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sras-viewer/sras_compute.py
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2026-08-06 21:20:35 -05:00

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#!/usr/bin/env python3
"""Image computation and angle alignment for .sras scans.
Depends only on numpy/scipy (+ optional pyfftw) and sras_format, so a
multiprocessing child can import it without loading Qt or matplotlib —
which matters because Python 3.14 on macOS spawns rather than forks.
"""
import atexit
import json
import os
import threading
from concurrent.futures import ThreadPoolExecutor
from dataclasses import dataclass
from pathlib import Path
import numpy as np
import scipy.fft as scipy_fft
import scipy.ndimage as scipy_ndimage
from sras_format import (
CH1_IDX, CH3_IDX, CH4_IDX, PAD_FACTOR_MAX, SrasFile, adc_to_mv,
)
# ---------------------------------------------------------------------------
# FFT backend
# ---------------------------------------------------------------------------
try:
import pyfftw
PYFFTW_AVAILABLE = True
except ImportError:
PYFFTW_AVAILABLE = False
try:
from threadpoolctl import threadpool_limits
except ImportError:
threadpool_limits = None
_fft_backend = "scipy" # "scipy" or "pyfftw"; set via set_fft_backend()
def set_fft_backend(name: str):
"""Select the rfft implementation. Module-level state, so it must be set
explicitly inside each multiprocessing child — it does not survive a
spawn. "numpy" is accepted as a legacy alias for "scipy"."""
global _fft_backend
if name == "numpy":
name = "scipy"
_fft_backend = name if (name == "pyfftw" and PYFFTW_AVAILABLE) else "scipy"
def get_fft_backend() -> str:
return _fft_backend
def _do_rfft(x: np.ndarray, n: int | None = None, axis: int = -1,
workers: int = 1) -> np.ndarray:
"""Dispatch rfft to the selected backend with optional multithreading."""
if _fft_backend == "pyfftw" and PYFFTW_AVAILABLE:
return pyfftw.interfaces.numpy_fft.rfft(x, n=n, axis=axis, threads=workers)
return scipy_fft.rfft(x, n=n, axis=axis, workers=workers)
# ---------------------------------------------------------------------------
# FFT worker pool and per-thread pyFFTW plans
# ---------------------------------------------------------------------------
_FFT_BLOCK = 512 # waveforms per FFT task. The knee on a 16-core machine:
# smaller blocks serialise on GIL-held numpy dispatch,
# larger ones lose cache residency and task granularity.
_ZOOM_MIN_PAD = 4 # zoom refinement engages at n_fft >= _ZOOM_MIN_PAD * spf
_FFT_EXACT_ENV = bool(int(os.environ.get("SRAS_FFT_EXACT", "0") or 0))
_pool_lock = threading.Lock()
_pool: ThreadPoolExecutor | None = None
def _fft_pool() -> ThreadPoolExecutor:
"""The persistent process-wide pool for FFT block tasks."""
global _pool
with _pool_lock:
if _pool is None:
_pool = ThreadPoolExecutor(max_workers=_MAX_WORKERS,
thread_name_prefix="sras-fft")
atexit.register(_pool.shutdown, wait=False, cancel_futures=True)
return _pool
_WISDOM_PATH = Path.home() / ".cache" / "sras-viewer" / "fftw_wisdom"
_wisdom_lock = threading.Lock()
_wisdom_loaded = False
_fftw_local = threading.local()
def _load_wisdom_once():
"""Import saved FFTW wisdom so FFTW_MEASURE planning is a one-time cost
per machine. Purely an optimisation: failures are ignored."""
global _wisdom_loaded
with _wisdom_lock:
if _wisdom_loaded:
return
_wisdom_loaded = True
try:
pyfftw.import_wisdom(_WISDOM_PATH.read_bytes().split(b"\x00\n"))
except Exception:
pass
def _save_wisdom():
with _wisdom_lock:
try:
_WISDOM_PATH.parent.mkdir(parents=True, exist_ok=True)
_WISDOM_PATH.write_bytes(b"\x00\n".join(pyfftw.export_wisdom()))
except Exception:
pass
def _fftw_block_rfft(waves: np.ndarray, n: int) -> np.ndarray:
"""rfft of a (B, spf) float32 block via a cached per-thread FFTW plan.
Plans have a fixed (_FFT_BLOCK, spf) input shape so each worker thread
plans once per transform length; a remainder block runs through the same
plan with its tail rows ignored. The returned array is the plan's output
buffer — consume it before the next call on the same thread.
"""
n_wf, spf = waves.shape
plans = getattr(_fftw_local, "plans", None)
if plans is None:
plans = _fftw_local.plans = {}
key = (_FFT_BLOCK, spf, n)
plan = plans.get(key)
if plan is None:
_load_wisdom_once()
buf = pyfftw.empty_aligned((_FFT_BLOCK, spf), dtype="float32")
# No overwrite_input: FFTW must not scribble on input_array, whose
# zero-padded tail (columns spf..n) is zeroed exactly once here.
plan = pyfftw.builders.rfft(buf, n=n, axis=-1, threads=1,
planner_effort="FFTW_MEASURE")
plan.input_array[:] = 0.0
plans[key] = plan
_save_wisdom()
inp = plan.input_array
inp[:n_wf, :spf] = waves
return plan()[:n_wf]
def _block_rfft(waves: np.ndarray, n: int) -> np.ndarray:
"""Single-threaded rfft of one block; outer parallelism comes from the
pool, so the transform itself must not spin up threads."""
if _fft_backend == "pyfftw" and PYFFTW_AVAILABLE:
return _fftw_block_rfft(waves, n)
return scipy_fft.rfft(waves, n=n, axis=-1, workers=1)
# ---------------------------------------------------------------------------
# Zoom peak search: coarse rfft + local fine DFT around the winning bin
# ---------------------------------------------------------------------------
_ZOOM_HALFWIDTH = 0.75 # refinement window half-width, in coarse spacings.
# Every fine bin lies within 0.5 spacings of its
# nearest coarse bin, and that bin is guaranteed to
# be a candidate (see _ZOOM_CAND_RATIO), so 0.5
# suffices; 0.75 adds rounding margin.
_ZOOM_CAND_RATIO = 0.7 # refine every coarse bin within this power ratio of
# its row's coarse maximum. Quarter-natural-bin
# scalloping at the 2x-oversampled coarse grid can
# understate a peak by at most ~19% in power, so 0.7
# keeps a wide margin — near-contenders are resolved
# on the fine grid, never ranked from coarse samples.
@dataclass
class _ZoomPlan:
"""Constants for the coarse+refine peak search, built once per
compute_rf_image call and shared across worker threads. *phases* is a
lazily-filled window-start -> phase-vector cache; a benign duplicate
compute under concurrency is cheaper than locking."""
n_fft: int
n_coarse: int
m: int # fine bins per refinement window
n_bins_fine: int
E: np.ndarray # (spf, m) complex64 fine-DFT matrix, relative bins
j: np.ndarray # (spf,) float64 sample indices
phases: dict
def _zoom_plan(spf: int, n_fft: int) -> _ZoomPlan:
# 2x-oversampled coarse grid: the padded power spectrum is a trig
# polynomial of degree spf-1, so at 2x sampling its global max cannot
# hide between coarse bins.
n_coarse = scipy_fft.next_fast_len(2 * spf, real=True)
n_bins_fine = n_fft // 2 + 1
m = int(np.ceil(2 * _ZOOM_HALFWIDTH * n_fft / n_coarse)) + 1
m = min(m, n_bins_fine - 1)
j = np.arange(spf, dtype=np.float64)
E = np.exp((-2j * np.pi / n_fft) * np.outer(j, np.arange(m))).astype(np.complex64)
return _ZoomPlan(n_fft, n_coarse, m, n_bins_fine, E, j, {})
def _window_start(k_c: np.ndarray, zp: _ZoomPlan) -> np.ndarray:
"""First fine bin of the refinement window around each coarse bin.
