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Python API Reference

The nereids Python package is a PyO3 layer over the Rust pipeline. This page is a curated narrative reference covering the typed APIs Python users reach for most often, with argument tables, array-shape contracts, and dispatch rules.

For the exhaustive auto-generated reference (every function, class, and attribute exported by the package), see the generated Python API reference built by pdoc from the installed wheel and the shipped nereids/__init__.pyi type stubs.

Install the base package with:

pip install nereids

Optional extras are:

pip install "nereids[mcp]"  # MCP server console script
pip install "nereids[gui]"  # GUI wheel dependency, when available for your platform

Data Objects

ResonanceData

Returned by load_endf(...), load_endf_file(...), and create_resonance_data(...).

Important properties:

PropertyTypeMeaning
zintAtomic number.
aintMass number.
awrfloatAtomic weight ratio.
n_resonancesintResonance count across parsed ranges.
target_spinfloatTarget spin from the first evaluable range (parse-and-skip placeholders are skipped).
scattering_radiusfloatEffective scattering radius in fm, from the first evaluable range.
l_valueslist[int]Orbital angular momentum values present in the data.
has_unevaluated_rangesboolTrue when the file carries parsed-but-not-evaluated spans (LRF=7 / URR / LRU=0); those spans contribute zero cross-section.
skipped_rangeslist[str]One description per parsed-but-not-evaluated span.

FitResult

Returned by fit_spectrum_typed(...) and fit_counts_spectrum_typed(...).

PropertyTypeMeaning
densitiesNDArray[float64]Fitted areal densities in atoms/barn.
uncertaintiesNDArray[float64]One-sigma density uncertainties; entries may be NaN when covariance is unavailable.
reduced_chi_squaredfloatPearson chi-squared per degree of freedom for LM/transmission paths.
deviance_per_doffloat or NonePrimary goodness-of-fit for counts-KL fits.
convergedboolWhether the optimizer converged.
iterationsintIteration count.
temperature_kfloat or NoneFitted temperature when fit_temperature=True.
t0_us, l_scalefloat or NoneFitted energy-scale parameters when fit_energy_scale=True.

InputData

Opaque typed 3D input for spatial mapping. Create it with:

data = nereids.from_transmission(transmission, uncertainty)
data = nereids.from_counts(sample_counts, open_beam_counts)

The spectral axis is always axis 0, so arrays have shape (n_energy, height, width).

SpatialResult

Returned by spatial_map_typed(...).

PropertyTypeMeaning
density_mapslist[NDArray[float64]]One (height, width) density map per isotope or isotope group.
uncertainty_mapslist[NDArray[float64]]Per-pixel density uncertainty maps.
chi_squared_mapNDArray[float64]Per-pixel reduced chi-squared for LM/transmission paths.
deviance_per_dof_mapNDArray[float64] or NonePrimary GOF map for counts-KL spatial fits.
converged_mapNDArray[bool_]Per-pixel convergence flags.
n_converged, n_failed, n_totalintPixel fit counts.
temperature_mapNDArray[float64] or NoneFitted temperature map when enabled.
temperature_uncertainty_mapNDArray[float64] or NonePer-pixel 1σ temperature uncertainty (K) when fit_temperature=True. Covariance-only lower bound on the raw-count joint-Poisson path: it captures only statistical curvature (inverse Fisher matrix), omits baseline/model noise, and on real data can underestimate the observed per-superpixel scatter by ~3–4×. Pass scale_by_chi2=True for a goodness-of-fit-scaled estimate: σ is multiplied by sqrt of the deviance_per_dof each pixel’s result reports. This inflates σ for an under-fit pixel (D/dof > 1) and, less commonly, shrinks it for an over-fit one (D/dof < 1). The flag is a no-op on the already-χ²-scaled LM transmission path.
anorm_map, background_mapsNDArray[float64] / list[...] or NoneSAMMY Anorm and the polynomial background [BackA, BackB, BackC] per pixel when background=True.
back_d_map, back_f_mapNDArray[float64] or NoneSAMMY exponential background BackD / BackF per pixel when background=True and fit_back_d=True / fit_back_f=True. Counts-KL spatial runs always return None for both (the joint-Poisson dispatch never fits the exponential tail).
t0_us_map, l_scale_mapNDArray[float64] or NoneEnergy-scale maps when enabled.

