Mesh Field Theory: Port-Hamiltonian Formulation of Mesh-Based Physics
Abstract: We present Mesh Field Theory (MeshFT) and its neural realization, MeshFT-Net: a structure-preserving framework for mesh-based continuum physics that cleanly separates the physics' topological structure from its metric structure. Imposing minimal physical principles (locality, permutation equivariance, orientation covariance, and energy balance/dissipation inequality), we prove a reduction theorem for mesh-based physics. Under these conditions, the physical dynamics admit a local factorization into a port-Hamiltonian form: the conservative interconnection is fixed uniquely by mesh topology, whereas metric effects enter only through constitutive relations and dissipation. This reduction clarifies what must be fixed and what should be learned, directly informing MeshFT-Net's design. Across evaluations on analytic and realistic datasets, physics-consistency tests, and out-of-distribution validation, MeshFT-Net achieves near-zero energy drift and strong physical fidelity (correct dispersion and momentum conservation) along with robust extrapolation and high data efficiency. By eliminating non-physical degrees of freedom and learning only metric-dependent structure, MeshFT provides a principled inductive bias for stable, faithful, and data-efficient learning-based physical simulation.
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What is this paper about?
This paper introduces a new way to build computer models that simulate physical things like waves, fluids, or electricity on a mesh (a grid made of connected points, lines, and faces). The authors call it Mesh Field Theory (MeshFT), and they also build a neural network version named MeshFT-Net. Their big idea is to clearly separate two parts of physics:
- the “wiring” of how places are connected (topology), and
- the “measurements” like lengths, areas, material properties, or how much things resist or dissipate energy (metric).
By fixing the wiring and only learning the measurements, their models stay stable, obey basic physics (like not creating energy from nothing), and learn faster from less data.
What questions are they asking?
In simple terms, the paper asks:
- Can we design physics-learning machines that always respect basic physical rules, like not making energy out of nowhere and behaving the same if we flip directions on a mesh?
- If we force these basic rules, do the math and the physics “reduce” to a standard shape where the connections are fixed by the mesh, and only material-specific stuff needs to be learned?
- Will a model built with this principle be more accurate, more stable over long time periods, and better at handling new situations it hasn’t seen before?
How did they approach the problem?
Think of a mesh like a network of pipes:
- Topology is which pipes connect to which (who’s attached to whom, and in what direction).
- Metric is how wide each pipe is, how long it is, or what the fluid inside is like (water, oil, air)—the things that change how flow behaves.
The authors start by writing down four simple, very general rules that good physical models should follow:
- Locality: Each part only looks at its nearby neighbors, not the whole mesh at once.
- Permutation equivariance: If you relabel the mesh points or parts, the physics shouldn’t change.
- Orientation covariance: If you flip the direction of an arrow on an edge or face (like reversing a pipe’s direction), the math changes sign where it should, but the physics itself doesn’t change.
- Energy balance (passivity): The system has a conservative part that doesn’t create or destroy energy, plus an optional dissipative part that can only remove energy (like friction). Without sources, total stored energy can’t go up.
Using these rules, they prove a “reduction theorem.” In everyday language:
- No matter which specific physics you’re learning (waves, electromagnetics, etc.), as long as you follow the four rules, the “conservative” part of the system (the part that moves energy around without creating or destroying it) must be wired exactly by the mesh connections and their directions. This is a port-Hamiltonian form—a standard, energy-based way to describe systems as “conservative wiring” plus “dissipation.”
- All the geometry and material effects (like density, stiffness, or damping) go into separate “learnable” pieces called metric and dissipation operators. That means the model doesn’t need to learn who’s connected to whom; it only learns how strongly and in what way the material responds.
They then build MeshFT-Net to match this proof:
- The conservative wiring is hard-coded from the mesh (so it can’t cheat).
- The network only learns the metric (how energies map to forces) and dissipation (how things lose energy).
- They use a stable time-stepping scheme that splits the evolution into a conservative pass and a damping pass, helping prevent numerical explosions.
Short analogies to keep in mind:
- Skeleton and muscles: Topology is the skeleton (the fixed connections). Metric is the muscles and tissues (how the system moves and resists).
- Road map: Topology is which roads connect cities. Metric is how long each road is and the speed limit.
- Wiring diagram: Topology is which wires connect which components. Metric/dissipation are the component values (resistors, capacitors).
What did they find, and why is it important?
