Demo Data from EDBT 2026 / reviewers in the wild / expert
Hongsheng Liu 0002
dblp:59/9103-2
· DBLP profile ↗
8ranked-venue papers
0as first author
8since 2021 · last 2025
0000-0003-0509-7967ORCID · conflict
Domains — the database's venue-derived domains; a paper can count in several
Artificial intelligence and machine learning · 8 · 8 since 2021Databases, data management, data science and information retrieval · 3 · 3 since 2021Graphics, computer vision, multimedia, augmented reality and games · 1 · 1 since 2021
Expertise — from the expertise taxonomy: the topics of the expert's papers under the CCF categories. A weight counts papers with recency: 1 for a paper about the topic, 0.3 when the topic is its context, halved every five years.
| Interdisciplinary, comprehensive, and emerging computing
7 papers |
Computational science and engineering · 100% | |
| Artificial intelligence
4 papers |
Graph learning · 34% 3D vision · 21% Time series and sequential data · 21% |
Topics — the 15 heaviest of 17, each with the papers that count most for it
| Topic | Weight | Papers | Last | Evidence papers |
|---|---|---|---|---|
Computational science and engineering
scientific machine learning |
2.2 | 3 | 2025 | PhyMPGN: Physics-encoded Message Passing Graph Network for spatiotemporal PDE systems · ICLR 2025 P2C2Net: PDE-Preserved Coarse Correction Network for efficient prediction of spatiotemporal dynamics · NeurIPS 2024 Meta-Auto-Decoder for Solving Parametric Partial Differential Equations · NeurIPS 2022 |
Computational science and engineering
computational fluid dynamics |
1.7 | 2 | 2025 | Learnable-Differentiable Finite Volume Solver for Accelerated Simulation of Flows · KDD (2) 2025 MultiPDENet: PDE-embedded Learning with Multi-time-stepping for Accelerated Flow Simulation · ICML 2025 |
Computational science and engineering › scientific machine learning
physics-informed machine learning |
1.6 | 2 | 2025 | MultiPDENet: PDE-embedded Learning with Multi-time-stepping for Accelerated Flow Simulation · ICML 2025 P2C2Net: PDE-Preserved Coarse Correction Network for efficient prediction of spatiotemporal dynamics · NeurIPS 2024 |
Computational science and engineering › partial differential equation solver
neural PDE solver |
1.3 | 2 | 2024 | P2C2Net: PDE-Preserved Coarse Correction Network for efficient prediction of spatiotemporal dynamics · NeurIPS 2024 Meta-Auto-Decoder for Solving Parametric Partial Differential Equations · NeurIPS 2022 |
Computational science and engineering › scientific machine learning › physics-informed machine learning › physics-informed neural networks
partial differential equation solving |
1.3 | 2 | 2024 | P2C2Net: PDE-Preserved Coarse Correction Network for efficient prediction of spatiotemporal dynamics · NeurIPS 2024 A Universal PINNs Method for Solving Partial Differential Equations with a Point Source · IJCAI 2022 |
Computational science and engineering › scientific machine learning › physics-informed machine learning
physics-informed neural networks |
1.1 | 2 | 2022 | Meta-Auto-Decoder for Solving Parametric Partial Differential Equations · NeurIPS 2022 A Universal PINNs Method for Solving Partial Differential Equations with a Point Source · IJCAI 2022 |
Computer vision › 3D vision
object-centric reasoning |
0.9 | 1 | 2025 | SlotPi: Physics-informed Object-centric Reasoning Models · KDD (2) 2025 |
Machine learning › Graph learning › graph neural network › graph neural network architecture
physics-informed graph neural networks |
0.9 | 1 | 2025 | PhyMPGN: Physics-encoded Message Passing Graph Network for spatiotemporal PDE systems · ICLR 2025 |
Machine learning › Time series and sequential data
spatiotemporal forecasting |
0.9 | 1 | 2025 | SlotPi: Physics-informed Object-centric Reasoning Models · KDD (2) 2025 |
Computational science and engineering › partial differential equations
partial differential equation simulation |
0.9 | 1 | 2025 | MultiPDENet: PDE-embedded Learning with Multi-time-stepping for Accelerated Flow Simulation · ICML 2025 |
Computational science and engineering › partial differential equations
parametric PDEs |
0.6 | 1 | 2022 | Meta-Auto-Decoder for Solving Parametric Partial Differential Equations · NeurIPS 2022 |
Machine learning › Graph learning
graph neural network |
0.5 | 2 | 2025 | Conservation-informed Graph Learning for Spatiotemporal Dynamics Prediction · KDD (1) 2025 PhyMPGN: Physics-encoded Message Passing Graph Network for spatiotemporal PDE systems · ICLR 2025 |
Machine learning › Trustworthy machine learning
interpretability |
0.3 | 1 | 2025 | Conservation-informed Graph Learning for Spatiotemporal Dynamics Prediction · KDD (1) 2025 |
Machine learning › Deep learning architectures and training
physics-informed neural network |