Clipped to [1, ...] so fine bin 0 stays excluded (DC suppression)."""
k0 = np.floor((k_c - _ZOOM_HALFWIDTH) * (zp.n_fft / zp.n_coarse)).astype(np.int64)
return np.clip(k0, 1, max(1, zp.n_bins_fine - zp.m))
def _refine_window(waves: np.ndarray, rows: np.ndarray, k0: int, zp: _ZoomPlan,
best_pow: np.ndarray, best_bin: np.ndarray):
"""Evaluate fine bins k0..k0+m-1 for the given rows and fold the result
into the per-row best (power, bin), preserving np.argmax's lowest-bin
tie-break."""
ph = zp.phases.get(k0)
if ph is None:
ph = np.exp((-2j * np.pi * k0 / zp.n_fft) * zp.j).astype(np.complex64)
zp.phases[k0] = ph
F = (waves[rows] * ph) @ zp.E
q = F.real ** 2
q += F.imag ** 2
i = np.argmax(q, axis=1)
p = q[np.arange(len(rows)), i]
b = k0 + i
upd = (p > best_pow[rows]) | ((p == best_pow[rows]) & (b < best_bin[rows]))
ridx = rows[upd]
best_pow[ridx] = p[upd]
best_bin[ridx] = b[upd]
def _peak_bins_zoom(waves: np.ndarray, zp: _ZoomPlan) -> np.ndarray:
"""Peak fine-bin per waveform without materialising the padded spectrum:
coarse rfft, then a small fine DFT (one gemm per shared window) on the
exact n_fft bin grid. Identity with the full padded argmax is enforced
by tests/test_compute.py::test_zoom_identity and the golden-hash sweep."""
n_wf = waves.shape[0]
S = _block_rfft(waves, zp.n_coarse)
P = S.real ** 2
P += S.imag ** 2
P[:, 0] = 0.0
p_c = np.max(P, axis=1)
best_pow = np.full(n_wf, -1.0, dtype=np.float32)
best_bin = np.full(n_wf, np.iinfo(np.int64).max, dtype=np.int64)
# For a clean signal this yields one or two windows; a noise spectrum
# (many near-equal peaks) yields a dozen or so — still a tiny fraction
# of the padded grid.
thr = np.where(p_c > 0, np.float32(_ZOOM_CAND_RATIO) * p_c,
np.float32(np.inf))
rows_c, bins_c = np.nonzero(P >= thr[:, None])
k0_c = _window_start(bins_c, zp)
# Zeroing the coarse DC bin (suppression) blinds the candidate scan to
# fine bins closer to DC than the first coarse sample — where the
# DC-leakage skirt of an un-subtracted offset peaks. Always refine the
# DC-adjacent window too.
rows_c = np.concatenate([rows_c, np.arange(n_wf)])
k0_c = np.concatenate([k0_c, np.ones(n_wf, dtype=np.int64)])
pair = np.unique(np.stack([rows_c, k0_c], axis=1), axis=0)
for k0 in np.unique(pair[:, 1]):
_refine_window(waves, pair[pair[:, 1] == k0, 0], int(k0), zp,
best_pow, best_bin)
# An all-zero spectrum must reproduce argmax-of-zeros = bin 0.
best_bin[p_c == 0.0] = 0
return best_bin
def _peak_bins_direct(waves: np.ndarray, n_len: int) -> np.ndarray:
"""Peak bin per waveform via the full transform — for pad factors too
small for the zoom search to pay."""
S = _block_rfft(waves, n_len)
power = S.real ** 2
power += S.imag ** 2
power[:, 0] = 0.0
return np.argmax(power, axis=1)
# ---------------------------------------------------------------------------
# Chunking / parallel budget
# ---------------------------------------------------------------------------
#
# Row chunks are budgeted so all concurrently-live working buffers fit in
# memory; the worker count is derived from the budget, not vice versa.
# Rationale and the measured 1024 MB default: docs/design.md ("Memory budget
# and row chunking").
_TOTAL_BYTES_BUDGET = int(os.environ.get("SRAS_MEM_BUDGET_MB", 1024)) * 1024 * 1024
_CHUNK_ROWS_MAX = 32 # cap for small scans (original behavior)
_MAX_WORKERS = int(os.environ.get("SRAS_MAX_WORKERS", 0)) or (os.cpu_count() or 4)
def _chunk_rows_for(n_frames: int, samples_per_frame: int,
budget: int = _TOTAL_BYTES_BUDGET) -> int:
bytes_per_row = max(1, n_frames * samples_per_frame * 4) # float32
return int(max(1, min(_CHUNK_ROWS_MAX, budget // bytes_per_row)))
def _plan_fft_rows(n_frames: int, samples_per_frame: int, budget: int) -> int:
"""Rows per outer chunk for the block-FFT path. Only the float32
waveform buffer scales with the chunk (in-flight block spectra total a
few MB across the whole pool), so budget it with 2x slack and let the
block fan-out saturate the pool regardless of pad factor."""
bytes_per_row = max(1, n_frames * samples_per_frame * 4 * 2)
return int(max(1, min(_CHUNK_ROWS_MAX, budget // bytes_per_row)))
def _plan_chunks(n_rows: int, n_frames: int, samples_per_frame: int,
live_multiplier: int = 1,
max_workers: int | None = None,
budget: int | None = None) -> tuple[int, int]:
"""(chunk_rows, n_workers) such that all concurrent chunks together fit
the budget: n_workers x live_multiplier x chunk_rows x n_frames x
samples x 4 bytes <= budget.
The worker count is chosen *first* and the chunk sized to it. Sizing the
chunk first is the trap: _chunk_rows_for spends whatever budget it is
given, so a single chunk would always consume the lot and leave room for
exactly one worker — no concurrency, on precisely the large scans that
need it most.
A caller that is itself running several of these concurrently must pass
*both* max_workers=1 and its share of the budget. Capping the workers
alone is not enough: the chunk would still be sized against the whole
budget, and N concurrent callers would each allocate all of it.
"""
total = _TOTAL_BYTES_BUDGET if budget is None else max(1, budget)
cap = max_workers if max_workers is not None else _MAX_WORKERS
bytes_per_row = max(1, live_multiplier * n_frames * samples_per_frame * 4)
# A chunk is at least one row, so that alone caps how many can be live.
n_workers = int(max(1, min(cap, n_rows, total // bytes_per_row)))
chunk_rows = _chunk_rows_for(n_frames, samples_per_frame,
max(1, total // (n_workers * live_multiplier)))
# With chunk_rows known, more workers than chunks buys nothing.
n_workers = int(max(1, min(n_workers, -(-n_rows // chunk_rows))))
return chunk_rows, n_workers
def _map_row_chunks(n_rows: int, chunk_rows: int, n_workers: int, fn,
should_stop=None):
"""Apply fn(r0, r1) over row chunks, in parallel when it pays.
Chunks write to disjoint output slices, so no locking is needed. numpy
ufuncs, scipy's pocketfft, and memmap page faults all release the GIL, so
threads give real parallelism here — and on a very large file they also
keep many more page-fault requests in flight, which is what the I/O path
wants.
*should_stop* is polled per chunk so a cancelled job abandons work within
one chunk rather than one whole angle — on a large scan an angle is
~40 s, which is far too long to block application shutdown.
"""
bounds = [(r0, min(r0 + chunk_rows, n_rows))
for r0 in range(0, n_rows, chunk_rows)]
def run(b):
if should_stop is not None and should_stop():
return
fn(*b)
if n_workers <= 1 or len(bounds) == 1:
for b in bounds:
run(b)
return
with ThreadPoolExecutor(max_workers=min(n_workers, len(bounds))) as pool:
list(pool.map(run, bounds))
# ---------------------------------------------------------------------------
# Image computation
# ---------------------------------------------------------------------------
def plan_angle_level(sras: SrasFile,
live_multiplier: int = 1) -> tuple[int, int]:
"""(n_angle_workers, per_angle_budget) for a caller that parallelises
over angles instead of over rows.
Callers that parallelise over angles must not also let each angle
parallelise over rows: the two levels multiply, in threads and in memory.
Each angle is therefore given max_workers=1 and the returned budget share,
which together keep total live buffers within _TOTAL_BYTES_BUDGET.
"""
biggest = max(range(sras.n_angles), key=lambda a: int(sras.n_frames[a]))
_, n_workers = _plan_chunks(int(sras.n_rows[biggest]),
int(sras.n_frames[biggest]),
sras.samples_per_frame,
live_multiplier=live_multiplier)
n_workers = max(1, min(n_workers, sras.n_angles))
return n_workers, max(1, _TOTAL_BYTES_BUDGET // n_workers)
def compute_dc_image(sras: SrasFile, angle_idx: int, ch_idx: int,
max_workers: int | None = None,
budget: int | None = None,
should_stop=None) -> np.ndarray:
"""Mean of each waveform → (n_rows, n_frames) float32, in ADC counts.
Pass max_workers=1 when the caller is already parallelising over angles.
If *should_stop* ever returns True the result is incomplete — the caller
is expected to be abandoning it.
"""
n_rows, n_frames = sras.image_shape(angle_idx)
data = sras.data[angle_idx]
chunk_rows, n_workers = _plan_chunks(n_rows, n_frames, sras.samples_per_frame,
max_workers=max_workers, budget=budget)
img = np.empty((n_rows, n_frames), dtype=np.float32)
def chunk(r0: int, r1: int):
img[r0:r1] = data[r0:r1, ch_idx, :, :].astype(np.float32).mean(axis=-1)
_map_row_chunks(n_rows, chunk_rows, n_workers, chunk, should_stop=should_stop)
return img
def dc_image_mv(sras: SrasFile, angle_idx: int, ch_idx: int,
max_workers: int | None = None, budget: int | None = None,
should_stop=None) -> np.ndarray:
"""DC image for (angle, channel) in mV, preferring a stored v5/v7 cache."""
cached = sras.cached_dc_mv(angle_idx, ch_idx)
if cached is not None:
return cached
return adc_to_mv(
compute_dc_image(sras, angle_idx, ch_idx, max_workers=max_workers,
budget=budget, should_stop=should_stop),
*sras.cal(ch_idx))
def cached_rf_image(sras: SrasFile, angle_idx: int,
dc_threshold_mv: float | None,
apply_bg_sub: bool = True,
n_fft: int | None = None,
dc4_mv: np.ndarray | None = None,
allow_dc_recompute: bool = True) -> np.ndarray | None:
"""The stored peak-frequency image for one angle (v5 PREC or v7 CACH),
masked and ready to display — or None if no stored image can serve these
settings and a real FFT is needed.