NexusData

Returned by load_nexus_histogram(...) and load_nexus_events(...).

PropertyTypeMeaning
countsNDArray[float64]Counts cube with shape (n_tof, height, width).
tof_edges_usNDArray[float64]TOF bin edges in microseconds, length n_tof + 1.
flight_path_mfloat or NoneFlight path from NeXus metadata when available.
dead_pixelsNDArray[bool_] or NoneDead-pixel mask, True means dead.
n_rotation_anglesintNumber of rotation angles in histogram input.
event_total, event_keptint or NoneEvent loader statistics.

ENDF Loading

u238 = nereids.load_endf(92, 238, library="endf8.1")
u238_local = nereids.load_endf_file("examples/data/u238_ex027.endf")

load_endf(...) fetches and caches evaluated nuclear data. Supported library names include endf8.0, endf8.1, jeff3.3, jendl5, tendl2023, and cendl3.2. First use can require network access; cached files are reused afterwards. load_endf_file(...) parses a local ENDF file and does not download data.

Both loaders evaluate resolved LRF=1/2/3 ranges only. A file with no evaluable range (for example a pure LRF=7 evaluation such as W-182) raises ValueError — loading it would yield zero cross-section everywhere. A mixed evaluation loads, emits a UserWarning naming the skipped spans, and flags them via has_unevaluated_ranges / skipped_ranges.

Forward Modeling

import numpy as np
import nereids

u238 = nereids.load_endf(92, 238)
energies = np.linspace(1.0, 30.0, 2000)

transmission = nereids.forward_model(
    energies,
    [(u238, 0.001)],
    temperature_k=300.0,
    flight_path_m=25.0,
    delta_t_us=5.0,
    delta_l_m=0.005,
)

forward_model(...) returns a 1D float64 transmission spectrum on the input energy grid. Pass either isotopes=[(ResonanceData, density), ...] or groups=[(IsotopeGroup, density), ...], but not both. Gaussian resolution is enabled by the flight_path_m, delta_t_us, and delta_l_m parameters. Tabulated resolution can be supplied with resolution=load_resolution(...).

delta_t_us and delta_l_m are W-parameters, the width in exp(-x^2/W^2), not standard deviations. The conversions are sigma = W/sqrt(2) and FWHM = 2*sqrt(ln 2)*W = 1.6651*W. This is SAMMY’s convention, shared with the Doppler width, so the two kernels compose without a conversion. A measured 1-sigma timing jitter must be converted before it is passed here; supplying it unconverted gives a kernel 29 % too narrow, and a resolution that is too narrow is absorbed into a fitted temperature that is too high.

Two helpers do the conversion, so no one has to scale by hand:

FunctionConvertsFormula
width_from_sigma(sigma)a standard deviationW = sigma * sqrt(2)
width_from_fwhm(fwhm)a full width at half maximumW = FWHM / (2*sqrt(ln 2))
resolution = nereids.resolution_broaden(
    energies,
    cross_sections,
    flight_path_m=25.0,
    delta_t_us=nereids.width_from_sigma(0.5),   # 0.5 us measured 1-sigma
    delta_l_m=nereids.width_from_sigma(2e-3),
)

width_from_fwhm is also the conversion SAMMY’s Deltag needs, so a timing width read from a SAMMY .inp can be passed straight through it.

Single-Spectrum Fitting

Transmission Data

result = nereids.fit_spectrum_typed(
    transmission,
    uncertainty,
    energies,
    [(u238, 0.0005)],
    temperature_k=300.0,
    solver="lm",
)

Shape contract:

  • transmission, uncertainty, and energies are 1D arrays with the same length.
  • energies is in eV and should be ascending.
  • isotopes supplies (ResonanceData, initial_density) pairs.