0.3 | 1 | 2025 | Conservation-informed Graph Learning for Spatiotemporal Dynamics Prediction · KDD (1) 2025 |
Computer vision › Vision and language
visual question answering |
0.3 | 1 | 2025 | SlotPi: Physics-informed Object-centric Reasoning Models · KDD (2) 2025 |
Methods — techniques the papers use, named apart from their topics
graph neural network · 3.5symmetry · 1.7numerical integrator · 1.7multi-scale modeling · 1.7laplace-beltrami operator · 1.7slot attention · 0.9runge-kutta integration · 0.9object-centric model · 0.9multiscale time stepping · 0.9hamiltonian principles · 0.9finite volume method · 0.9finite difference · 0.9differentiable solver · 0.9high-order numerical scheme · 0.8coarse correction · 0.8
| Year | Publication | Venue | Position |
|---|---|---|---|
| 2025 | PhyMPGN: Physics-encoded Message Passing Graph Network for spatiotemporal PDE systemsabstractSolving partial differential equations (PDEs) serves as a cornerstone for modeling complex dynamical systems. Recent progresses have demonstrated grand benefits of data-driven neural-based models for predicting spatiotemporal dynamics (e.g., tremendous speedup gain compared with classical numerical methods). However, most existing neural models rely on rich training data, have limited extrapolation and generalization abilities, and suffer to produce precise or reliable physical prediction under intricate conditions (e.g., irregular mesh or geometry, complex boundary conditions, diverse PDE parameters, etc.). To this end, we propose a new graph learning approach, namely, Physics-encoded Message Passing Graph Network (PhyMPGN), to model spatiotemporal PDE systems on irregular meshes given small training datasets. Specifically, we incorporate a GNN into a numerical integrator to approximate the temporal marching of spatiotemporal dynamics for a given PDE system. Considering that many physical phenomena are governed by diffusion processes, we further design a learnable Laplace block, which encodes the discrete Laplace-Beltrami operator, to aid and guide the GNN learning in a physically feasible solution space. A boundary condition padding strategy is also designed to improve the model convergence and accuracy. Extensive experiments demonstrate that PhyMPGN is capable of accurately predicting various types of spatiotemporal dynamics on coarse unstructured meshes, consistently achieves the state-of-the-art results, and outperforms other baselines with considerable gains. Bocheng Zeng, Qi Wang 0123, Mengtao Yan, Ruizhi Chengze, Yi Zhang 0164, Hongsheng Liu 0002, Zidong Wang 0010, Hao Sun 0002 |
ICLR | 7 |
| 2025 | MultiPDENet: PDE-embedded Learning with Multi-time-stepping for Accelerated Flow SimulationabstractSolving partial differential equations (PDEs) by numerical methods meet computational cost challenge for getting the accurate solution since fine grids and small time steps are required. Machine learning can accelerate this process, but struggle with weak generalizability, interpretability, and data dependency, as well as suffer in long-term prediction. To this end, we propose a PDE-embedded network with multiscale time stepping (MultiPDENet), which fuses the scheme of numerical methods and machine learning, for accelerated simulation of flows. In particular, we design a convolutional filter based on the structure of finite difference stencils with a small number of parameters to optimize, which estimates the equivalent form of spatial derivative on a coarse grid to minimize the equation's residual. A Physics Block with a 4th-order Runge-Kutta integrator at the fine time scale is established that embeds the structure of PDEs to guide the prediction. To alleviate the curse of temporal error accumulation in long-term prediction, we introduce a multiscale time integration approach, where a neural network is used to correct the prediction error at a coarse time scale. Experiments across various PDE systems, including the Navier-Stokes equations, demonstrate that MultiPDENet can accurately predict long-term spatiotemporal dynamics, even given small and incomplete training data, e.g., spatiotemporally down-sampled datasets. MultiPDENet achieves the state-of-the-art performance compared with other neural baseline models, also with clear speedup compared to classical numerical methods Qi Wang 0123, Yuan Mi, Haoyun Wang, Yi Zhang 0164, Ruizhi Chengze, Hongsheng Liu 0002, Ji-Rong Wen, Hao Sun 0002 |
ICML | 6 |