Main findings:
- Theory: They prove that, under the four rules, the conservative part of any mesh-based physics must follow a standard “incidence wiring” given by the mesh. In other words, the connection structure isn’t something to learn—it’s already determined by the mesh’s topology. Only metric- and dissipation-related parts should be learned.
- Architecture: MeshFT-Net implements exactly this: fixed interconnection, learn metric and dissipation. No need to assume a particular PDE upfront.
- Experiments show:
- Near-zero energy drift: Over long simulations, the model does not mysteriously gain or lose energy when it shouldn’t.
- Correct physical behavior: It preserves momentum well and gets wave properties like speed and dispersion right.
- Robust generalization: It stays accurate even when tested on different meshes, different resolutions, different frequencies, or different materials than those seen during training.
- Data efficiency: It learns good behavior from less data compared to common baselines like MeshGraphNets (MGN), Hamiltonian Neural Networks (HNN), and neural operators.
Why this matters:
- Stability: Simulations don’t blow up or drift away from physical behavior over time.
- Faithfulness: Results look and feel like real physics—not “spurious modes” or weird non-physical artifacts.
- Efficiency: Since the model learns only what’s truly unknown (metrics/dissipation), it needs less data and generalizes better.
What could this change going forward?
- Better simulators: Engineers and scientists can get faster, more trustworthy simulations for things like acoustics, fluids, or electromagnetics on complex meshes.
- Clearer modeling: The method tells you what to hard-code (the mesh wiring) and what to learn (material behavior and damping). That helps avoid overfitting to non-physical patterns.
- Transfer across problems: Because the wiring is fixed by topology, models can transfer across different mesh shapes and sizes more reliably.
- Safer use in the wild: With stronger physical guarantees (like non-increasing energy without sources), these models are less likely to produce nonsense in long-term predictions.
In short, the paper shows that if you respect four simple physical principles, the complicated part of physics on meshes falls into a neat, energy-based form. That lets you lock in the right structure and only learn what actually depends on the material and geometry, leading to stable, accurate, and data-efficient simulations.
Knowledge Gaps
Knowledge gaps, limitations, and open questions
Below is a single, consolidated list of what remains missing, uncertain, or unexplored in the paper, phrased to guide concrete future research.
- Only a local (Jacobian-level) reduction is proven: conditions under which the port-Hamiltonian structure integrates to a single global model (global H, J, R) are not characterized.
- Differentiability requirements are implicit: how the reduction applies with piecewise-smooth networks (e.g., ReLU MLPs) at nondifferentiable points and how this impacts training and guarantees remain unclear.
- Strict convexity and block-separable storage H is assumed; extensions to nonconvex energies (e.g., multiwell potentials, plasticity) and cross-degree energy couplings are not developed.
- The paper adopts state-independent interconnection J for most results; a systematic framework for learning and regularizing state-dependent incidence gains Ck(z) with stability/passivity guarantees is not provided.
- Identifiability of learned metric G and dissipation R from data is not analyzed: multiple (G, R) factorizations can fit the same trajectories up to scaling or similarity transforms; uniqueness conditions are open.
- Parameterization of G (diagonal or small Cholesky blocks) may be too restrictive for strongly anisotropic, chiral, or gyrotropic media; how to scale to full SPD operators (with tractable learning) is not addressed.
- Constraint- and gauge-rich systems (e.g., incompressible flow, electromagnetism’s Gauss constraints, cohomology/harmonic forms) are not treated; mechanisms to enforce constraints and handle null spaces are missing.
- Boundary conditions are handled empirically (e.g., open/reflective in The Well) but lack a principled port/Dirac-structure treatment; learning boundary ports/impedances while preserving passivity remains an open design problem.
- External inputs and control ports are mentioned but not instantiated or evaluated; how to learn input maps and preserve passivity in closed-loop scenarios is untested.
- Coverage of nonlinear advection/convection-dominated systems (e.g., Navier–Stokes) is absent; whether fixed incidence wiring suffices or requires robust state-dependent coupling for such nonlinear transport is unresolved.
- Behavior in the presence of shocks/discontinuities (hyperbolic conservation laws) is largely unexplored beyond mild acoustic cases; entropy consistency and shock-capturing mechanisms compatible with MeshFT are not developed.
- The locality assumption (L) excludes nonlocal or fractional operators; strategies to extend MeshFT to long-range interactions or fractional PDEs are not provided.
- Generalization to 3D, curved manifolds, high-order elements, and complex polyhedral meshes is not demonstrated; how curvature and high-order DEC impact parameterization and guarantees is unclear.