Keyword arguments:

OptionMeaning
temperature_k=293.6Sample temperature in kelvin.
fit_temperature=FalseFit sample temperature in addition to densities.
max_iter=200Maximum optimizer iterations.
solver="lm""lm" (default) or "auto". The count-likelihood names ("kl", "poisson", "joint_poisson") are rejected for normalized transmission — a ratio is not Poisson count data.
background=FalseEnable SAMMY-style transmission background parameters.
fit_back_d=False, fit_back_f=FalseFit optional exponential background terms.
back_d_init=0.01, back_f_init=1.0Initial exponential background values.
fit_energy_scale=FalseFit TOF energy-scale parameters t0_us and l_scale.
t0_init_us=0.0, l_scale_init=1.0Initial energy-scale values.
energy_scale_flight_path_m=25.0Nominal flight path for energy-scale fitting.
resolution=...Tabulated resolution from load_resolution(...). Mutually exclusive with the Gaussian parameters below — pass either resolution= (tabulated) or the flight_path_m/delta_t_us/delta_l_m trio (Gaussian), never both.
flight_path_m=..., delta_t_us=..., delta_l_m=...Gaussian resolution parameters (mutually exclusive with resolution=).
fit_energy_range=(emin, emax)Restrict the cost function to an energy window.
groups=[...]Fit isotope groups instead of individual isotopes.
initial_densities=[...]Initial density guesses when fitting groups.
tzero_jacobian="..."Select the TZERO Jacobian implementation.

Raw Counts

result = nereids.fit_counts_spectrum_typed(
    sample_counts,
    open_beam_counts,
    energies,
    [(u238, 0.0005)],
    solver="auto",
    c=1.0,
)

solver="auto", "kl", "poisson", and "joint_poisson" all route counts data to the counts-KL dispatch; solver="lm" is rejected because dividing the count arms into transmission loses count statistics. Use c=Q_s / Q_ob when sample and open-beam counts have different proton charge or dwell-time normalization. The primary GOF for this path is FitResult.deviance_per_dof.

Counts fitting accepts the same temperature, background, and group options as transmission fitting.

Resolved Counts (Exact Separate-Arm Response)

Instrument response acts on the open and sample count arms separately: the detector observes O_i = Σ_j F_j R_ij and S_i = Σ_j F_j T_j R_ij, never a broadened transmission ratio R[T]. To fit raw counts with an active resolution, supply the exact-response inputs:

result = nereids.fit_counts_spectrum_typed(
    sample_counts,               # per measured detector-time bin
    open_beam_counts,            # per measured detector-time bin
    energies,                    # true-energy quadrature (may differ in length)
    [(u238, 0.0005)],
    solver="kl",
    resolution=response,         # TabulatedResolution or IkedaCarpenter
    incident_fluence_weights=F,  # F_j = w_j * eps(E_j) * Phi(E_j)
    detector_time_edges_us=edges,  # len(edges) == len(sample_counts) + 1
    timing_offset_us=0.0,
)

The true-energy grid and the measured detector-time bins are different axes: energies drives the physics model while the count arrays live on the detector clock. two_arm_count_response(...) is the same operator exposed standalone for synthesizing or checking expected counts (it additionally reports the per-arm acquisition-window loss). A resolution without the exact-response inputs still fails closed with a ValueError, and fit_energy_scale / fit_energy_range are not yet supported through the exact response (the response clock and the energy axis would disagree).

Counts specific options are:

OptionMeaning
detector_background=...Reserved detector background spectrum; the counts-KL dispatch rejects non-zero values.
c=1.0Proton-charge ratio Q_s / Q_ob.
enable_polish=True/False/NoneOverride counts-KL polish behavior; None uses the dispatcher default.
resolution=..., incident_fluence_weights=..., detector_time_edges_us=..., timing_offset_us=0.0Exact separate-arm response inputs (see above).