| 2025 | SlotPi: Physics-informed Object-centric Reasoning ModelsabstractUnderstanding and reasoning about dynamics governed by physical laws through visual observation, akin to human capabilities in the real world, poses significant challenges. Currently, object-centric dynamic simulation methods, which emulate human behavior, have achieved notable progress but overlook two critical aspects: 1) the integration of physical knowledge into models. Humans gain physical insights by observing the world and apply this knowledge to accurately reason about various dynamic scenarios; 2) the validation of model adaptability across diverse scenarios. Real-world dynamics, especially those involving fluids and objects, demand models that not only capture object interactions but also simulate fluid flow characteristics. To address these gaps, we introduce SlotPi, a slot-based physics-informed object-centric reasoning model. SlotPi integrates a physical module based on Hamiltonian principles with a spatio-temporal prediction module for dynamic forecasting. Our experiments highlight the model's strengths in tasks such as prediction and Visual Question Answering (VQA) on benchmark and fluid datasets. Furthermore, we have created a real-world dataset encompassing object interactions, fluid dynamics, and fluid-object interactions, on which we validated our model's capabilities. The model's robust performance across all datasets underscores its strong adaptability, laying a foundation for developing more advanced world models. Jian Li 0064, Han Wan, Ning Lin, Yuliang Zhan, Ruizhi Chengze, Yi Zhang 0164, Hongsheng Liu 0002, Zidong Wang 0010, Fan Yu 0004, Hao Sun 0002 |
KDD (2) | 8 |
| 2025 | Conservation-informed Graph Learning for Spatiotemporal Dynamics PredictionabstractData-centric methods have shown great potential in understanding and predicting spatiotemporal dynamics, enabling better design and control of the object system. However, deep learning models often lack interpretability, fail to obey intrinsic physics, and struggle to cope with the various domains. While geometry-based methods, e.g., graph neural networks (GNNs), have been proposed to further tackle these challenges, they still need to find the implicit physical laws from large datasets and rely excessively on rich labeled data. In this paper, we herein introduce the conservation-informed GNN (CiGNN), an end-to-end explainable learning framework, to learn spatiotemporal dynamics based on limited training data. The network is designed to conform to the general conservation law via symmetry, where conservative and non-conservative information passes over a multiscale space enhanced by a latent temporal marching strategy. The efficacy of our model has been verified in various spatiotemporal systems based on synthetic and real-world datasets, showing superiority over baseline models. Results demonstrate that CiGNN exhibits remarkable accuracy and generalizability, and is readily applicable to learning for prediction of various spatiotemporal dynamics in a spatial domain with complex geometry. Yuan Mi, Pu Ren, Hongteng Xu, Hongsheng Liu 0002, Zidong Wang 0010, Yike Guo, Ji-Rong Wen, Hao Sun 0002, Yang Liu 0005 |
KDD (1) | 4 |
| 2025 | Learnable-Differentiable Finite Volume Solver for Accelerated Simulation of FlowsabstractSimulation of fluid flows is crucial for modeling physical phenomena like meteorology, aerodynamics, and biomedicine. Classical numerical solvers often require fine spatiotemporal grids to satisfy stability, consistency, and convergence conditions, leading to substantial computational costs. Although machine learning has demonstrated better efficiency, they typically suffer from issues of interpretability, generalizability, and data dependency. Hence, we propose a learnable and differentiable finite volume solver, called LDSolver, designed for efficient and accurate simulation of fluid flows on spatiotemporal coarse grids. LDSolver comprises two key components: (1) a differentiable finite volume solver, and (2) an learnable module providing equivalent approximation for fluxes (derivatives and interpolations), and temporal error correction on coarse grids. Even with limited training data (e.g., only a few trajectories), our model could accelerate the simulation while maintaining a high accuracy with superior generalizability. Experiments on different flow systems (e.g., Burgers, decaying, forced and shear flows) show that LDSolver achieves state-of-the-art performance, surpassing baseline models with notable margins. Mengtao Yan, Qi Wang 0123, Ruizhi Chengze, Yi Zhang 0164, Hongsheng Liu 0002, Zidong Wang 0010, Fan Yu 0004, Qi Qi 0003, Hao Sun 0002 |
KDD (2) | 6 |