- Dynamic/moving meshes and adaptive mesh refinement are out of scope; how to update topology-fixed interconnection on-the-fly and keep learned G/R consistent is an open question.
- Orientation covariance is formalized, but a general recipe for constructing orientation-even/odd feature channels for vector/tensor fields (and ensuring expressivity) is not fully specified; risks of under- or over-constraining remain.
- The effect of including non-physical metadata (types, categorical features) on symmetry and passivity constraints is not analyzed; guidelines to prevent symmetry violation are missing.
- Discrete-time guarantees are empirical: the Strang splitting with half-damping and CFL guard is used, but a proof of discrete passivity/energy decay and error bounds (vs. step size) is not provided.
- Handling stiffness (e.g., strong dissipation) and large time steps is not analyzed; stability regions of the chosen integrator and alternatives that preserve structure in the discrete time setting are not compared.
- Scalability to very large meshes and training-time memory/compute constraints (e.g., backprop through long rollouts, distributed training) are not benchmarked.
- Multi-physics couplings (e.g., thermoelasticity, piezoelectricity, MHD) across multiple cochain ladders and fields are not addressed; how to compose interconnections and metrics across subsystems is open.
- Ambiguity at cohomology/harmonic modes on domains with nontrivial topology is unaddressed; how MeshFT treats harmonic subspaces (not seen by Dk) and their energetic contributions is unclear.
- Robustness to mesh quality issues (high aspect ratios, irregular connectivity) and their effect on learned G/R and stability is not evaluated.
- Learning under partial observability and noise (e.g., when only a subset of fields like pressure is supervised) lacks a theoretical identifiability/stability analysis and systematic regularization strategies.
- More expressive dissipation models (nonsmooth/monotone but not differentiable, e.g., Coulomb friction, plasticity) and their discrete integration within MeshFT are not developed.
- The empirical scope is narrow (primarily linear waves and a small nonlinear toy); performance on turbulent flows, strongly nonlinear elastodynamics, or broader subsets of The Well remains to be demonstrated.
- Interaction between one-step teacher-forced training and long-horizon stability is not analyzed; whether rollout losses or multi-step training improve fidelity without harming passivity is open.
- Effect of CFL guard policy on accuracy and generalization is not studied; adaptive stepping and error control strategies compatible with MeshFT are not explored.
- Extension to nonlocal learning of Hodge operators (e.g., data-driven but mesh-independent parameterizations) while retaining topology-fixed interconnection needs investigation.
- Formal conditions connecting the principles (L/P/O/E) to existing DEC/FEM discretizations (consistency and convergence to continuum limits) are not established.
Practical Applications
Immediate Applications
The following use cases can be deployed now by leveraging MeshFT’s topology–metric split, fixed incidence-based interconnection, and the MeshFT-Net implementation with CFL-guarded Strang splitting and learned metric/dissipation operators.
- Stable learned surrogates for linear and weakly damped wave phenomena (acoustics, elastodynamics, electromagnetics)
- Sectors: software, engineering (automotive/aerospace/civil), audio/AR-VR, healthcare (ultrasound), telecom (RF/EM propagation)
- What to deploy:
- “MeshFT-Acoustics” for room/building acoustics, cabin NVH predesign, and AR/VR spatial audio
- “MeshFT-EM” for FDTD-like time-domain EM propagation in fixed media (EMC/antenna prechecks, indoor RF planning)
- “MeshFT-Vib” for structural vibration surrogates (modal responses, long-horizon decay with Rayleigh damping)
- Workflow: train MeshFT-Net on solver-generated trajectories; integrate as a surrogate time-stepper in existing FEM/FDTD pipelines; use CFLGUARD for stability and physics-consistency diagnostics (wave speed, momentum, energy drift) as QA gates
