Adaptive Fast Multipole Method with Laplace kernel in JAX.
Project description
jaxFMM
jaxFMM is an open source implementation of the Fast Multipole Method in JAX. The goal is to offer an easily readable/maintainable FMM implementation with good performance that runs on CPU/GPU and supports autodiff. This is enabled through JAX's just-in-time compiler.
📖 Documentation: https://jaxfmm.gitlab.io/jaxfmm
Installation
jaxFMM depends only on JAX and can be installed from pypi or by downloading the source as follows:
pip install jaxfmm
If you want to run jaxFMM on GPUs, the easiest way is to use NVIDIA CUDA and cuDNN from pip wheels by instead typing:
pip install jaxfmm[cuda]
Using a custom, self-installed CUDA with jax is described in the JAX documentation.
Quickstart
The simplest entry point is a certified evaluator: pick a target accuracy, get a function.
import jaxfmm
fmm = jaxfmm.plan(pts, err_tol=1e-3) # picks + certifies a configuration on first call
pot = fmm(chrgs) # fast evaluations from then on
For explicit control, each engine offers the same two-call pattern (setup once per
geometry, evaluate per charge vector):
from jaxfmm import kifmm
s = kifmm.setup(pts, p=3) # tuned tree + operators for this point cloud
fmm = kifmm.compile_evaluator(s) # frozen, jitted: fmm(chrgs) -> potential
The flavors tour walks through every engine in a few lines each; demos/README.md describes the full demo set, including two inverse-design examples that differentiate straight through the FMM.
Engines
jaxFMM ships several FMM engines on two tree families, sharing one near-field module:
| engine | tree | best at |
|---|---|---|
flexible (jaxfmm.flex) |
non-uniform 2^N-ary, arbitrary box shapes | adaptive clouds, shape derivatives |
KIFMM (jaxfmm.kifmm) |
2:1-balanced cubic octree | general workhorse; potentials and fields (−∇φ); pluggable kernels |
uniform spherical-harmonic (jaxfmm.uniform) |
cubic octree, precomputed per-level operators | raw speed on space-filling clouds |
All engines support periodic boundary conditions (periodic_axes=, hierarchical lattice
operators, validated against the NaCl Madelung constant) and mixed-precision fast paths
(f32 kernels with f64 accumulation) where the extra noise provably sits below the
truncation error — accuracy-neutral defaults, opt-out via m2l_mixed/p2p_mixed.
Features
- Laplace kernel with real solid-harmonic bases computed via recurrence relations; rotation-based O(p^3) M2M/M2L/L2L on the flexible tree (following Goude & Engblom), equivalent-density (kernel-independent) and precomputed-operator variants on the cubic tree.
- Pluggable kernels on the KIFMM engine (
jaxfmm.kernels): bring five callables and a symmetry flag; Laplace and Yukawa ship built in (kifmm.setup(pts, kernel=jaxfmm.kernels.yukawa(2.0))). - End-to-end jit compilation; autodiff through charges and geometry (guarded
moving-geometry drivers rebuild capped tree topology inside jit — see
jaxfmm.driver). - Periodic boundary conditions in 1/2/3 axes for all engines.
- Finite-element sources: P0 volume + P1 surface charge FMM with singular
(Duffy) self-term correction (
jaxfmm.fem). - Micromagnetic stray-field evaluation for P1-FEM meshes
(
jaxfmm.apps.mag.strayfield, see below), Oersted fields from currents (jaxfmm.apps.mag.oersted). - Scales to 10^9 sources on a single 80 GB GPU.
For the full API reference and guide, see the documentation; for algorithmic details, see the paper; for the internal architecture, see ARCHITECTURE.md.
Stray Field Evaluation
jaxFMM is primarily developed for rapid stray field evaluation in finite-element micromagnetics:
from jaxfmm.apps.mag.strayfield import init_strayfield, eval_strayfield
h = init_strayfield(verts, tets, Ms) # geometry-fixed setup
H = eval_strayfield(m, **h) # stray field for a magnetization state
eval_strayfield supports both a lumped (fast, per-timestep) and an energy-consistent
autodiff mode (mode="diff"); the field-text demos show the full
pipeline including shape optimization through the solver.
Citing
jaxFMM is described in our Journal of Computational Physics paper:
@article{kraft2026jaxfmm,
title = {jaxFMM: An Adaptive, GPU-Parallel Implementation of the Fast Multipole Method in JAX},
author = {Robert Kraft and Florian Bruckner and Dieter Suess and Claas Abert},
journal = {Journal of Computational Physics},
pages = {115130},
year = {2026},
doi = {10.1016/j.jcp.2026.115130},
}
TODOs
jaxFMM is primarily developed for fast stray-field evaluation in finite-element micromagnetics, which explains the feature set and design decisions above. Contributions are always welcome; current directions in development:
- symmetry-class M2L application (validated prototype: ~3.7× on non-Laplace kernels, 17× operator-table memory) and further per-kernel performance work.
- multi-RHS evaluation (several charge vectors per tree traversal).
- distributed parallelism via jax.sharding.
- volume FMM (continuous source densities) — prototype exists, on hold.
AI-assisted development
jaxFMM is co-developed with Claude Code: large parts of the
library were written, benchmarked and refactored in human-directed agent sessions, with every
change gated by the test suite and reviewed by the maintainers. The repo is set up so agents are
first-class contributors: AGENTS.md (with CLAUDE.md as a compatibility import)
carries the working conventions, and ARCHITECTURE.md is the maintained
internal map — including the hard-won invariants and measured dead ends (§7/§8) that keep both
humans and agents from re-deriving or re-breaking things. If you contribute with an agent, point
it there first.
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