Stored images are unmasked, so they serve any threshold — but they carry
one bg-sub state and one zero-padding, and a view asking for either of the
others is asking for different numbers, not a different rendering of the
same ones. Padding is the sharp edge: a pad-10 view resolves peaks on a
10x finer bin grid, so handing back a pad-1 image would quietly undo the
setting. v5 PREC and CACH v1 tails record no pad and are natural
resolution by construction.
Cheap enough to call on the GUI thread — a copy plus a comparison —
*except* when the CH4 mask has to be read from disk to build it. Pass
*allow_dc_recompute* False to return None in that case instead, and leave
the whole-channel read to a worker.
"""
cached_freq = sras.precomputed_freq_mhz[angle_idx]
# n_fft None means "no padding", i.e. exactly samples_per_frame points.
want_n_fft = n_fft if n_fft is not None else sras.samples_per_frame
if (cached_freq is None
or want_n_fft != sras.precomputed_pad_factor * sras.samples_per_frame
or sras.precomputed_bg_sub != (apply_bg_sub and sras.background is not None)):
return None
if dc_threshold_mv is None:
return cached_freq.copy()
# DC4 mask, in priority order: stored DC block, caller-supplied image,
# or a fresh (cheap — no FFT) recompute.
dc4_img = sras.cached_dc_mv(angle_idx, CH4_IDX)
if dc4_img is None:
dc4_img = dc4_mv
if dc4_img is None:
if not allow_dc_recompute:
return None
dc4_img = adc_to_mv(compute_dc_image(sras, angle_idx, CH4_IDX),
*sras.cal(CH4_IDX))
freq_img = cached_freq.copy()
freq_img[dc4_img < dc_threshold_mv] = 0.0
return freq_img
def compute_rf_image(sras: SrasFile, angle_idx: int,
dc_threshold_mv: float | None,
apply_bg_sub: bool = True,
n_fft: int | None = None,
dc4_mv: np.ndarray | None = None,
max_workers: int | None = None,
budget: int | None = None,
should_stop=None,
exact: bool = False) -> np.ndarray:
"""FFT of each CH1 waveform; pixel = peak frequency in MHz.
Pixels where CH4_dc < dc_threshold_mv are set to 0 — and the FFT is
never run for them, since that's the expensive part. The masked-out
CH1 samples are also never *read*: the boolean mask is applied to the
raw memmap slice before any dtype conversion, so numpy only pages in
the bytes for pixels that pass the threshold (an untouched memmap page
is never read from disk).
*dc_threshold_mv* of None means "mask nothing", and skips reading and
averaging CH4 entirely — worth a third of the I/O when caching a whole
file, where the mask is applied later at display time.
If the DC4 image for this angle is already known (e.g. from the
DC-channel precompute cache), pass it as *dc4_mv* (mV, shape
(n_rows, n_frames)) to reuse it instead of re-reading CH4 here.
At pad factors >= _ZOOM_MIN_PAD the padded spectrum is never
materialised: a coarse rfft finds each peak and a local fine DFT
resolves it on the exact n_fft bin grid (_peak_bins_zoom). *exact*
forces the reference full-padded transform instead — it exists for
tests, audits, and the SRAS_FFT_EXACT=1 escape hatch, and is slow and
memory-hungry at high pad.
Fast path: if the file has a precomputed peak-frequency image for this
angle (v5 PREC or v7 CACH), zero-padding is off, and the bg-sub flag
matches, the stored image is used directly — no FFT is run. That test is
cached_rf_image, which the viewer also applies before it ever dispatches
a compute at all.
"""
# ---- Fast path: precomputed image (v5 PREC or v7 CACH) ----------------
cached = cached_rf_image(sras, angle_idx, dc_threshold_mv,
apply_bg_sub=apply_bg_sub, n_fft=n_fft,
dc4_mv=dc4_mv)
if cached is not None:
return cached
# ---- Chunked FFT path --------------------------------------------------
n_rows, n_frames = sras.image_shape(angle_idx)
data = sras.data[angle_idx]
exact = exact or _FFT_EXACT_ENV
spf = sras.samples_per_frame
n_len = n_fft if n_fft is not None else spf
freq32 = sras.freq_axis_mhz(n_fft).astype(np.float32)
img = np.zeros((n_rows, n_frames), dtype=np.float32)
background = sras.background if (apply_bg_sub and sras.background is not None) else None
cal4 = sras.cal(CH4_IDX)
zp = (_zoom_plan(spf, n_fft)
if not exact and n_fft is not None and n_fft >= _ZOOM_MIN_PAD * spf
else None)
total = _TOTAL_BYTES_BUDGET if budget is None else max(1, budget)
cap = max_workers if max_workers is not None else _MAX_WORKERS
if exact:
# The reference path materialises the full padded spectrum, so rows
# are budgeted against it (complex64 + power + temp per bin) and the
# chunk runs as one serial transform.
bytes_per_row = max(1, n_frames * (4 * spf + 16 * (n_len // 2 + 1)))
chunk_rows = int(max(1, min(_CHUNK_ROWS_MAX, total // bytes_per_row)))
cap = 1
else:
chunk_rows = _plan_fft_rows(n_frames, spf, total)
pool = _fft_pool() if cap > 1 else None
def process(r0: int, r1: int):
if dc_threshold_mv is None:
valid = None
else:
if dc4_mv is not None:
dc4_chunk = dc4_mv[r0:r1]
else:
dc4_chunk = adc_to_mv(
data[r0:r1, CH4_IDX, :, :].astype(np.float32).mean(axis=-1), *cal4)
valid = dc4_chunk >= dc_threshold_mv # True = run the FFT
if not valid.any():
return
counts = (valid.sum(axis=1) if valid is not None
else np.full(r1 - r0, n_frames, dtype=np.int64))
offs = np.concatenate(([0], np.cumsum(counts)))
n_wf = int(offs[-1])
waves = np.empty((n_wf, spf), dtype=np.float32)
def read_row(i: int):
if should_stop is not None and should_stop():
return
# Index the raw memmap slice with the boolean mask *before*
# converting dtype — this is a lazy view until touched, so only
# the selected elements are actually read from disk; masked-out
# pixels' pages are never paged in at all.
raw = data[r0 + i, CH1_IDX]
dst = waves[offs[i]:offs[i + 1]]
dst[:] = raw[valid[i]] if valid is not None else raw
if background is not None:
dst -= background # background is 1-D (spf,)
if pool is None:
for i in range(r1 - r0):
read_row(i)
else:
list(pool.map(read_row, range(r1 - r0)))
out = np.empty(n_wf, dtype=np.float32)
def fft_block(b0: int):
if should_stop is not None and should_stop():
return
b1 = min(b0 + _FFT_BLOCK, n_wf)
w = waves[b0:b1]
bins = (_peak_bins_zoom(w, zp) if zp is not None
else _peak_bins_direct(w, n_len))
out[b0:b1] = freq32[bins]
if exact:
spectrum = _do_rfft(waves, n=n_fft, axis=-1, workers=1)
power = spectrum.real ** 2
power += spectrum.imag ** 2
power[:, 0] = 0.0 # suppress DC bin
out[:] = freq32[np.argmax(power, axis=1)]
elif pool is None:
for b0 in range(0, n_wf, _FFT_BLOCK):
fft_block(b0)
else:
list(pool.map(fft_block, range(0, n_wf, _FFT_BLOCK)))
# Boolean scatter is row-major, matching the read pass's
# concatenation order.
if valid is not None:
img[r0:r1][valid] = out
else:
img[r0:r1] = out.reshape(r1 - r0, n_frames)
# BLAS must not thread under the pool (the fine-DFT gemm would multiply
# against the pool's own workers).
limiter = (threadpool_limits(limits=1)
if pool is not None and threadpool_limits is not None else None)
try:
for r0 in range(0, n_rows, chunk_rows):
if should_stop is not None and should_stop():
break
process(r0, min(r0 + chunk_rows, n_rows))
finally:
if limiter is not None:
limiter.unregister()
return img
# ---------------------------------------------------------------------------
# Batch cache (Convert menu) — process-pool entry point
# ---------------------------------------------------------------------------
def cache_file(path: str, mode: str, apply_bg_sub: bool,
fft_backend: str = "scipy", max_workers: int = 0,
pad_factor: int = 1) -> str:
"""Compute and store DC or FFT images for every angle of one file,
converting v6 → v7 in place. Returns "" on success or an error message.
Module-level and picklable so it can run in a ProcessPoolExecutor. The
FFT backend, worker cap and pad factor are passed explicitly because
module globals do not survive a spawn.
*pad_factor* is stored alongside the images: a cache is only usable by a
view asking for the same padding, so caching at the viewer's own setting
is the difference between a batch that pays off and one that can never be
read back (see cached_rf_image).