- Assumptions/dependencies: near-Hamiltonian or mildly dissipative regimes; mesh topology available; boundary conditions handled consistently in training/deployment; state-independent interconnection adequate (linear media)
- Resolution-robust and parameter-robust simulation across meshes
- Sectors: software (CAE vendors), HPC, engineering consulting
- What to deploy: multi-resolution surrogates that generalize across mesh refinements and material parameters for rapid parameter sweeps and design-of-experiments
- Workflow: pretrain on coarse meshes, deploy on finer meshes using fixed incidence operators; use MeshFT’s O(N) sparse matvec updates for fast rollouts
- Assumptions/dependencies: geometric/topological consistency across meshes; training ranges cover expected parameter variations
- Physics-consistency test suite for ML simulators
- Sectors: software QA, academia, standards bodies
- What to deploy: a lightweight “PhysCheck” harness implementing the paper’s diagnostics (energy drift, wave-speed error, canonical consistency, PDE residuals, equipartition, momentum conservation)
- Workflow: incorporate tests into CI pipelines for ML surrogates; gate model promotions on pass/fail thresholds
- Assumptions/dependencies: access to states and derivatives from the surrogate; reference energy metric defined or learned
- Structure-preserving components for graph-based simulators
- Sectors: software (ML frameworks), academia
- What to deploy: PyTorch/TF layers that expose signed-incidence wiring and orientation covariance, plus SPD/PSD parameterizations for metric/dissipation (e.g., “MeshFT-Layers”)
- Workflow: replace unconstrained message-passing blocks with MeshFT blocks in existing GNN simulators; retain learned constitutive/dissipation modules only
- Assumptions/dependencies: oriented cell complexes available; adherence to locality/permutation equivariance in surrounding architecture
- Constitutive/dissipation learning with guaranteed energy behavior
- Sectors: materials/structures, academia
- What to deploy: learning of discrete Hodge operators (metric) and Rayleigh-type dissipation on fixed meshes while pinning the conservative interconnection
- Workflow: fit Ge (SPD) and Re (PSD) from motion data; use learned operators within DEC/FEM solvers for calibrated predictions
- Assumptions/dependencies: constitutive behavior can be captured by local metric/dissipation operators; sufficient excitation in training data
- Accelerated what-if analysis and digital prototyping
- Sectors: architecture/urban planning (noise), automotive/aerospace (acoustics/EMC)
- What to deploy: plug-ins for COMSOL/ANSYS/Clawpack/FEniCS to offload time stepping to MeshFT-Net for rapid scenario evaluation
- Workflow: generate training pairs from the in-house solver; embed MeshFT-Net as a co-simulation component with live parameter knobs (materials, sources)
- Assumptions/dependencies: solver can export/import mesh and states; domain lies within tested regimes (linear/weakly nonlinear, mild dissipation)
- Education and training tools for structure-preserving numerics
- Sectors: education, academia
- What to deploy: interactive notebooks and demos showing orientation covariance, incidence coupling, and energy-preserving/dissipative behaviors
- Workflow: use the released code/datasets to teach DEC, port-Hamiltonian structure, and stable integrators
- Assumptions/dependencies: basic familiarity with meshes and differential forms
- Preconditioning and operator surrogates within DEC/FEM solvers
- Sectors: HPC, software
- What to deploy: learned metric (Hodge star) approximations as preconditioners or surrogate operators to reduce linear solve cost
- Workflow: train on representative subproblems; insert learned SPD blocks into solver pipelines with safeguards (eigenvalue bounds)
- Assumptions/dependencies: solver hooks for custom preconditioners; stable spectra preserved by learned SPD approximations
Long-Term Applications
These applications require further research in nonlinear coupling, state-dependent interconnections, multiphysics, complex boundaries, or large-scale deployment.
