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scanengine-3/core/saw_check.py
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"""Middle-row SAW quality check: acquire one row per angle, then read the
alignment off the frequencies it produces.
Two halves of one test mode, kept together because neither is much use
without the other:
*Acquisition* — ``middle_row_plan`` reduces a full ScanPlan to a single row
per angle, the row-wise middle of the ROI. ScanEngine runs the result
exactly like any other scan and writes it as a v11 .sras file
(``sras_format.VERSION_SAW_CHECK``), so a check costs one row-time per angle
instead of the hours a full multi-angle scan takes.
*Analysis* — ``frequency_traces`` turns such a file back into one peak-SAW-
frequency trace per angle, and ``alignment_summary`` reduces those to the
numbers the operator is actually asking about. Both are Qt-free; the plotting
lives in saw_check_viewer.py.
Why the middle row answers an alignment question: ``scan_geometry.build_plan``
centres every angle's rotated bounding box on the same nominal ROI centre, so
each angle's middle row crosses that one point on the sample. Every angle
therefore measures the same material, and a spread in the per-angle
frequencies is a property of the rig (or of a genuinely anisotropic sample),
not of where each row happened to land.
"""
from __future__ import annotations
from dataclasses import dataclass, field, replace
import numpy as np
from core.scan_geometry import ScanGeometryError, ScanPlan
from core.sras_analysis import ChannelCalibration, compute_rf_image
from core.sras_format import SrasFile
# Rules of thumb for the read-out, not physics. A well-aligned rig on an
# isotropic sample reads the same frequency at every angle, so the spread of
# the per-angle medians is the alignment signal — but an anisotropic sample
# genuinely varies with angle, so a wide spread is a prompt to look at the
# curves, never a verdict on its own.
SPREAD_GOOD_PCT = 1.0
SPREAD_MARGINAL_PCT = 3.0
# Below this fraction of unmasked pixels a trace is too sparse to read.
VALID_FRACTION_FLOOR = 0.5
# ── Acquisition side ─────────────────────────────────────────────────────────
def middle_row_plan(plan: ScanPlan) -> ScanPlan:
"""Reduce a scan plan to its row-wise middle row at every angle.
Each angle keeps the geometry the full scan would have used — same
x_start, x_delta and n_frames from its own rotated bounding box — and
scans only the middle entry of its row list, so the check samples exactly
what the scan would along that row.
An even row count has no exact middle; the upper of the two central rows
is taken (``n_rows // 2``), which is also the row the viewer picks when it
reads the middle row out of a full scan.
"""
if plan.n_angles == 0:
raise ScanGeometryError("Cannot build a SAW check from a plan with no angles")
per_angle = []
for pa in plan.per_angle:
if not pa.y_positions:
raise ScanGeometryError(
f"Angle {pa.angle_deg:.1f}° has no rows, so it has no middle row to check"
)
per_angle.append(replace(pa, n_rows=1,
y_positions=[pa.y_positions[middle_row_index(pa.n_rows)]]))
return replace(plan, per_angle=per_angle)
def middle_row_index(n_rows: int) -> int:
"""The row this check calls the middle one. One rule, two callers."""
return max(0, n_rows // 2)
# ── Analysis side ────────────────────────────────────────────────────────────
@dataclass
class AngleTrace:
"""One angle's peak SAW frequency along its middle row.
``freq_mhz`` is NaN wherever the pixel was masked out (CH4 DC below the
threshold), so the gaps stay gaps instead of reading as 0 MHz.
"""
angle_idx: int
angle_deg: float
row_idx: int
y_mm: float
x_mm: np.ndarray # absolute stage X of each frame
freq_mhz: np.ndarray # NaN where masked
_valid: np.ndarray = field(init=False, repr=False)
def __post_init__(self):
self._valid = np.isfinite(self.freq_mhz)
@property
def offset_mm(self) -> np.ndarray:
"""X relative to the centre of this row.
Every angle's row is centred on the same ROI centre, so plotting
against this puts all the angles' curves over the same piece of
sample — which is the whole point of the comparison.
"""
if len(self.x_mm) == 0:
return self.x_mm
return self.x_mm - 0.5 * (self.x_mm[0] + self.x_mm[-1])
@property
def n_valid(self) -> int:
return int(self._valid.sum())
@property
def valid_fraction(self) -> float:
return self.n_valid / len(self.freq_mhz) if len(self.freq_mhz) else 0.0
@property
def median_mhz(self) -> float:
return float(np.median(self.freq_mhz[self._valid])) if self.n_valid else float("nan")
@property
def std_mhz(self) -> float:
return float(np.std(self.freq_mhz[self._valid])) if self.n_valid > 1 else float("nan")
@property
def drift_mhz_per_mm(self) -> float:
"""Least-squares slope of frequency along the row.
A flat trace means the response did not change across the ROI; a
sloped one is the signature of a tilt or a defocus the angle spread
alone would not show.