"""
global _MAX_WORKERS
try:
if mode not in ("dc", "fft"):
return f"unknown cache mode {mode!r} (expected 'dc' or 'fft')"
set_fft_backend(fft_backend)
if max_workers:
_MAX_WORKERS = max_workers
sras = SrasFile(path)
if sras.version not in (6, 7):
return (f"unsupported version {sras.version} — only v6/v7 files "
"can be batch-cached")
n = sras.n_angles
n_workers, angle_budget = plan_angle_level(sras)
if mode == "dc":
dc3 = _parallel_map(
lambda a: adc_to_mv(
compute_dc_image(sras, a, CH3_IDX, max_workers=1,
budget=angle_budget), *sras.cal(CH3_IDX)),
range(n), n_workers)
dc4 = _parallel_map(
lambda a: adc_to_mv(
compute_dc_image(sras, a, CH4_IDX, max_workers=1,
budget=angle_budget), *sras.cal(CH4_IDX)),
range(n), n_workers)
sras.write_v7_cache(new_dc3_mv=dc3, new_dc4_mv=dc4)
else:
effective_bg = apply_bg_sub and sras.background is not None
pad = max(1, min(PAD_FACTOR_MAX, int(pad_factor)))
n_fft = None if pad <= 1 else sras.samples_per_frame * pad
# dc_threshold_mv=None: store unmasked images and mask at display
# time (same convention as v5's PREC block). Skipping the mask
# also skips reading CH4 entirely. The FFT path parallelises
# internally over blocks, so angles run one at a time with the
# full budget.
freq = [compute_rf_image(sras, a, dc_threshold_mv=None,
apply_bg_sub=effective_bg, n_fft=n_fft)
for a in range(n)]
sras.write_v7_cache(new_freq_mhz=freq, new_bg_sub=effective_bg,
new_pad_factor=pad)
return ""
except Exception as exc:
return str(exc)
# ---------------------------------------------------------------------------
# Angle alignment (Fusion menu)
#
# Rigid transforms only (rotation + translation, never scale), computed in mm
# on two frames: each angle's "local mm" (origin at its own array center) and
# the reference angle's local mm. Angle 0 is the sole coordinate authority;
# every other angle is placed purely by image content. Why, and the full
# frame/affine conventions: docs/design.md ("Angle alignment coordinate
# frames").
# ---------------------------------------------------------------------------
@dataclass
class AngleTransform:
rotation_deg: float
shift_mm: tuple[float, float] # (dx_mm, dy_mm) in ref mm
matrix: np.ndarray # (2,2): canvas (row,col) -> this angle's raw (row,col)
offset: np.ndarray # (2,)
score: float = 1.0 # registration NCC (1.0 = reference/manual)
source: str = "" # image that won registration: "signal"/"mask"
@dataclass
class AlignmentResult:
ref_angle_idx: int
dc_threshold_mv: float
canvas_shape: tuple[int, int] # (n_rows, n_cols)
canvas_dx_mm: float
canvas_dy_mm: float
canvas_origin_mm: tuple[float, float] # mm at canvas pixel index (0, 0)
per_angle: dict[int, AngleTransform]
@dataclass
class ManualAngleParams:
"""One angle's manual-alignment state, independent of any canvas.
rotation_deg/shift_mm are exactly AngleTransform's non-derived fields — the
rigid map from this angle's local mm to ref mm, the pair a canvas-bound
AngleTransform's matrix/offset get built from once a canvas is decided
(build_manual_alignment). Defaults to identity: a fresh angle with no prior
alignment is shown centered on the reference with no rotation, which is the
same "fully unaligned" state Clear Alignment resets back to.
"""
rotation_deg: float = 0.0
shift_mm: tuple[float, float] = (0.0, 0.0)
# Side length of the grid the rotation refinement runs on. The whole cost of
# registration scales with it: ~325 ms per candidate rotation at 640, roughly
# quadrupling per doubling, against ~200 MB of live masked-correlation buffers
# (see _registration_workers). 640 puts a full-size scan at ~0.1 mm/px, which
# resolves rotation on a 20 mm sample to well under a tenth of a degree.
_DEFAULT_FINE_DIM = 640
@dataclass
class RigidFit:
"""What register_angle_to_reference found for one angle."""
rotation_deg: float
shift_mm: tuple[float, float]
score: float # zero-mean NCC over the valid overlap
source: str # "signal", "mask", or "reference"
def _skimage_phase_cross_correlation():
"""Import skimage.registration lazily and cache it.
Deliberately not a module-level import: this module is imported by every
multiprocessing child (see the module docstring), skimage costs ~0.6 s to
import, and no child ever registers anything — registration runs in GUI-
process threads.
"""
global _pcc
try:
return _pcc
except NameError:
from skimage.registration import phase_cross_correlation as _fn
_pcc = _fn
return _pcc
# ---- Geometry: local mm, ref mm, and the one affine builder ---------------
def pixel_pitch_mm(sras: SrasFile, angle_idx: int) -> tuple[float, float]:
"""(dx, dy) mm/pixel for one angle: dx is the file-wide constant
pixel_x_mm; dy is this angle's own row spacing (assumed uniform, the same
assumption _redraw_image makes when it builds the display extent). dy keeps
its sign, so +row always means the same physical direction as +y."""
y = sras.y_positions_mm(angle_idx)
return sras.pixel_x_mm, (float(y[1] - y[0]) if len(y) > 1 else 1.0)
def _center_idx(sras: SrasFile, angle_idx: int) -> np.ndarray:
"""(row, col) index of this angle's array center — the origin of its local
mm frame. Purely geometric: it depends on the array shape and nothing
else, which is what keeps local mm free of stage position."""
n_rows, n_frames = sras.image_shape(angle_idx)
return np.array([(n_rows - 1) / 2.0, (n_frames - 1) / 2.0])
def ref_center_mm(sras: SrasFile, ref_angle_idx: int) -> np.ndarray:
"""Stage mm of the reference angle's array center: ref mm + this == stage
mm.
The single bridge between ref mm and stage mm, and the only place in the
whole alignment path where any angle's stage position is read at all —
which is why it takes the *reference* index by name rather than an
arbitrary angle.
"""
x = sras.x_axis_mm(ref_angle_idx)
y = sras.y_positions_mm(ref_angle_idx)
return np.array([(x[0] + x[-1]) / 2.0, (y[0] + y[-1]) / 2.0], dtype=np.float64)
def _local_half_extent_mm(sras: SrasFile, angle_idx: int) -> tuple[float, float]:
"""(half width, half height) in mm from this angle's array center to the
center of its outermost pixel."""
n_rows, n_frames = sras.image_shape(angle_idx)
dx, dy = pixel_pitch_mm(sras, angle_idx)
return (n_frames - 1) / 2.0 * abs(dx), (n_rows - 1) / 2.0 * abs(dy)
def _rotation_matrix(theta_deg: float) -> np.ndarray:
t = np.radians(theta_deg)
c, s = np.cos(t), np.sin(t)
return np.array([[c, -s], [s, c]]) # CCW rotation acting on (x, y)
def nominal_delta_deg(sras: SrasFile, angle_idx: int, ref_idx: int) -> float:
"""The rotation-stage's own reported angle change between two angles.
Used only to *seed* the rotation search, never as the answer: the stage's
sign convention relative to this module's math-positive (CCW, x toward y)
convention in scan mm is not knowable from the file, so
register_angle_to_reference scores both +this and -this and lets the image
content decide (see _rotation_candidates).
"""
return float(sras.angles_deg[angle_idx] - sras.angles_deg[ref_idx])
def _footprint_corners_ref_mm(sras: SrasFile, angle_idx: int,
rotation_deg: float,
shift_mm: tuple[float, float]) -> np.ndarray:
"""This angle's 4 footprint corners mapped into ref mm by its rigid
transform, shape (4, 2). Zero-padding cost, not content: it is the scan
window's corners, which is what the shared canvas has to cover."""
hw, hh = _local_half_extent_mm(sras, angle_idx)
corners = np.array([[sx * hw, sy * hh] for sx in (-1.0, 1.0) for sy in (-1.0, 1.0)])
R = _rotation_matrix(rotation_deg)
return corners @ R.T + np.asarray(shift_mm, dtype=np.float64)
def _affine_out_to_src(*, out_pitch_mm: tuple[float, float],
out_origin_ref_mm, src_dx_mm: float, src_dy_mm: float,
src_center_idx, src_center_off_mm=(0.0, 0.0),
rotation_deg: float = 0.0,
shift_mm: tuple[float, float] = (0.0, 0.0)
) -> tuple[np.ndarray, np.ndarray]:
"""matrix, offset s.t. src_index = matrix @ [row_out, col_out] + offset,
matching scipy.ndimage.affine_transform's output->input convention.
The single affine builder behind every resampling in this module — the
registration grid, the manual-alignment preview and the final canvas all
differ only in their arguments.
