Muon Induced Neutrino Tool (MINT)

Neutrino fluxes at muon colliders and neutrino factories. MINT decays muons along realistic accelerator lattices (built from MAD-X TFS tables or simple parametric geometries), including polarization, radiative corrections to the decay, and beam optics (beam size and divergence). It also propagates the neutrinos to arbitrary detector locations and estimates neutrino event rates with ray tracing through detector geometries.

pip install .            # from the repository root
pip install -e .[dev]    # editable install for development

import numpy as np
import mint

# 1. Load a collider-ring lattice shipped with MINT
print(mint.lattices.available())
ring = mint.lattices.load("mc_10tev_hybrid_v06")

# ... or build one from your own MAD-X TWISS/TFS file
# ring = mint.lattices.from_tfs("my_ring.tfs", emittance_RMS=5.25e-10, Nmu_per_bunch=2e12)

# 2. Decay muons along the ring (mu+ -> e+ nu_e nu_mu-bar)
sim = mint.MuDecaySimulator(
    muon_polarization=0.0,
    lattice=ring,
    nuflavor="numubar",
    n_evals=1e5,
    beam_dynamics=True,
)
sim.decay_muons()
sim.place_muons_on_lattice(lattice=ring, direction="clockwise")

# 3. Neutrino flux through a detector face 1 km downstream of the IP
E, flux = sim.get_flux_at_generic_location(
    det_location=[0, 0, 1e5],  # cm
    det_radius=2e2,            # cm
    ebins=np.linspace(0, 5e3, 31),
)

Vegas and caching. The event generation only samples the rest-frame muon decay phase space. Flavor, polarization, and radiative corrections are implemented by reweighting matrix-elements with the same sample:

sim_nue = sim.reweighted_copy(nuflavor="nue")      # no new vegas run
sim_nue.place_muons_on_lattice(lattice=ring, direction="clockwise")

sim.save_events("mudecays.npz")                    # persist the sample ...
sim2 = mint.MuDecaySimulator.load_events("mudecays.npz", lattice=ring)  # ... reuse later

Interaction vertices. Ray-trace the placed neutrinos through a detector and generate weighted interaction vertices, with exponential attenuation along each chord and upstream shielding included:

det = mint.detectors.benchmark                     # the benchmark forward detector
rates = det.signal_interactions(sim, nuflavor="numubar", exposure=ipy)
print(rates["total"])                              # interactions/year in the signal volume

A detector is a stack of coaxial material volumes, so you can build your own geometry by composing mint.detector_tools volumes with any Material. See MINT_examples/benchmark_detector.ipynb for a worked construction.

Partial lattices. If a TFS file covers only part of a machine — an interaction region of a larger ring, say — pass the full machine length. Decays are placed on the covered section while the muons age and decay over the whole ring:

ring = mint.lattices.load("mc_10tev_hybrid_v06", total_circumference=10e5)  # cm

mint.lattices.available() lists these; load() takes the name.

The tables are MAD-X TWISS output, stored gzip-compressed (they are repetitive text and shrink by ~96%); read_tfs decompresses transparently. Bring your own with mint.lattices.from_tfs("my_ring.tfs", emittance_RMS=...) — plain or gzipped, both work.

pip install -e ".[dev]"
pytest                    # the suite
pytest --cov=mint         # with a coverage report

Every push runs the suite on Python 3.10, 3.11 and 3.12, plus a ruff lint pass. See .github/workflows/tests.yml.

These check the properties the physics leans on: that the beam normalization closes including muon survival in the store, that the Courant–Snyder envelopes are self-consistent, that the detector column densities are what the rates assume, and that the cross-section backends agree.

Parts of this repository were written with the help of an AI assistant (Claude).

Scientific decisions from what to simulate, with what approximations, detector choices, the accelerator lattices, how to interpret the results, and everything in the accompanying paper was made by the authors.

The AI assistant was responsible for most of the package structure and import logic, writing the test suite and the continuous-integration setup, vast majority of the docstrings, parts of this README, the explanatory text in the notebooks, lots of debugging, and a fair amount of the analysis and plotting code.

If you find something wrong, please open an issue or contact us directly.

If you use MINT, please cite the accompanying paper:

@article{Choi:2026yzw,
    author = "Choi, Ju-Yeol and Hostert, Matheus and Li, Peiran and Liu, Zhen",
    title = "{The Forward Neutrino Flux and its Secondaries at a 10 TeV Muon Collider}",
    eprint = "2608.02718",
    archivePrefix = "arXiv",
    primaryClass = "hep-ph",
    month = "8",
    year = "2026"
}

python -m build

Artifacts land in dist/. The packaged data — cross-section tables and the reference lattices in mint/lattice_data/ — ships inside the wheel, so an installed user can run flux simulations without cloning the repository.