- Nonlinear and multiphysics simulation (e.g., shallow water with shocks, fluid–structure interaction, nonlinear elastodynamics)
- Sectors: energy (offshore), civil engineering, environmental modeling
- Potential products: “MeshFT-Nonlinear” supporting state-dependent interconnection gains Ck(z) and richer dissipation beyond Rayleigh
- Dependencies: robust learning of Ck(z) while preserving incidence wiring; stabilization for discontinuities (Riemann solvers, limiters); validated benchmarks for strong nonlinearity
- Turbulent and high–Reynolds-number flows with structure preservation
- Sectors: aerospace, automotive, climate/CFD software
- Potential products: MeshFT-enhanced LES/RANS surrogates that encode incidence-driven conservation and learned subgrid dissipation
- Dependencies: extension from wave-like to advective-dominated regimes; incorporation of invariants (e.g., kinetic energy, enstrophy) into the passivity framework; coupling with turbulence closures
- Real-time digital twins with certified passivity for control
- Sectors: robotics (soft robots), manufacturing (machine tools), energy systems (vibration monitoring)
- Potential products: embedded MeshFT surrogates with passivity certificates for closed-loop control and monitoring
- Dependencies: demonstrable stability under feedback; online parameter identification for metric/dissipation; edge deployment optimizations
- Inverse problems and constitutive discovery from sparse observations
- Sectors: healthcare (elastography/ultrasound), nondestructive testing, geophysics
- Potential products: “MeshFT-Inverse” to recover spatially varying Ge/Re (material maps) from limited sensor data using the fixed-topology inductive bias
- Dependencies: differentiable solvers with adjoints; uniqueness/identifiability guarantees; noise robustness
- Large-scale geoscience and climate meshes (global wave/EM/seismic propagation)
- Sectors: climate, energy exploration, disaster mitigation
- Potential products: MeshFT surrogates for regional seismic hazard assessment or EM subsurface imaging with energy-stable long-horizon rollouts
- Dependencies: handling complex boundary conditions and heterogeneities at scale; AMR and multiresolution compatibility; HPC training/inference pipelines
- Standardization and certification of ML-accelerated physics solvers
- Sectors: policy/standards, regulated industries (aerospace, medical devices)
- Potential outputs: guideline documents and benchmarks using MeshFT’s diagnostics for acceptance criteria (energy drift thresholds, momentum conservation)
- Dependencies: consensus on test suites; alignment with existing V&V frameworks; community datasets beyond The Well
- Interactive design and topology optimization with MeshFT-in-the-loop
- Sectors: mechanical design, acoustics, antenna engineering
- Potential products: differentiable MeshFT modules enabling fast gradients for shape/material optimization under physics-consistent dynamics
- Dependencies: verified differentiability through the MeshFT time-stepper; coupling with CAD/mesh morphing; guardrails for stability during optimization
- AMR, high-order elements, and curved geometries
- Sectors: scientific computing software
- Potential products: MeshFT extensions for high-order DEC/FEM and dynamically adapting meshes while preserving orientation covariance and incidence coupling
- Dependencies: consistent cochain transfer across refinements; stability analysis under mesh changes; efficient sparse kernels
- On-device physics for AR/VR and wearables
- Sectors: consumer electronics
- Potential products: low-latency spatial audio or haptics driven by MeshFT surrogates with guaranteed energy behavior
- Dependencies: model compression and quantization; power/latency budgets; robust handling of dynamic scenes and moving boundaries
- Cross-domain operator libraries and plug-ins
- Sectors: software ecosystem
- Potential products: standardized “MeshFT-Core” libraries for PyTorch/TF/JAX, and plug-ins for COMSOL, ANSYS, FEniCS, Clawpack
- Dependencies: API alignment with solver internals; user-friendly tooling for orientation management and incidence extraction; maintenance of SPD/PSD constraints during training
Notes on Feasibility Assumptions
- The current strongest evidence is for mesh-based, near-linear wave-like systems with mild, local dissipation and fixed (state-independent) conservative interconnection; extensions to state-dependent coupling are promising but need more validation.
- Orientation covariance and energy balance/passivity must be respected end-to-end (data curation, boundary handling, and architecture) to realize the advertised stability.
- Success depends on high-quality meshes with correct incidence operators and consistent boundary/source modeling during training and deployment.
- While MeshFT promotes data efficiency, adequate coverage of parameter and boundary variations in training remains important for robust generalization.
Glossary
- Autonomous update: A time-invariant evolution rule for the state that depends only on the current state. "and consider an autonomous update ż = F(z)."
- Cell complex: A combinatorial structure made of cells (vertices, edges, faces, etc.) with orientations used to model mesh topology. "Let K be a finite oriented cell complex of di- mension d."
- Coboundary operator: The incidence map taking k-cochains to (k+1)-cochains, satisfying a nilpotency property that encodes topology. "the coboundary operator Dk satisfies Dk+1Dk = 0"
- Cochain: An assignment of scalar values to oriented k-dimensional cells of a mesh. "For each k, let Ck ~ Rnk denote the space of real-valued k-cochains (one scalar per oriented k-cell)"
- Co-energy: The conjugate (energy-coordinate) variable obtained as the gradient of the storage function with respect to the state. "Define the co-energy (conjugate) variable e := VH(z)"
- Coface: A (k+1)-dimensional cell that has a given k-cell as a face; part of the local neighborhood in a mesh. "a k-cell receives only from itself, its own faces (k - 1)-cell, and its own cofaces (k + 1)-cell."