The counts-domain alpha_1/alpha_2 nuisance parameters are not fit by fit_counts_spectrum_typed or spatial_map_typed. Only compute_model_jacobian retains the alpha parameters, as a research/UQ surface.

Independently Measured Count Backgrounds

background_fit = nereids.fit_two_arm_background_templates(
    observed_open_counts,
    observed_sample_counts,
    open_signal,                 # from two_arm_count_response(...)
    sample_signal,
    open_exposure_scale,
    sample_exposure_scale,
    ["blocked_beam"],
    open_background_templates,   # 2-D, one row per named component
    sample_background_templates,
    initial_amplitudes,
    open_loss,                   # the two losses from the same
    sample_loss,                 # two_arm_count_response(...) call
)

Each row of the two template matrices is a fixed detector-bin shape from an independent measurement such as blocked-beam or detector-only data. NEREIDS fits only a non-negative amplitude per component and returns all three pieces for each arm — the fixed neutron signal, the fitted background, and their exact total — so they are never conflated. This count background is added after the instrument response and is not the SAMMY transmission-level background.

The code deliberately does not generate a flexible residual curve, and it cannot establish a template’s provenance: fitting a free curve to the residual it is meant to explain would identify nothing physical, so callers must retain the independent measurement record themselves.

open_exposure_scale and sample_exposure_scale are required. They convert the common reference neutron signal into expected counts for each complete acquisition (proton charge, live time, or another documented exposure), so a run-normalization difference between the arms cannot be absorbed as background. The scales apply to the neutron signal and its window losses only — templates are never multiplied by them, so supply each arm’s template already expressed in that arm’s own exposure. (Supplying a per-unit-exposure template to a 3× exposure arm biases its amplitude by ~50% while the fit still looks only mildly poor.)

open_window_loss and sample_window_loss are also required: pass the two losses that two_arm_count_response returned alongside the signals. They are the acquisition-window disclosure the result carries forward, exposure-scaled; they are never defaulted, because a default of zero would be a false “no loss” report.

The returned TwoArmBackgroundFitResult reports whether the amplitudes are separately determined:

AttributeMeaning
amplitudes, namesFitted non-negative amplitude per named component.
amplitudes_identifiableFalse when two supplied shapes are linearly dependent. The total background is still valid, but the individual amplitudes are not physically interpretable.
amplitude_uncertaintiesOne-sigma values from the expected (Fisher) information of the constrained fit, or None when withheld (the fit did not converge, the amplitudes are not identifiable, or the free block of the information matrix is singular). Free amplitudes are conditioned on any partner held at its bound. An individual entry is NaN when its variance is non-positive or when its template is sensitive on a bin with zero expectation, where the expected information diverges; a reported number is never zero.
amplitude_at_boundTrue where the data pull an amplitude negative and the non-negativity bound holds it at zero. Its reported sigma is then a one-sided curvature scale, not a symmetric interval.
open_total, sample_totalneutron_signal + background, exactly.
open_window_loss, sample_window_lossExpected counts lost outside the acquisition window, exposure-scaled and reported rather than renormalized away.
poisson_deviance, deviance_per_dofGoodness of fit.
n_informativeBins that contribute to the deviance — the observation, the neutron signal, or at least one template is nonzero there. Bins where all three are exactly zero are excluded from the degrees of freedom.

Background amplitude estimation is a standalone analysis surface: it is not a solver route, and the counts-KL dispatch still rejects a non-zero detector_background (see the option table above).

Spatial Mapping

Pre-Normalized Transmission Cubes

data = nereids.from_transmission(transmission_3d, uncertainty_3d)
result = nereids.spatial_map_typed(
    data,
    energies,
    [u238],
    initial_densities=[0.0005],
    solver="auto",
)

For from_transmission(...) inputs both solver="lm" (default) and solver="auto" route to LM; a Poisson/KL count likelihood is rejected for normalized transmission because the separate open/sample count arms are no longer available. density_maps[0] is the fitted U-238 map.