Pipeline (mm unless noted):
[X;Y] = A_out @ [row_out;col_out] + out_origin_ref_mm # out idx -> ref mm
[lx;ly] = R(rotation)^T @ ([X;Y] - shift) # ref mm -> this angle's local mm
[row;col] = D @ ([lx;ly] - src_center_off) + src_center_idx
*src_center_off_mm* is the local-mm position of the source array's own
center, nonzero only when the source has been block-mean downsampled (its
center can land up to half a block off the full-resolution center — see
_prepare_reg_image). Everything is expressed relative to array centers, so
no per-angle stage coordinate appears anywhere in here.
"""
Rinv = _rotation_matrix(rotation_deg).T
A_out = np.array([[0.0, out_pitch_mm[0]], [out_pitch_mm[1], 0.0]]) # [row,col] -> [x,y]
D = np.array([[0.0, 1.0 / src_dy_mm], [1.0 / src_dx_mm, 0.0]]) # [x,y] -> [row,col]
b_out = np.asarray(out_origin_ref_mm, dtype=np.float64)
shift = np.asarray(shift_mm, dtype=np.float64)
off = np.asarray(src_center_off_mm, dtype=np.float64)
matrix = D @ Rinv @ A_out
offset = D @ (Rinv @ (b_out - shift) - off) + np.asarray(src_center_idx, dtype=np.float64)
return matrix, offset
def apply_alignment(result: AlignmentResult, angle_idx: int, img: np.ndarray,
order: int = 0) -> np.ndarray:
"""Resample any already-computed 2D image for `angle_idx` (same shape as
that angle's raw (n_rows, n_frames)) onto the shared alignment canvas.
order=0 (nearest) avoids blending real data with zero-padding or with
masked-out (0-valued) CH1/velocity pixels at mask edges. Channel-
agnostic: the same per-angle transform (found from the CH4 image) works
for any channel's image of that angle."""
t = result.per_angle[angle_idx]
return scipy_ndimage.affine_transform(
img.astype(np.float32, copy=False), t.matrix, offset=t.offset,
output_shape=result.canvas_shape, order=order,
mode="constant", cval=0.0)
def block_mean_2d(img: np.ndarray, fy: int, fx: int) -> np.ndarray:
"""Block-mean by independent row/column factors. Independent factors matter
because the raw grid is strongly anisotropic (5 µm along x, 50 µm along y):
a single square factor would either alias along x or throw away rows."""
fy, fx = max(1, int(fy)), max(1, int(fx))
if fy == 1 and fx == 1:
return img
h, w = img.shape
h2, w2 = (h // fy) * fy, (w // fx) * fx
if h2 == 0 or w2 == 0:
return img
trimmed = img[:h2, :w2]
return trimmed.reshape(h2 // fy, fy, w2 // fx, fx).mean(axis=(1, 3))
# ---- Registration: rigid (rotation + translation) fit against the reference
#
# Everything below works on _RegImage, an angle's image resampled to a shared
# *isotropic* grid centered on its own array center. Nothing in here can see a
# stage coordinate even in principle, which is the point: the fit is decided by
# image content alone.
@dataclass
class _RegImage:
"""One angle's image prepared for registration: block-mean downsampled to
roughly the registration pitch, carrying the physical pitch it ended up
with and the local-mm offset of its own array center from the
full-resolution array center (block-mean trims a partial trailing block, so
the two centers can differ by up to half a block)."""
img: np.ndarray
dx_mm: float
dy_mm: float
center_off_mm: tuple[float, float]
def _block_center_off(n_full: int, n_small: int, factor: int,
pitch_mm: float) -> float:
"""Local-mm offset of a block-mean-downsampled array's own center from the
full-resolution array's center along one axis.
Small pixel k averages full pixels [k*f, k*f + f - 1], so its center sits
at full index k*f + (f-1)/2; block-mean also trims a partial trailing
block. Both effects together move the small array's center by up to half a
block, which has to be accounted for or a downsampled image registers (or
previews) at a systematically shifted position.
"""
return (((n_small - 1) / 2.0) * factor + (factor - 1) / 2.0
- (n_full - 1) / 2.0) * pitch_mm
def _prepare_reg_image(sras: SrasFile, angle_idx: int, img: np.ndarray,
pitch_mm: float) -> _RegImage:
"""Block-mean an angle's image down to roughly *pitch_mm* before it is
resampled onto the registration grid. Pre-averaging matters: the raw grid
is 10x finer along x than along y, so sampling it directly at the (much
coarser) isotropic registration pitch would alias badly along x."""
dx, dy = pixel_pitch_mm(sras, angle_idx)
fx = max(1, int(pitch_mm / abs(dx)))
fy = max(1, int(pitch_mm / abs(dy)))
small = block_mean_2d(np.asarray(img, dtype=np.float32), fy, fx)
n_rows, n_frames = img.shape
return _RegImage(
small, dx * fx, dy * fy,
(_block_center_off(n_frames, small.shape[1], fx, dx),
_block_center_off(n_rows, small.shape[0], fy, dy)))
def _embed(reg: _RegImage, pitch_mm: float, n: int, rotation_deg: float,
order: int) -> np.ndarray:
"""Resample a _RegImage onto the shared n x n isotropic registration grid,
rotated by *rotation_deg* about the grid center and with no translation
(translation is what phase correlation then measures)."""
half = (n - 1) / 2.0 * pitch_mm
matrix, offset = _affine_out_to_src(
out_pitch_mm=(pitch_mm, pitch_mm), out_origin_ref_mm=(-half, -half),
src_dx_mm=reg.dx_mm, src_dy_mm=reg.dy_mm,
src_center_idx=((reg.img.shape[0] - 1) / 2.0, (reg.img.shape[1] - 1) / 2.0),
src_center_off_mm=reg.center_off_mm, rotation_deg=rotation_deg)
return scipy_ndimage.affine_transform(
reg.img, matrix, offset=offset, output_shape=(n, n), order=order,
mode="constant", cval=0.0)
def _embed_with_valid(reg: _RegImage, pitch_mm: float, n: int,
rotation_deg: float) -> tuple[np.ndarray, np.ndarray]:
"""Embedded image plus the boolean mask of where that angle actually has
data. The valid mask is what lets registration ignore each angle's
differently-shaped scan window instead of locking onto its silhouette."""
img = _embed(reg, pitch_mm, n, rotation_deg, order=1)
ones = _RegImage(np.ones_like(reg.img), reg.dx_mm, reg.dy_mm, reg.center_off_mm)
valid = _embed(ones, pitch_mm, n, rotation_deg, order=0) > 0.5
return img, valid
def _shift_into(img: np.ndarray, dr: int, dc: int) -> np.ndarray:
"""img translated by whole pixels with zero fill (never wrapping, unlike
np.roll — wrapped content would score as a spurious match)."""
out = np.zeros_like(img)
h, w = img.shape
sr0, sr1 = max(0, dr), min(h, h + dr)
sc0, sc1 = max(0, dc), min(w, w + dc)
if sr0 >= sr1 or sc0 >= sc1:
return out
out[sr0:sr1, sc0:sc1] = img[sr0 - dr:sr1 - dr, sc0 - dc:sc1 - dc]
return out
def _overlap_ncc(ref: np.ndarray, ref_valid: np.ndarray,
mov: np.ndarray, mov_valid: np.ndarray,
min_overlap_frac: float = 0.15) -> float:
"""Zero-mean normalized cross-correlation over the two images' common valid
region — the score every rotation candidate is ranked by.
Computed on the overlap only, and rejected outright (-1) when the overlap
is too small a fraction of the smaller footprint: without that floor a
candidate that slides the angles almost entirely apart can win on a handful
of coincidentally-similar pixels.
"""
both = ref_valid & mov_valid
n = int(both.sum())
smaller = min(int(ref_valid.sum()), int(mov_valid.sum()))
if smaller == 0 or n < min_overlap_frac * smaller or n < 16:
return -1.0
a = ref[both].astype(np.float64)
b = mov[both].astype(np.float64)
a -= a.mean()
b -= b.mean()
denom = np.sqrt((a * a).sum() * (b * b).sum())
return float((a * b).sum() / denom) if denom > 0 else -1.0
def _masked_shift(ref: np.ndarray, ref_valid: np.ndarray,
mov: np.ndarray, mov_valid: np.ndarray) -> tuple[int, int]:
"""Integer (dr, dc) that best registers *mov* onto *ref*, from skimage's
masked FFT phase correlation (Padfield). The masked variant is the whole
reason scikit-image is a dependency: plain phase correlation on these
images locks onto the scan window's rectangular silhouette, which differs
per angle, instead of onto the sample."""
pcc = _skimage_phase_cross_correlation()
result = pcc(ref, mov, reference_mask=ref_valid, moving_mask=mov_valid)
shift = result[0] if isinstance(result, tuple) else result
return int(round(float(shift[0]))), int(round(float(shift[1])))
def _subpixel_residual(ref: np.ndarray, mov: np.ndarray,
both: np.ndarray) -> tuple[float, float]:
"""Sub-pixel leftover shift between two already integer-aligned images,
from upsampled phase correlation over their common valid region.
A separate pass because skimage's *masked* phase correlation has no
upsample_factor; here both images are zeroed outside the shared overlap and
mean-subtracted inside it, so the plain upsampled version is well posed.