- Conservative interconnection: The energy-preserving coupling structure in a port-Hamiltonian system determined by topology. "the conservative interconnection is fixed uniquely by mesh topology"
- Courant–Friedrichs–Lewy (CFL) condition: A stability condition relating time step size to spatial discretization and wave speeds. "to satisfy a target CFL condition (Courant et al., 1967; Le Veque, 1992)."
- Delaunay triangulation: A triangulation that maximizes the minimum angle of all triangles, used here as a mesh type for evaluation. "regular grids and Delaunay triangulations."
- Discrete exterior calculus (DEC): A discrete framework for differential forms on meshes that preserves topological identities. "Discrete exterior calculus (DEC) (Hirani, 2003; Desbrun et al., 2005a;b) argues that mesh topology already provides the algebraic backbone for differential operators"
- Energy balance: The decomposition of dynamics into parts that do no net work and parts that dissipate energy, ensuring non-increasing stored energy. "(E) Energy balance and passivity."
- Energy drift: The accumulated deviation of a model’s energy from perfect conservation over a rollout. "MeshFT- Net achieves near-zero energy drift"
- Equipartition: The balanced sharing of energy between kinetic and potential components in oscillatory systems. "kinetic-potential equipartition"
- Exterior calculus: The calculus of differential forms on manifolds, separating topological and metric components of operators. "In ex- terior calculus on a manifold (Flanders, 1963)"
- Exterior derivative: The topological (metric-independent) operator mapping k-forms to (k+1)-forms. "the exterior derivative d is topological (metric-independent)"
- Finite-difference time-domain (FDTD): A structure-preserving time-stepping method commonly used in computational electromagnetics. "finite-difference time- domain (FDTD)"
- Hamiltonian vector field: The vector field defined by a Hamiltonian function that governs conservative dynamics. "aligns v(z) with the Hamiltonian vector field X He (z)"
- Hodge star: A metric-dependent operator mapping k-forms to (n−k)-forms, introducing geometry into discrete operators. "metric- dependent operators such as the Hodge star *."
- Incidence-normalized coordinates: A state reparameterization that absorbs incidence gains so the interconnection uses pure signed incidences. "we ... work in the incidence-normalized coordinates"
- Jacobian: The matrix of partial derivatives of the dynamics with respect to the state, used for local linearization and reduction. "At any point where the Jacobian exists"
- k-cell: A k-dimensional element of a cell complex, such as a vertex (0-cell), edge (1-cell), or face (2-cell). "one scalar per oriented k-cell"
- Orientation covariance: The requirement that flipping mesh orientations only flips oriented variables while leaving scalar quantities unchanged. "(O) Orientation covariance."
- Out-of-distribution (OOD): A testing regime where inputs differ from the training distribution to assess generalization. "out-of-distribution (OOD) validation"
- PDE residual: The discrepancy between predicted fields and those satisfying the governing partial differential equation. "(iii) PDE residual,"
- Permutation equivariance: Invariance of a model’s outputs under relabelings (permutations) of mesh entities. "permu- tation equivariance"
- Port-Hamiltonian: A system formulation that separates energy storage, interconnection (skew), and dissipation, enabling energy-consistent modeling. "a local factorization into a port-Hamiltonian form"
- Rayleigh damping: A linear damping model often proportional to combinations of mass and stiffness matrices. "We also test a Rayleigh-damped setting"
- Signed-incidence wiring: The sparsity and sign pattern of conservative couplings determined by signed incidence matrices of the mesh. "signed-incidence wiring dictated by the mesh topol- ogy,"
- Skew interconnection: An energy-preserving coupling matrix J with JT = −J in the port-Hamiltonian factorization. "constant skew interconnection JT = - J"
- Storage function: A strictly convex energy function that maps states to stored energy and defines co-energy variables. "We equip the state z = (zk, Zk+1) € Ck @ Ck+1 with a storage function H"
- Strang splitting: A second-order operator-splitting integrator that alternates sub-steps for different components of the dynamics. "Strang splitting (Strang, 1968)"
- Symmetric positive-definite (SPD): A matrix property ensuring positive energy metrics; used for learned metric operators. "Ge is degreewise SPD, implemented as diagonals (softplus) or small Cholesky blocks,"
- Symplectic step: A time-integration step that preserves the symplectic structure of Hamiltonian systems, aiding long-term stability. "MeshFT-Net's topological interconnection with a symplec- tic step yields orders of magnitude greater robustness."
- Topology–metric separation: The modeling principle that topological operators are fixed by mesh incidence while metric effects are learned. "explicit topology-metric separation"
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