Raw Count Cubes

data = nereids.from_counts(sample_counts_3d, open_beam_counts_3d)
result = nereids.spatial_map_typed(
    data,
    energies,
    [u238],
    initial_densities=[0.0005],
    solver="auto",
    c=1.0,
)

solver="auto" uses counts-KL for from_counts(...) data and populates deviance_per_dof_map.

Shape contract:

  • sample_counts_3d, open_beam_counts_3d, transmission_3d, and uncertainty_3d use shape (n_energy, height, width).
  • energies.shape == (n_energy,).
  • dead_pixels, when supplied, uses shape (height, width) with True marking pixels to skip.

Keyword arguments:

OptionMeaning
temperature_k=293.6, fit_temperature=FalseFixed or fitted sample temperature.
initial_densities=[...]Initial density guesses.
dead_pixels=...(height, width) skip mask.
max_iter=200Maximum per-pixel optimizer iterations.
solver="auto"Dispatch from input type unless explicitly set.
background=FalseEnable SAMMY-style background for LM/transmission paths.
fit_back_d=False, fit_back_f=FalseFit the SAMMY exponential background tail (BackD * exp(-BackF / √E)). Requires background=True. Per-pixel back_d_map / back_f_map are populated on the returned SpatialResult (issue #538).
back_d_init=0.01, back_f_init=1.0Initial values for the exponential tail.
c=1.0Proton-charge ratio for counts-KL spatial fitting.
enable_polish=True/False/NoneOverride counts-KL polish behavior; None auto-disables polish for multi-pixel maps.
fit_energy_scale=FalseFit per-pixel t0_us and l_scale maps.
t0_init_us=0.0, l_scale_init=1.0Initial energy-scale values.
energy_scale_flight_path_m=25.0Nominal flight path for energy-scale fitting.
resolution=...Tabulated resolution from load_resolution(...). Mutually exclusive with the Gaussian parameters below — pass either resolution= (tabulated) or the flight_path_m/delta_t_us/delta_l_m trio (Gaussian), never both. Rejected for count cubes: counts input with active resolution fails closed (the exact separate-arm model is single-spectrum only for now) — fit pre-normalized transmission cubes instead.
flight_path_m=..., delta_t_us=..., delta_l_m=...Gaussian resolution parameters (mutually exclusive with resolution=; same count-cube rejection applies).
groups=[...]Fit isotope groups instead of individual isotopes.
tzero_jacobian="..."Select the TZERO Jacobian implementation.
fit_energy_range=(emin, emax)Restrict the cost function to an energy window.

Pixel Masks

Pixel masks exist only to exclude pipeline-corrupting pixels (dead or hot/railed detector defects). They are not a data-quality or coverage filter: low-count pixels are alive and must be kept (the KL-domain fitters handle them), and coverage/thickness inhomogeneity is a model concern, not a masking concern. Downstream, a masked pixel is hard-excluded — never fitted, NaN in the result maps. Masks are (height, width) boolean arrays, True = exclude, and feed directly into spatial_map(dead_pixels=...).

# Recommended entry point: dead ∪ hot over sample AND open beam.
mask = nereids.detect_bad_pixels(sample, open_beam=open_beam)

# Individual criteria:
dead = nereids.detect_dead_pixels(sample)             # exactly zero in every TOF bin
hot  = nereids.detect_hot_pixels(sample, k_mad=6.0)   # railed/hot point defects
gone = nereids.detect_dead_pixels_chunked([chunk_a, chunk_b])  # intermittent deadness

result = nereids.spatial_map(cube, energies, isotopes, dead_pixels=mask)

detect_bad_pixels(sample, open_beam=None, hot_k_mad=6.0)