Clamped to ±1 px: this only ever polishes an already-good integer fit, and
a larger "residual" means the peak was spurious.
normalization=None (plain cross-correlation, not phase correlation) is
load-bearing. Whitening the spectrum is what makes phase correlation good
at finding a large unknown shift, but here the two images are already
aligned to within a pixel and the masked-off surroundings put a hard edge
in both: whitened, that edge and the high-frequency noise swamp the true
sub-pixel peak and the default returns a flat zero every time.
"""
if not both.any():
return 0.0, 0.0
a = np.zeros_like(ref)
b = np.zeros_like(mov)
a[both] = ref[both] - ref[both].mean()
b[both] = mov[both] - mov[both].mean()
if not (np.any(a) and np.any(b)):
return 0.0, 0.0
pcc = _skimage_phase_cross_correlation()
result = pcc(a, b, upsample_factor=20, normalization=None)
shift = result[0] if isinstance(result, tuple) else result
dr, dc = float(shift[0]), float(shift[1])
if abs(dr) > 1.0 or abs(dc) > 1.0:
return 0.0, 0.0
return dr, dc
def _reg_pitch_and_size(sras: SrasFile, max_dim: int,
margin: float = 1.25) -> tuple[float, int]:
"""Isotropic pitch (mm/px) and side length for the shared registration
grid: square, big enough for the largest angle's footprint at any rotation
(hence its diagonal) plus *margin* headroom for the translation search.
The floor on pitch is the *geometric mean* of the two native pitches, not
the coarser of them. The raw grid is anisotropic (5 µm along x, 50 µm along
y): flooring at 50 µm would throw away all the extra x detail, and rotation
precision depends directly on it — a feature at radius r moves by r·δθ, so
at 50 µm a 20 mm-wide sample can only resolve rotation to a few tenths of a
degree. The geometric mean interpolates y up by ~3x rather than discarding
x, which costs a little memory and buys real angular precision. On a
full-size scan max_dim binds first and this floor never applies at all.
"""
diag = max(float(np.hypot(*(2 * v for v in _local_half_extent_mm(sras, a))))
for a in range(sras.n_angles))
span = diag * margin
native = float(np.sqrt(
abs(sras.pixel_x_mm)
* max(abs(pixel_pitch_mm(sras, a)[1]) for a in range(sras.n_angles))))
pitch = max(span / max_dim, native)
n = int(scipy_fft.next_fast_len(max(16, int(np.ceil(span / pitch)))))
return pitch, n
def _registration_workers(sras: SrasFile, fine_dim: int) -> int:
"""How many angles may register concurrently.
Not plan_angle_level: that budgets for waveform chunks, and registration
never touches a waveform — it works on already-computed DC images and a few
grid-sized arrays. The real limit is the masked phase correlation, which
pads to roughly twice the grid and holds several complex128 arrays of that
size live at once, so the count is derived from the same
_TOTAL_BYTES_BUDGET the rest of the module honours. The estimate below
comes out at 262 MB for the default fine_dim=640, against 199 MB measured —
deliberately on the pessimistic side, since overshooting the budget costs
swapping while undershooting only costs a little wall time.
"""
per_worker = 10 * (2 * fine_dim) ** 2 * 16 # ~10 complex128 grids
return int(max(1, min(_MAX_WORKERS, sras.n_angles,
_TOTAL_BYTES_BUDGET // max(1, per_worker))))
def registration_workers(sras: SrasFile) -> int:
"""Public: concurrent-registration cap at the default fine grid."""
return _registration_workers(sras, _DEFAULT_FINE_DIM)
def default_max_workers() -> int:
"""Public: the module-wide worker cap (SRAS_MAX_WORKERS or cpu count)."""
return _MAX_WORKERS
def _rotation_candidates(nominal_deg: float, search_deg: float,
step_deg: float) -> list[float]:
"""Coarse rotation candidates: a window around *both* signs of the stage's
reported angle change. Scoring both is what makes the stage's sign
convention a non-issue — the images decide which way the stage turns, and
a file whose stage reports the opposite sense registers just as well."""
out: list[float] = []
for center in (-nominal_deg, nominal_deg):
k = int(np.floor(search_deg / step_deg))
for i in range(-k, k + 1):
out.append(center + i * step_deg)
# Dedupe (the two windows coincide when nominal_deg is 0) while keeping order.
seen: set[float] = set()
return [t for t in out if not (round(t, 6) in seen or seen.add(round(t, 6)))]
def _score_rotation(ref_img: np.ndarray, ref_valid: np.ndarray,
mov: _RegImage, pitch: float, n: int, theta: float,
subpixel: bool = False) -> tuple[float, tuple[float, float]]:
"""Best score this rotation can reach, and the translation that reaches it:
rotate, phase-correlate for the shift, score the overlap.
*subpixel* also removes the leftover sub-pixel translation before scoring.
That matters more than it sounds: without it every candidate is scored at
whole-pixel alignment, so rotations that differ by less than one pixel of
rim displacement are ranked by quantization noise rather than by fit, and
the refinement stalls a degree or so off. Left off for the coarse sweep,
which only has to pick a basin, and on for the refinement.
"""
img, valid = _embed_with_valid(mov, pitch, n, theta)
dr, dc = _masked_shift(ref_img, ref_valid, img, valid)
shifted = _shift_into(img, dr, dc)
shifted_valid = _shift_into(valid.astype(np.float32), dr, dc) > 0.5
if subpixel:
sub_dr, sub_dc = _subpixel_residual(
ref_img, shifted, ref_valid & shifted_valid)
if sub_dr or sub_dc:
shifted = scipy_ndimage.shift(shifted, (sub_dr, sub_dc), order=1,
mode="constant", cval=0.0)
dr, dc = dr + sub_dr, dc + sub_dc
return (_overlap_ncc(ref_img, ref_valid, shifted, shifted_valid),
(float(dr), float(dc)))
def _refine_rotation(ref_img: np.ndarray, ref_valid: np.ndarray,
mov: _RegImage, pitch: float, n: int,
theta: float, score: float, shift: tuple[float, float],
step_deg: float, min_step_deg: float = 0.05,
max_evals: int = 80
) -> tuple[float, float, tuple[float, float]]:
"""Hill-climb the rotation from the coarse winner: step out while the score
improves, halve the step when it doesn't, stop below *min_step_deg*.
A walking search rather than a fixed grid around the coarse winner, because
the coarse stage ranks rotations at a coarse pitch where a degree can be
worth less than the translation quantization — its winner can legitimately
land a degree or two off, which a fixed ±½° refinement window could never
recover from.
Every candidate here is scored with subpixel=True, matching how the
incoming *score* was measured. Mixing the two is silently fatal: the
sub-pixel-corrected score is strictly the higher of the two, so a
subpixel-scored start compared against un-corrected candidates can never be
beaten and the search sits still at whatever the coarse stage handed it.
"""
evals = 0
while step_deg >= min_step_deg and evals < max_evals:
trials = []
for cand in (theta - step_deg, theta + step_deg):
s, sh = _score_rotation(ref_img, ref_valid, mov, pitch, n, cand,
subpixel=True)
evals += 1
trials.append((s, cand, sh))
best_s, best_cand, best_sh = max(trials, key=lambda t: t[0])
if best_s > score:
theta, score, shift = best_cand, best_s, best_sh
else:
step_deg /= 2.0
return theta, score, shift
def _source_images(sras: SrasFile, angle_idx: int, ref_angle_idx: int,
signal_mv: dict[int, np.ndarray], dc_threshold_mv: float,
sources) -> list[tuple[str, np.ndarray, np.ndarray]]:
"""(name, reference image, moving image) per requested registration source.
"signal" is each angle's own CH4 image minus its own minimum — subtracting
per-angle rather than globally keeps a nonzero DC baseline from reading as
a high-contrast edge against the zero padding. "mask" is the binarized
>= dc_threshold_mv image, the same silhouette the overlay draws. A mask
that is empty or completely full for either angle carries no registration
information at all, so that source is dropped rather than scored.
"""
out = []
for name in sources:
pair = []
for a in (ref_angle_idx, angle_idx):
img = signal_mv[a]
if name == "mask":
m = img >= dc_threshold_mv
if not m.any() or m.all():
pair = []
break
pair.append(m.astype(np.float32))
else:
pair.append((img - img.min()).astype(np.float32))
if pair:
out.append((name, pair[0], pair[1]))
return out
def register_angle_to_reference(
sras: SrasFile, angle_idx: int, ref_angle_idx: int,
signal_mv: dict[int, np.ndarray], *,
dc_threshold_mv: float = 0.0,
sources: tuple[str, ...] = ("signal", "mask"),
coarse_dim: int = 256, fine_dim: int = _DEFAULT_FINE_DIM,
search_deg: float = 6.0, coarse_step_deg: float = 2.0) -> RigidFit:
"""Rigid (rotation + translation, never scale) fit of *angle_idx* onto
*ref_angle_idx*, found entirely by cross-correlating image content.
Two stages:
1. Coarse sweep at *coarse_dim* over a ±*search_deg* window around both
signs of the stage's reported angle change (see _rotation_candidates),
for each requested source image, scored by _overlap_ncc. Only has to
pick the right basin.
