20] . It should be emphasized that the quasistatic and dynamical encirclement around EPs exhibits intriguing band braiding [21][22][23][24][25][26] and chiral mode transfer [27][28][29][30][31][32] , respectively, which signify the unique consequences of nontrivial EPs topology and provide broad applications for novel generation of quantum devices [6][7][8] . Besides the unique topology of non-Hermitian systems, EPs also inherit some topological properties of spectral degeneracies in Hermitian systems [4][5][6] . ...

Dynamically Encircling Exceptional Points in Different Riemann Sheets for Orbital Angular Momentum Topological Charge Conversion
  • Citing Article
  • June 2024

Physical Review Letters

... tracking changes in the near-fields or fix broken or distorted wavefronts. A direct feedback could only be provided by scatterers that perturb the field 19,20,34,35 , limiting the applicability of nano-scale wavefront shaping in dynamic processes. ...

Subwavelength imaging using a solid-immersion diffractive optical processor

... With the rapid increase in dataset size and computational cost, computing hardware with high calculation speed is strongly desired for the development of machine learning and artificial intelligence [1][2][3][4][5][6][7]. Several technologies have been proposed for the next-generation computing accelerator, such as quantum computing [8,9], neuromorphic computing [10][11][12][13], and photonic computing [14][15][16][17][18]. Integrated neuromorphic photonic networks have emerged as a promising hardware accelerator for complex matrix-vector multiplication and convolution operation, which are the fundamental operation in artificial neural networks [19][20][21]. ...

A programmable topological photonic chip

Nature Materials

... They are sub-wavelength structures or meta-atoms arranged in two dimensions. Thus, they can manipulate light in more ways than natural materials [33][34][35][36][37][38][39][40][41][42][43][44]. Researchers are striving to advance metasurfaces design to new levels by testing new types of materials, developing new fabrication techniques, and exploring new capabilities [45]. ...

Metasurface on integrated photonic platform: From mode converters to machine learning

... On the basis of constructing the DSmT evidence optimization model, the library intelligent intelligence authenticity recognition model is designed to realize the intelligence authenticity feature detection, and the library intelligent intelligence information entropy feature quantity is extracted through the fuzzy information pseudo-feature analysis method [20]. Using the grid semantic feature decomposition method, the fuzzy subset () yn of library intelligent intelligence information features is obtained, and using load balancing control, the information pseudo-response feature of library intelligent intelligence is obtained as: ...

Information-entropy enabled identifying topological photonic phase in real space

Frontiers of Optoelectronics

... For example, dynamic changes in the TIME are analyzed based on the overall expression levels of specific genes, and prognostic biomarkers have been developed to predict bladder cancer outcomes. 15 However, bulk RNA-seq measures the average gene expression across the entire transcriptome of all cells, which overlooks potential cellular heterogeneity. 16 Single-cell RNA sequencing (scRNA-seq) is a revolutionary genomics technology that enables comprehensive analysis of gene expression profiles at the single-cell level, revealing the roles of different cell subsets and intercellular communication within tumors. ...

Tumor immune dysfunction and exclusion subtypes in bladder cancer and pan-cancer: a novel molecular subtyping strategy and immunotherapeutic prediction model

Journal of Translational Medicine