Union mask dead(sample) ∪ hot(sample) [∪ dead(ob) ∪ hot(ob)] — deadness and hotness are per-acquisition, so a mask built from one stack alone misses failures in the other. This is the validating entry point (rejects non-finite/negative counts and empty TOF axes with ValueError). hot_k_mad=None disables the hot screen (dead-only mask).

detect_dead_pixels(data)

Legacy single-stack detector: flags pixels that are exactly 0.0 in every TOF bin. Assumes counts already validated finite and non-negative; prefer detect_bad_pixels for new code.

detect_hot_pixels(data, k_mad=6.0)

Two-stage hot/railed screen on raw counts: a global robust cut on log total counts (median + k_mad · max(1.4826 · MAD, Poisson floor)) nominates candidates, and a local 8-neighbor confirmation (≥ 10× the neighbors’ median, iterated to a fixpoint) keeps contiguous bright scene regions — open-beam areas, slit apertures — unmasked while catching isolated point, line, and small-cluster defects. Pass raw detected counts, not proton-charge-normalized rates or transmission ratios: scaling breaks the Poisson floor.

detect_dead_pixels_chunked(chunks)

Intermittent deadness: a pixel dead for part of the acquisition is invisible in a summed stack (uniformly reduced counts, no zeros). Given per-chunk stacks (e.g. per-run splits or event data re-histogrammed in time windows), flags pixels all-zero in any chunk. Chunk so that live pixels expect λ ≥ 20 counts each (false-flag probability ≤ m·e^(−λ)). Spatial dims must match across chunks; the TOF axis may differ.

TIFF and NeXus I/O

stack = nereids.load_tiff_stack("transmission_stack.tif", pixel_policy="allow")
folder_stack, info = nereids.load_tiff_folder(
    "frames",
    pattern="frame_*.tif",
    sum_chunks=True,        # sum chunked VENUS runs element-wise (default)
    pixel_policy="reject",  # "reject" | "clip" | "allow" (default "reject")
    return_info=True,       # also return the load-provenance dict
)
info["n_chunks"]            # DAQ chunks detected (1 if not chunked)
info["chunks_summed"]       # True when they were summed element-wise
info["n_clipped_pixels"]    # pixels clamped under pixel_policy="clip"
# full key set: n_files, n_chunks, chunk_ids, chunks_summed,
# n_clipped_pixels, chunk_inconsistent, n_unrecognized_files,
# unrecognized_examples
edges_us = nereids.read_tof_sidecar(
    "run_764/run_764_Spectra.txt",
    n_frames=folder_stack.shape[0],
)

sample = nereids.load_nexus_histogram("sample.nxs")
open_beam = nereids.load_nexus_histogram("open_beam.nxs")
energies = nereids.tof_to_energy_centers(
    sample.tof_edges_us,
    sample.flight_path_m or 25.0,
)
health = nereids.run_health("sample.nxs")   # RunHealth: pause/beam-dip fractions

load_tiff_folder detects chunked VENUS folders (<prefix>_<chunk>_<frame>.tif) and sums chunks element-wise by default, emitting a UserWarning naming the summed chunks (and one with the clipped-pixel count under pixel_policy="clip"); return_info=True returns the load provenance as a second value. read_tof_sidecar converts a VENUS *_Spectra.txt sidecar (frame start times in seconds — the left bin edges, verified on measured autoreduce output) into the N+1 ascending microsecond TOF bin edges that tof_to_energy_centers expects. Negative or non-finite pixels are rejected at load time unless pixel_policy says otherwise. run_health returns a RunHealth summary of the /entry/DASlogs pause and beam-power logs using last-value-held time-weighted integration (SNS PV-name defaults).

See Data I/O and NeXus/TOF for ordering and pairing rules, chunk semantics, the pixel-value policy, and run health.