2. Hill-climbing refinement of the winning (source, rotation) at
*fine_dim* with sub-pixel translation folded into every score
(_refine_rotation, _score_rotation), down to 0.05°.
The returned rotation_deg/shift_mm are the rigid map from this angle's
local mm to ref mm (q = R @ l + shift); score is the final NCC, which the
caller can surface so a bad scan is visible rather than silently fused in.
Returns identity for the reference angle itself.
"""
if angle_idx == ref_angle_idx:
return RigidFit(0.0, (0.0, 0.0), 1.0, "reference")
candidates = _source_images(sras, angle_idx, ref_angle_idx, signal_mv,
dc_threshold_mv, sources)
if not candidates:
return RigidFit(0.0, (0.0, 0.0), -1.0, "none")
nominal = nominal_delta_deg(sras, angle_idx, ref_angle_idx)
thetas = _rotation_candidates(nominal, search_deg, coarse_step_deg)
# ---- Stage 1: coarse sweep, every source ------------------------------
pitch_c, n_c = _reg_pitch_and_size(sras, coarse_dim)
best = (-2.0, 0.0, (0, 0), "none") # score, theta, (dr, dc), source
for name, ref_raw, mov_raw in candidates:
ref_reg = _prepare_reg_image(sras, ref_angle_idx, ref_raw, pitch_c)
mov_reg = _prepare_reg_image(sras, angle_idx, mov_raw, pitch_c)
ref_img, ref_valid = _embed_with_valid(ref_reg, pitch_c, n_c, 0.0)
for theta in thetas:
score, shift = _score_rotation(ref_img, ref_valid, mov_reg,
pitch_c, n_c, theta)
if score > best[0]:
best = (score, theta, shift, name)
if best[3] == "none":
return RigidFit(0.0, (0.0, 0.0), -1.0, "none")
# ---- Stage 2: refine the winner at full registration resolution -------
name = best[3]
ref_raw, mov_raw = next((r, m) for n_, r, m in candidates if n_ == name)
pitch_f, n_f = _reg_pitch_and_size(sras, fine_dim)
ref_reg = _prepare_reg_image(sras, ref_angle_idx, ref_raw, pitch_f)
mov_reg = _prepare_reg_image(sras, angle_idx, mov_raw, pitch_f)
ref_img, ref_valid = _embed_with_valid(ref_reg, pitch_f, n_f, 0.0)
theta = best[1]
score, shift = _score_rotation(ref_img, ref_valid, mov_reg, pitch_f, n_f,
theta, subpixel=True)
theta, score, shift = _refine_rotation(
ref_img, ref_valid, mov_reg, pitch_f, n_f, theta, score, shift,
step_deg=coarse_step_deg)
dr, dc = shift
return RigidFit(float(theta), (float(dc * pitch_f), float(dr * pitch_f)),
float(score), name)
# ---- Shared canvas: angle 0's own pixel grid, extended --------------------
def canvas_for_params(sras: SrasFile, ref_angle_idx: int,
pitch_mm: tuple[float, float],
per_angle_params: dict[int, ManualAngleParams],
*, margin_frac: float = 0.0, snap: bool = True
) -> tuple[tuple[float, float], tuple[int, int]]:
"""Shared-canvas origin (stage mm) and (n_rows, n_cols) at *pitch_mm* that
contains every angle's footprint after its own rigid transform. Angles
missing from per_angle_params default to identity (e.g. a sidecar saved
before a rescan added more angles).
snap=True aligns the canvas grid with the reference angle's own pixel grid,
so the reference lands on integer canvas pixels and is resampled by an
exact integer translation — the concrete meaning of "the canvas carries
angle 0's X/Y coordinates". It requires pitch_mm to be the reference's own
pitch; the manual-alignment preview passes a coarser pitch and snap=False.
margin_frac pads the box on every side: 0 for a final canvas, nonzero for
ManualAlignmentDialog's preview canvas, which needs headroom so an ordinary
translation nudge never has to trigger a full canvas resize (an extreme
nudge can still push content past this padding; accepted, and cheap to
recover from by re-opening the dialog).
"""
dx, dy = pitch_mm
corners = np.vstack([
_footprint_corners_ref_mm(
sras, a,
per_angle_params.get(a, ManualAngleParams()).rotation_deg,
per_angle_params.get(a, ManualAngleParams()).shift_mm)
for a in range(sras.n_angles)])
x_min, y_min = corners.min(axis=0)
x_max, y_max = corners.max(axis=0)
if margin_frac:
pad_x, pad_y = (x_max - x_min) * margin_frac, (y_max - y_min) * margin_frac
x_min, x_max = x_min - pad_x, x_max + pad_x
y_min, y_max = y_min - pad_y, y_max + pad_y
center = ref_center_mm(sras, ref_angle_idx)
if snap:
# Express the box in the reference's own pixel indices and grow it
# outward to whole pixels, so canvas index k lands exactly where the
# reference's own pixel (k + const) does.
cy, cx = _center_idx(sras, ref_angle_idx)
cols = sorted((x_min / dx + cx, x_max / dx + cx))
rows = sorted((y_min / dy + cy, y_max / dy + cy))
col0, col1 = int(np.floor(cols[0])), int(np.ceil(cols[1]))
row0, row1 = int(np.floor(rows[0])), int(np.ceil(rows[1]))
origin_ref = np.array([(col0 - cx) * dx, (row0 - cy) * dy])
shape = (row1 - row0 + 1, col1 - col0 + 1)
else:
origin_ref = np.array([x_min, y_min if dy > 0 else y_max])
shape = (int(np.ceil((y_max - y_min) / abs(dy))) + 1,
int(np.ceil((x_max - x_min) / dx)) + 1)
origin_stage = origin_ref + center
return (float(origin_stage[0]), float(origin_stage[1])), shape
def build_canvas_affine(sras: SrasFile, angle_idx: int, ref_angle_idx: int,
rotation_deg: float, shift_mm: tuple[float, float],
pitch_mm: tuple[float, float],
canvas_origin_mm: tuple[float, float],
*, src_downsample: tuple[int, int] = (1, 1)
) -> tuple[np.ndarray, np.ndarray]:
"""canvas index -> this angle's raw index, for a canvas whose origin is
given in *stage* mm (the reference's frame). *src_downsample* is the
(rows, cols) block-mean factor already applied to the image the caller will
resample — 1:1 for the raw image, coarser for the manual-alignment
preview's downsampled masks."""
dx_a, dy_a = pixel_pitch_mm(sras, angle_idx)
n_rows, n_frames = sras.image_shape(angle_idx)
fy, fx = (max(1, int(v)) for v in src_downsample)
if (fy, fx) != (1, 1):
# Same block-mean bookkeeping _prepare_reg_image does: the downsampled
# array's own center can sit up to half a block off the full-resolution
# center, and that offset has to be undone here or every preview layer
# lands slightly (and inconsistently) off.
nr_s, nf_s = n_rows // fy, n_frames // fx
src_dx, src_dy = dx_a * fx, dy_a * fy
src_center = ((nr_s - 1) / 2.0, (nf_s - 1) / 2.0)
src_off = (_block_center_off(n_frames, nf_s, fx, dx_a),
_block_center_off(n_rows, nr_s, fy, dy_a))
else:
src_dx, src_dy = dx_a, dy_a
src_center = _center_idx(sras, angle_idx)
src_off = (0.0, 0.0)
origin_ref = np.asarray(canvas_origin_mm, dtype=np.float64) \
- ref_center_mm(sras, ref_angle_idx)
return _affine_out_to_src(
out_pitch_mm=pitch_mm, out_origin_ref_mm=origin_ref,
src_dx_mm=src_dx, src_dy_mm=src_dy, src_center_idx=src_center,
src_center_off_mm=src_off, rotation_deg=rotation_deg, shift_mm=shift_mm)
def _result_from_params(sras: SrasFile, ref_angle_idx: int,
dc_threshold_mv: float,
params: dict[int, ManualAngleParams],
extra: dict[int, tuple[float, str]] | None = None
) -> AlignmentResult:
"""Assemble the final AlignmentResult from per-angle rigid parameters: pick
the shared canvas, then build each angle's canvas->raw affine. Pure matrix
and bbox math, so it is cheap enough to call synchronously on the GUI
thread on every manual edit."""
pitch = pixel_pitch_mm(sras, ref_angle_idx)
canvas_origin_mm, canvas_shape = canvas_for_params(
sras, ref_angle_idx, pitch, params, snap=True)
extra = extra or {}
per_angle: dict[int, AngleTransform] = {}
for a in range(sras.n_angles):
p = params.get(a, ManualAngleParams())
matrix, offset = build_canvas_affine(
sras, a, ref_angle_idx, p.rotation_deg, p.shift_mm,
pitch, canvas_origin_mm)
score, source = extra.get(a, (1.0, ""))
per_angle[a] = AngleTransform(p.rotation_deg, p.shift_mm, matrix, offset,
score, source)
return AlignmentResult(ref_angle_idx, dc_threshold_mv, canvas_shape,
pitch[0], pitch[1], canvas_origin_mm, per_angle)
def _parallel_map(fn, items, n_workers: int) -> list:
"""fn over items, in order, threaded when it pays."""
items = list(items)
if n_workers <= 1 or len(items) <= 1:
return [fn(x) for x in items]
with ThreadPoolExecutor(max_workers=min(n_workers, len(items))) as pool:
return list(pool.map(fn, items))
def compute_angle_alignment(sras: SrasFile, ref_angle_idx: int,
dc_threshold_mv: float, progress_cb=None,
fine_dim: int = _DEFAULT_FINE_DIM) -> AlignmentResult:
"""Top-level alignment driver: register every angle onto *ref_angle_idx* by
content, then lay them all out on that angle's own coordinate grid.