"""
if self.n_valid < 2:
return float("nan")
x = self.offset_mm[self._valid]
if np.ptp(x) == 0:
return float("nan")
return float(np.polyfit(x, self.freq_mhz[self._valid], 1)[0])
@dataclass
class AlignmentSummary:
"""What the per-angle traces say about the alignment, in scalars."""
n_angles: int
median_mhz: float
spread_mhz: float # max − min of the per-angle medians
spread_pct: float # that spread as a % of the overall median
best_angle_deg: float # angle reading the highest median
worst_angle_deg: float # angle reading the lowest median
worst_drift_mhz_per_mm: float
worst_drift_angle_deg: float
min_valid_fraction: float
@property
def level(self) -> str:
""""good" / "marginal" / "poor" — see the module's threshold note."""
if self.n_angles == 0 or not np.isfinite(self.spread_pct):
return "poor"
if self.min_valid_fraction < VALID_FRACTION_FLOOR:
return "poor"
if self.spread_pct <= SPREAD_GOOD_PCT:
return "good"
if self.spread_pct <= SPREAD_MARGINAL_PCT:
return "marginal"
return "poor"
def describe(self) -> str:
if self.n_angles == 0:
return "No angle produced a usable frequency trace."
if self.min_valid_fraction < VALID_FRACTION_FLOOR:
return (f"Only {self.min_valid_fraction * 100:.0f} % of the worst angle's row "
f"is above the DC threshold — check the detection beam and the "
f"threshold before reading the spread.")
return (f"Per-angle medians span {self.spread_mhz:.3f} MHz "
f"({self.spread_pct:.2f} % of {self.median_mhz:.3f} MHz), "
f"lowest at {self.worst_angle_deg:.1f}°, highest at {self.best_angle_deg:.1f}°. "
f"Largest drift along a row: {self.worst_drift_mhz_per_mm:+.3f} MHz/mm "
f"at {self.worst_drift_angle_deg:.1f}°.")
def frequency_traces(sras: SrasFile, *, dc_threshold_mv: float = 0.0,
subtract_background: bool = False,
gate_start_ns: float | None = None,
gate_end_ns: float | None = None,
calib: ChannelCalibration | None = None,
on_progress=lambda done, total: None) -> list[AngleTrace]:
"""Peak SAW frequency along the middle row of every angle in ``sras``.
Works on a v11 check (one row per angle, so the middle row is the only
row) and on a full scan alike — the same middle row the check would
have acquired is pulled out of the scan, which is what lets a finished
scan be re-examined with the check's own read-out.
``subtract_background`` takes each angle's own background out of its
frames (v6/v10 files have only the one, which every angle then shares).
Doing it per angle is the point of the per-angle capture: comparing
angles is exactly what this read-out is for, so they must not be
referenced against one background taken at whichever angle came first.
Angles with nothing on disk (an aborted file) are skipped rather than
reported as flat zero.
"""
calib = calib if calib is not None else ChannelCalibration.from_preambles(sras.preambles)
freq_axis = sras.freq_axis_mhz(sras.header.samples_per_frame)
time_axis = sras.time_axis_ns()
statuses = sras.angle_status()
traces: list[AngleTrace] = []
for st in statuses:
on_progress(st.index, len(statuses))
if st.n_rows_available < 1:
continue
pa = sras.per_angle[st.index]
row = middle_row_index(st.n_rows_available)
view = sras.load_angle(st.index, n_rows=st.n_rows_available)[row:row + 1]
background = sras.background_array(st.index) if subtract_background else None
img = compute_rf_image(view, calib, freq_axis, dc_threshold_mv,
background=background,
gate_start_ns=gate_start_ns, gate_end_ns=gate_end_ns,
time_axis_ns=time_axis)
# compute_rf_image zeroes masked pixels and its FFT never peaks in the
# suppressed DC bin, so 0 MHz means "no reading" and nothing else.
freq = img[0].astype(np.float64)
freq[freq <= 0.0] = np.nan
traces.append(AngleTrace(
angle_idx=st.index, angle_deg=pa.angle_deg, row_idx=row,
y_mm=pa.y_positions[row] if row < len(pa.y_positions) else float("nan"),
x_mm=sras.x_axis_mm(st.index), freq_mhz=freq,
))
on_progress(len(statuses), len(statuses))
return traces
def alignment_summary(traces: list[AngleTrace]) -> AlignmentSummary:
"""Reduce per-angle traces to the alignment read-out."""
usable = [t for t in traces if t.n_valid > 0]
if not usable:
nan = float("nan")
return AlignmentSummary(0, nan, nan, nan, nan, nan, nan, nan, 0.0)
medians = np.array([t.median_mhz for t in usable])
overall = float(np.median(medians))
spread = float(medians.max() - medians.min())
drifts = [(abs(t.drift_mhz_per_mm), t) for t in usable
if np.isfinite(t.drift_mhz_per_mm)]
worst_drift = max(drifts, key=lambda d: d[0])[1] if drifts else None
return AlignmentSummary(
n_angles=len(usable),
median_mhz=overall,
spread_mhz=spread,
spread_pct=spread / overall * 100.0 if overall else float("nan"),
best_angle_deg=usable[int(np.argmax(medians))].angle_deg,
worst_angle_deg=usable[int(np.argmin(medians))].angle_deg,
worst_drift_mhz_per_mm=worst_drift.drift_mhz_per_mm if worst_drift else float("nan"),
worst_drift_angle_deg=worst_drift.angle_deg if worst_drift else float("nan"),
min_valid_fraction=min(t.valid_fraction for t in usable),
)