Beam-State Filtering (DASlogs and Event Banks)

Facility NeXus files record slow-control PVs under /entry/DASlogs/<pv> as transition logs: each value takes effect at its timestamp and persists until the next entry. Averaging the value array directly is wrong whenever entries are unevenly spaced — on a real VENUS run the entry-mean of the pause log read 0.43 while the time-weighted pause fraction was 0.90.

read_run_log(path, pv)

Returns a RunLog with times (seconds since run start), values, duration_s, offset_iso (ISO-8601 epoch of the clock), and n_dropped_corrupt — the number of corrupt device-reconnect records (backward time jumps or subnormal garbage payloads, both seen in real SNS files) dropped from the log.

intervals_where(times, values, duration_s, min_value=None, max_value=None)

Derives (t_start, t_end) intervals where the PV satisfies the bounds, under correct step-function semantics: the last value persists to duration_s (padded one f32 ULP — SNS records duration in float32 while pulse times are float64, and the final pulse of about half of real runs is stamped just beyond it), time before the first entry never matches, NaN never matches, and adjacent segments merge.

intervals_intersect(a, b)

Composes conditions across PVs (e.g. not-paused AND beam power above threshold). Inputs are validated and normalised (sorted, merged).

load_nexus_bank_spectrum(path, bank, n_bins, tof_min_us, tof_max_us, keep_intervals=None)

Loads one NXevent_data bank (e.g. "monitor1") as a BankSpectrum — a 1-D TOF spectrum (tof_edges_us, counts) with retention statistics (pulses_total/pulses_kept, events_total/events_kept, drop counters, pulse_time_offset_iso). With keep_intervals, only pulses whose event_time_zero falls inside the intervals (half-open, DASlogs clock) are histogrammed. units attributes are required on both event datasets (never guess a scale); a bank with zero events loads gracefully to a zero spectrum — on VENUS every imaging-detector bank is empty because tpx1 is frame-mode, and only monitors carry events.

pause = nereids.read_run_log("run.nxs.h5", "pause")
live = nereids.intervals_where(
    pause.times, pause.values, pause.duration_s, max_value=0.5
)
power = nereids.read_run_log("run.nxs.h5", "BL10:Det:rtdl:BeamPowerAvg")
stable = nereids.intervals_where(
    power.times, power.values, power.duration_s, min_value=1.5
)
keep = nereids.intervals_intersect(live, stable)

mon = nereids.load_nexus_bank_spectrum(
    "run.nxs.h5", "monitor1",
    n_bins=500, tof_min_us=0.0, tof_max_us=16667.0,
    keep_intervals=keep,
)
print(mon.pulses_kept, "/", mon.pulses_total, "pulses in stable beam")

Element and Utility APIs

nereids.element_symbol(92)        # "U"
nereids.element_name(92)          # "Uranium"
nereids.parse_isotope_str("U-238") # (92, 238)
nereids.natural_abundance(92, 238)
nereids.natural_isotopes(26)
nereids.tof_to_energy(tof_us, flight_path_m)
nereids.energy_to_tof(energy_ev, flight_path_m)

How This Page Is Generated

The published docs site renders three things side by side:

Site pathSourceWhat it shows
/ (this page)Hand-maintained docs/guide/src/python-api.mdCurated narrative tour of the typed APIs
/python/pdoc over the installed nereids wheel and nereids/__init__.pyi stubsAuto-generated exhaustive reference
/api/cargo doc (rustdoc)Rust crate API reference

To rebuild the whole site locally:

pixi run doc-build   # depends on: doc-guide, doc-api, doc-python
pixi run doc         # serves target/book/ at http://localhost:8000

doc-python invokes pdoc -o target/book/python --no-show-source nereids after pixi run build has produced an importable wheel. Whenever bindings/python/python/nereids/__init__.pyi or PyO3 docstrings in bindings/python/src/lib.rs change, both the auto-generated python/ reference and any affected sections of this curated page should be reviewed in the same PR.

This page does not execute notebooks or compile-test Python snippets. The Rust quickstart on this site IS compile-tested by cargo check --workspace --examples (see crates/nereids-fitting/examples/quickstart.rs).