| 2024 | P2C2Net: PDE-Preserved Coarse Correction Network for efficient prediction of spatiotemporal dynamicsabstractWhen solving partial differential equations (PDEs), classical numerical methods often require fine mesh grids and small time stepping to meet stability, consistency, and convergence conditions, leading to high computational cost. Recently, machine learning has been increasingly utilized to solve PDE problems, but they often encounter challenges related to interpretability, generalizability, and strong dependency on rich labeled data. Hence, we introduce a new PDE-Preserved Coarse Correction Network (P$^2$C$^2$Net) to efficiently solve spatiotemporal PDE problems on coarse mesh grids in small data regimes. The model consists of two synergistic modules: (1) a trainable PDE block that learns to update the coarse solution (i.e., the system state), based on a high-order numerical scheme with boundary condition encoding, and (2) a neural network block that consistently corrects the solution on the fly. In particular, we propose a learnable symmetric Conv filter, with weights shared over the entire model, to accurately estimate the spatial derivatives of PDE based on the neural-corrected system state. The resulting physics-encoded model is capable of handling limited training data (e.g., 3--5 trajectories) and accelerates the prediction of PDE solutions on coarse spatiotemporal grids while maintaining a high accuracy. P$^2$C$^2$Net achieves consistent state-of-the-art performance with over 50\% gain (e.g., in terms of relative prediction error) across four datasets covering complex reaction-diffusion processes and turbulent flows. Qi Wang 0123, Pu Ren, Xin-Yang Liu, Yi Zhang 0164, Zeruizhi Cheng, Hongsheng Liu 0002, Zidong Wang 0010, Jian-Xun Wang 0001, Ji-Rong Wen, Hao Sun 0002, Yang Liu 0130 |
NeurIPS | 8 |
| 2022 | A Universal PINNs Method for Solving Partial Differential Equations with a Point SourceabstractIn recent years, deep learning technology has been used to solve partial differential equations (PDEs), among which the physics-informed neural networks (PINNs)method emerges to be a promising method for solving both forward and inverse PDE problems. PDEs with a point source that is expressed as a Dirac delta function in the governing equations are mathematical models of many physical processes. However, they cannot be solved directly by conventional PINNs method due to the singularity brought by the Dirac delta function. In this paper, we propose a universal solution to tackle this problem by proposing three novel techniques. Firstly the Dirac delta function is modeled as a continuous probability density function to eliminate the singularity at the point source; secondly a lower bound constrained uncertainty weighting algorithm is proposed to balance the physics-informed loss terms of point source area and the remaining areas; and thirdly a multi-scale deep neural network with periodic activation function is used to improve the accuracy and convergence speed. We evaluate the proposed method with three representative PDEs, and the experimental results show that our method outperforms existing deep learning based methods with respect to the accuracy, the efficiency and the versatility. Hongsheng Liu 0002, Beiji Shi, Zidong Wang 0010, Yang Li 0106, Min Wang 0037, Haotian Chu, Fan Yu 0004, Bei Hua, Bin Dong 0001, Lei Chen 0002 |
IJCAI | 2 |
| 2022 | Meta-Auto-Decoder for Solving Parametric Partial Differential EquationsabstractMany important problems in science and engineering require solving the so-called parametric partial differential equations (PDEs), i.e., PDEs with different physical parameters, boundary conditions, shapes of computation domains, etc. Recently, building learning-based numerical solvers for parametric PDEs has become an emerging new field. One category of methods such as the Deep Galerkin Method (DGM) and Physics-Informed Neural Networks (PINNs) aim to approximate the solution of the PDEs. They are typically unsupervised and mesh-free, but require going through the time-consuming network training process from scratch for each set of parameters of the PDE. Another category of methods such as Fourier Neural Operator (FNO) and Deep Operator Network (DeepONet) try to approximate the solution mapping directly. Being fast with only one forward inference for each PDE parameter without retraining, they often require a large corpus of paired input-output observations drawn from numerical simulations, and most of them need a predefined mesh as well. In this paper, we propose Meta-Auto-Decoder (MAD), a mesh-free and unsupervised deep learning method that enables the pre-trained model to be quickly adapted to equation instances by implicitly encoding (possibly heterogenous) PDE parameters as latent vectors. The proposed method MAD can be interpreted by manifold learning in infinite-dimensional spaces, granting it a geometric insight. Extensive numerical experiments show that the MAD method exhibits faster convergence speed without losing accuracy than other deep learning-based methods. Zhanhong Ye, Hongsheng Liu 0002, Beiji Shi, Zidong Wang 0010, Yang Li 0106, Min Wang 0037, Haotian Chu, Fan Yu 0004, Bei Hua, Lei Chen 0002, Bin Dong 0001 |
NeurIPS | 3 |