Jin Zhang’s scientific contributions

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Publications (2)


Schematic diagram of PC design based on a deep learning model. Forward calculation allows us to obtain the band structures of PCs for given parameters d 1 and d 2 using the PWE method. For the inverse design process, a machine learning model is trained to predict the geometric parameters d 1 and d 2 when a PC with a specific band structure is aimed.
(a) The DL model constructed by a fully connected multilayer neural network with an input layer, an output layer, and five hidden layers. The number of neurons for each layer is labeled. The output layer corresponds to the structure parameters d 1 and d 2. (b) The band spectra in the ΓM direction, in which the whole frequency span is divided into 501 parts, and the passband and stopband are remarked as 1 and 0, respectively. (c) Loss function vs the number of iterations trained by 11 336 samples labeled as a, by 1974 samples labeled as b, and by 5037 samples labeled as c.
(a) Band structures of a PC. Red dots are the results predicted by the DL model. Blue lines correspond to the original results. (b) Targeted bandgap labeled in lines and a predicted bandgap marked by dots from the model. (c) Similar to (a) but band structures only in the XM direction are considered. (d) When partial bandgaps along the XM marked by blue are aimed, the DL model can predict the structure parameter of a PC with partial bandgaps marked by red dots.
(a) The global machine learning (ML) model predicts the possibility of the existence of the Dirac cone highlighted by a box around Γ for d 1 = 2.54 mm and d 2 = 2.96 mm. (b) Zoomed view of the boxed area in (a). By a re-learning process, the local property of bands around this region can be precisely predicted. The re-learning frequency window is chosen to be [ f 3, f 4] = [31.625, 30.604] kHz. After a re-training process, a local ML model is established. This leads to a perfect Dirac cone shown in blue lines in (c) with d 1 = 2.45 mm and d 2 = 2.97 mm. The red dots are the results from simulation. (d) The two eigenmodes of the Dirac point. The color level indicates the amplitude of sound pressure.
(a) Double Dirac cone predicted by the local ML model with d 1 = 5.26 mm and d 2 = 3.04 mm. Blue lines are the predicted results, and red dots are the simulation. (b) The four eigenmodes at the Dirac point. The color level indicates the amplitude of sound pressure.
Deep learning for Dirac dispersion engineering in sonic crystals
  • Article
  • Full-text available

June 2024

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122 Reads

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1 Citation

Xiao-Huan Wan

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Jin Zhang

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Band structure and Dirac degeneracy are essential features of sonic crystals/acoustic metamaterials to achieve advanced control of exciting wave effects. In this work, we explore a deep learning approach for the design of phononic crystals with desired dispersion. A plane wave expansion method is utilized to establish the dataset relation between the structural parameters and the energy band features. Subsequently, a multilayer perceptron model trained using the dataset can yield accurate predictions of wave behavior. Based on the trained model, we further impose a re-learning process around a targeted frequency, by which Dirac degeneracy and double Dirac degeneracy can be embedded into the band structures. Our study enables the deep learning approach as a reliable design strategy for Dirac structures/metamaterials, opening up the possibilities for intriguing wave physics associated with Dirac cone.

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FIG. 1. Schematic presentation of the zigzag granular chain and its band structures. (a) A unit cell marked by a green dashed box contains two sublattice beads A and B. Each bead has two rotational DOFs along the x and y axes, respectively, and one translational DOF along the z axis. The interactions between beads are characterized by effective springs with shear K s , bending K b , and torsional K t rigidities. (b) and (c) show the bulk band structures with dashed lines representing H e modes and solid lines corresponding to H o modes. (b) ξ b = K b /K s = 0.1 and ξ t = K t /K s = 0.328. The latent symmetry induced linear degeneracies appear at ±q D . (c) For ξ b = 0.1 and ξ t = 0.2, the degeneracy is gapped.
FIG. 2. Graphical representations for H j , R S j , and H j . The colored circles represent different pure modes in the corresponding eigenmode space. Arrowed lines stand for the couplings between modes, and loops starting and ending at the same circles mark the on-site potentials. (a) Graph of H j . (b) σ x chiral is visualized and a mirror placed vertically in between the two circles is possible when δ j = ρ j = 0. (c) The lines of δ o = 0 and ρ o = 0 cross each other at ±q D where the degeneracies appear (gray lines). (d) A mirror passing vertically through the green circle exists when Im(L j ) = 0. This requires ϕ j − ϕ = 0. (e) The curves of ϕ o and ϕ for q ∈ [−π, π] intersect at ±q D . case, under the basis U j = Y j U j (see the form of Y j in the SM), the new Hamiltonian reads
FIG. 3. Eigenfrequency calculations of a ZGC consisting of 200 beads with free boundaries. (a) The setting ξ b = 0.1, ξ t = 0.2 corresponds to the topological phase. Red/blue dots label the bulk/edge modes. Cyan area is the band gap. Bulk band structure is also presented by gray dashed lines. (b) The setting ξ b = 0.1, ξ t = 0.5 belongs to the trivial phase. No edge states are observed inside the band gap. (c) The winding of R S j . Red/blue lines correspond to the occupied S e /S o bands. The color level from light to dark indicates the value of q varying from [−π, π]. (d) and (e) show the profiles of the eigenmodes of the edge states in (a).
FIG. 4. Robustness verifications of topological edge states under different disorder settings. (a) Distribution of eigenfrequency for random mass in [(1 − γ M )M, (1 + γ M )M] over 200 ZGC configurations for each γ M . Gray/red dots mark the positions of bulk/edge states. (b) Same as (a) but with identical mass in the chain while the angles of every two beads are randomly distributed in [(1 − γ θ )π/6, (1 + γ θ )π/6].
Robust topological edge states induced by latent mirror symmetry

December 2023

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134 Reads

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5 Citations

In recent years, topology has offered an elegant degree of freedom (DOF) for light and sound manipulation. There exists persistent effort to explore the origin of topological phases based on symmetry, while it becomes rather challenging in complex networks or multiple DOF systems where geometric symmetries are not apparent. Here, we demonstrate a linear degeneracy induced by latent mirror symmetry in a zigzag granular chain whose DOF is three times larger than its bead number. An isospectral reduction approach and graphical representation are developed to track the topological origin of the degeneracy. We show how the latent mirror symmetry leads to the degeneracy and how it is manifested in a properly chosen eigenmode space. Moreover, we reveal the existence of topological edge states and their robustness against different disorders when the degeneracy is gapped. Our study takes a pivotal step toward exploiting topological waves in complex networks or disordered systems, opening up the perspective of offering new flexibilities for classical wave tailoring.

Citations (2)


... On the other hand, combining several different unit cells into a supercell leads to changes in the lattice constant of the structure, thereby affecting the Bragg bandgap and widening its tunable range. 18,19 Despite significant advances in bandgap calculation methods such as the finite element method, 20 the plane wave expansion method, 5,18,21,22 and the transfer matrix method, [23][24][25][26][27] incorporating a supercell structure complicates the analysis. Additionally, in engineering practice, frequencies typically vary in real time. ...

Reference:

Programmable piezoelectric phononic crystal beams with shunt circuits: A deep learning neural network-assisted design strategy for real-time tunable bandgaps
Deep learning for Dirac dispersion engineering in sonic crystals

... This method has been used to create stability preserving transformations of networks [37,38], and study the survival probabilities in open dynamical systems [39]. Recent studies of topological states show that IR of the system's Hamiltonian can be used to unearth the hidden symmetry, giving rise to exotic band degeneracy [40][41][42] and robust topological edge states [43,44]. ...

Robust topological edge states induced by latent mirror symmetry