Runs on a background thread (see AngleAlignmentWorker) — deliberately
recomputes CH4 DC images from scratch rather than reading the GUI-thread
_dc_cache dict, since background-thread workers must not touch
GUI-thread-owned caches.
"""
n = sras.n_angles # already the *complete*-angle count for aborted v6 scans
# Parallel over angles, serial within each — see plan_angle_level.
n_workers, angle_budget = plan_angle_level(sras)
# progress_cb fires from pool threads, so the counter behind it must be
# atomic. list.append is, and len() of a list is a consistent read.
_ticks: list[int] = []
def tick(base: int, span: int):
if progress_cb:
_ticks.append(1)
progress_cb(base + int(min(len(_ticks), n) / n * span))
# ---- Step 1: CH4 DC image per angle, native grid ----------------------
def dc4_for(a: int) -> np.ndarray:
dc4 = adc_to_mv(
compute_dc_image(sras, a, CH4_IDX, max_workers=1, budget=angle_budget),
*sras.cal(CH4_IDX))
tick(0, 25)
return dc4
dc4_mv = dict(enumerate(_parallel_map(dc4_for, range(n), n_workers)))
# ---- Step 2: rigid registration of every angle against the reference --
# Its own worker count: registration is bounded by grid-sized FFT buffers,
# not by the waveform chunking plan_angle_level budgets for.
_ticks.clear()
def fit_for(a: int) -> RigidFit:
fit = register_angle_to_reference(
sras, a, ref_angle_idx, dc4_mv, dc_threshold_mv=dc_threshold_mv,
fine_dim=fine_dim)
tick(25, 65)
return fit
fits = dict(enumerate(_parallel_map(
fit_for, range(n), _registration_workers(sras, fine_dim))))
# ---- Step 3/4: shared canvas on the reference's grid, per-angle affines
params = {a: ManualAngleParams(f.rotation_deg, f.shift_mm) for a, f in fits.items()}
extra = {a: (f.score, f.source) for a, f in fits.items()}
result = _result_from_params(sras, ref_angle_idx, dc_threshold_mv, params, extra)
if progress_cb:
progress_cb(100)
return result
# ---------------------------------------------------------------------------
# Manual alignment (Fusion menu -> Manual Alignment... dialog)
#
# Skips register_angle_to_reference's search entirely: every angle's
# rotation_deg/shift_mm is supplied directly by the caller (nudged by eye
# against a live multi-angle mask overlay, or pre-seeded from a registration
# run or a saved sidecar). Building the final AlignmentResult from already-known
# per-angle parameters is pure closed-form matrix math (_result_from_params)
# with no per-pixel image work at all, so build_manual_alignment is cheap enough
# to call synchronously on the GUI thread on every edit. The only genuinely
# expensive per-pixel operation anywhere in this flow is reproject_mask, and
# only ManualAlignmentDialog's own downsampled preview calls that per keystroke
# — see that class's docstring for how it limits each nudge to reprojecting only
# the actively-edited angle.
# ---------------------------------------------------------------------------
def reproject_mask(sras: SrasFile, angle_idx: int, ref_angle_idx: int,
mask: np.ndarray, rotation_deg: float,
shift_mm: tuple[float, float],
canvas_pitch_mm: tuple[float, float],
canvas_origin_mm: tuple[float, float],
canvas_shape: tuple[int, int],
*, src_downsample: tuple[int, int] = (1, 1)) -> np.ndarray:
"""Resample one angle's binary/float mask onto an arbitrary canvas via an
explicit rotation+shift — the single building block ManualAlignmentDialog's
live preview repeatedly calls (once per keystroke, for only the
actively-nudged angle). *src_downsample* must match the (rows, cols)
block-mean factor already applied to *mask*, or the reprojection lands at
the wrong scale. order=0 (nearest) matches apply_alignment's own reasoning:
a binary mask must never be blended with zero-padding."""
matrix, offset = build_canvas_affine(
sras, angle_idx, ref_angle_idx, rotation_deg, shift_mm,
canvas_pitch_mm, canvas_origin_mm, src_downsample=src_downsample)
return scipy_ndimage.affine_transform(
mask.astype(np.float32, copy=False), matrix, offset=offset,
output_shape=canvas_shape, order=0, mode="constant", cval=0.0)
def build_manual_alignment(sras: SrasFile, ref_angle_idx: int,
dc_threshold_mv: float,
per_angle_params: dict[int, ManualAngleParams]
) -> AlignmentResult:
"""Build a full, full-resolution AlignmentResult from user-supplied
per-angle rotation+shift — the Manual Alignment counterpart to
compute_angle_alignment, skipping its registration search entirely (every
angle's transform here is exactly what the caller supplied). The reference
angle's params are always forced to identity, regardless of what
per_angle_params holds for it — it defines the shared origin and must never
be transformed.
dc_threshold_mv plays no part in the geometry; it's stored on the returned
AlignmentResult purely as a record of the RF-mask threshold in effect at
the time.
"""
params = {a: per_angle_params.get(a, ManualAngleParams())
for a in range(sras.n_angles)}
params[ref_angle_idx] = ManualAngleParams()
return _result_from_params(sras, ref_angle_idx, dc_threshold_mv, params)
# ---- Sidecar persistence (<name>.sras.align.json) -------------------------
# A viewer-computed derived artifact, so it lives with the alignment math
# rather than in sras_format (see docs/design.md, "Manual-alignment sidecar").
@dataclass
class ManualAlignmentSidecar:
ref_angle_idx: int
dc_threshold_mv: float
per_angle: dict[int, ManualAngleParams]
def sidecar_path(sras_path) -> Path:
"""<name>.sras.align.json next to the scan file. A thin, independently
testable function since save/load/delete and the GUI's status messages
all need the identical path."""
p = Path(sras_path)
return p.with_name(p.name + ".align.json")
# Bumped whenever the frame the stored numbers are measured in changes; older
# sidecars are treated as absent, never migrated. Bump history:
# docs/design.md ("Schema history").
_SIDECAR_SCHEMA_VERSION = 3
def save_manual_alignment(sras: SrasFile, ref_angle_idx: int,
dc_threshold_mv: float,
per_angle: dict[int, ManualAngleParams]) -> Path:
"""Write the sidecar JSON for sras.path (overwriting any existing one)
and return the path written. Angle indices become JSON object keys, so
they round-trip as strings — load_manual_alignment converts them back."""
path = sidecar_path(sras.path)
payload = {
"schema_version": _SIDECAR_SCHEMA_VERSION,
"ref_angle_idx": ref_angle_idx,
"dc_threshold_mv": dc_threshold_mv,
"per_angle": {
str(a): {"rotation_deg": p.rotation_deg, "shift_mm": list(p.shift_mm)}
for a, p in per_angle.items()
},
}
path.write_text(json.dumps(payload, indent=2))
return path
def load_manual_alignment(sras: SrasFile) -> ManualAlignmentSidecar | None:
"""Read <sras.path>'s sidecar JSON if present, else None — never raises:
a missing, corrupt, foreign, or version-mismatched JSON file must not
block opening the .sras file itself (see SrasViewerWindow._on_load_done).
Per-angle entries for an angle index no longer present in *sras* (e.g.
re-scanned with fewer angles) are silently dropped.
"""
path = sidecar_path(sras.path)
if not path.exists():
return None
try:
raw = json.loads(path.read_text())
if raw.get("schema_version") != _SIDECAR_SCHEMA_VERSION:
return None
per_angle = {
int(a): ManualAngleParams(
float(v["rotation_deg"]),
(float(v["shift_mm"][0]), float(v["shift_mm"][1])))
for a, v in raw.get("per_angle", {}).items()
if int(a) < sras.n_angles
}
return ManualAlignmentSidecar(
ref_angle_idx=int(raw.get("ref_angle_idx", 0)),
dc_threshold_mv=float(raw.get("dc_threshold_mv", 0.0)),
per_angle=per_angle)
except (OSError, ValueError, KeyError, TypeError, IndexError,
json.JSONDecodeError):
return None
def delete_manual_alignment(sras: SrasFile) -> bool:
"""Delete the sidecar if present. Returns whether a file actually existed
to delete, so Clear Alignment's status message can say so. Genuine I/O
errors (permission denied, read-only share) propagate — the caller
(ManualAlignmentDialog._on_clear) surfaces them rather than silently
pretending the destructive action succeeded."""
path = sidecar_path(sras.path)
try:
path.unlink()
return True
except FileNotFoundError:
return False