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leonarski_fandClaude Opus 5 a27c4cf26f reader: take a miniCBF's mounting from the imgCIF axis table its header states
A miniCBF header states three things about how the instrument is put together
that the reader was assuming instead: which laboratory direction the image's
columns run along, which its rows run along, and which the spindle turns about.
Some beamlines append a CBF template block holding the full imgCIF axis table,
which says all three outright.

Two instruments in the corpus are not what was assumed, in two different ways.
One mounts its detector a quarter turn round, so the image's columns run
vertically. Another turns its spindle about the VERTICAL, with the image mounted
the usual way; its table says so, and its "# Oscillation_axis" line says so a
second way, by naming the image direction the spindle runs along rather than a
vector. Either error leaves the spindle 90 degrees from the image. That is not a
sign, so the run's axis-sign rescue cannot reach it, and no refinement recovers
it: all three affected sweeps indexed nothing usable.

So the table is read. The element axes give the image orientation, matched against
the eight discrete mountings exactly as the NXmx module directions already are -
the match itself moves to DetectorOrientation, so both readers share one
definition rather than two copies. The goniometer axis with no parent gives the
spindle DIRECTION; its sign stays the rescue's business, which is the part a
convention can legitimately differ on. The detector axis with no parent gives the
2theta arm, replacing the assumption that the arm shares the spindle's axis - the
one header stating both states them with the same vector, so this changes no
answer, only what it rests on. imgCIF's frame differs from the internal one by a
half turn about x, a rotation and not a mirror, as writer/HDF5NXmx.cpp already
records from the other side.

Where a header carries no table, a "+SLOW" on the Oscillation_axis line still
says the spindle runs along the image's slow direction. That is the only thing one
of the three affected sets says about it. The axis NAME on that line stays
unusable - the header that carries both says "X.CW" where its own table says Y -
but the direction token is not: where both are present they agree, which is what
makes reading it evidence rather than a guess.

Also: naming a frame with no directory at all now finds its sweep. parent_path()
of a bare filename is empty and iterating an empty path finds nothing, so running
from inside the data directory reported that no images were found.

Measured, with nothing on the command line. The vertical-spindle protein set goes
from no usable lattice to 100% indexed, P 6(3) 2 2 with a cell 0.43% from
deposited, 87846 reflections at 86.3% completeness and CC(1/2) 0.995. Its
companion from the same detector, which has no table and only the +SLOW token,
goes from a spurious monoclinic cell at 2.3% completeness and I/sigma 0.21 to the
right orthorhombic lattice, 97.7% indexed, 59.7% complete, CC(1/2) 0.996. The
quarter-turned set's three sweeps, at three arm positions, now all index without
the hand-passed quarter turn they needed and agree on one cell to 0.03 A. Six
miniCBF sets that state no table and no +SLOW - including one whose
Oscillation_axis line names an axis in a third dialect - are byte-identical in
.hkl, .mtz, .cif and the image statistics, as are two NXmx sets, which is the
shared orientation matcher moving nothing on that path either.

Co-Authored-By: Claude Opus 5 (1M context) <noreply@anthropic.com>
Claude-Session: https://claude.ai/code/session_01T3yNBXk4wKdMZy1ak2NY7f
2026-08-30 14:03:32 +02:00
leonarski_fandClaude Opus 5 fed077e683 geometry: hold the detector plane as axis vectors, and give the discrete part its own home
The detector plane was three PONI angles and nothing else, so the two things it
cannot express - an image mirrored in Y, and one mounted at a multiple of 90
degrees - had no home at all. They are now the DetectorOrientation carried by the
detector setup, composed with the PONI rotation into one orthogonal matrix whose
columns ARE the fast axis, the slow axis and the sample->PONI normal:

    lab = R(rot1, rot2, rot3) * Delta * ( (x-bx)*p , (y-by)*p , distance )

GetFastAxis/GetSlowAxis/GetNormalAxis read those columns and DetectorAxes() sets
the plane from them, decomposing back to the angles; PoniRotMatrix and
PoniAnglesFromMatrix are the conversion in both directions, exact on the canonical
branch (rot2 in [-pi/2, pi/2]) and with a stated convention at gimbal lock. The
angles stay stored rather than re-derived, so a geometry given as angles is
written back as the same angles, to the bit.

Delta is never inferred. In particular an arbitrary rot3 is NOT decomposed into a
quarter turn plus a residual: rot3 is a fitted quantity, and a least-squares step
must not be able to turn the stored image. It is set only where something states
it - the detector setup, --detector-mirror-y / --detector-quarter-turns, or the
value a file this system wrote records - and defaults to the identity, which makes
the whole change a no-op for every existing detector and every existing file.

It is a different setting from DetectorSetup::mirror_y, which flips the MODULE
LAYOUT while an image is assembled and so decides what the stored pixels are.
Merging the two would apply the mirror twice for every modular detector, or change
the pixel content of every file written; both are ruled out. The new one earns its
keep exactly where the old one is a no-op: a detector whose image arrives already
assembled has no layout to flip.

Both generators are signed permutations of the in-plane offset, so they preserve
the distance from the PONI. That is why almost nothing downstream changes:
everything needing an azimuth already goes through LabCoord, and everything that
does not needs only a radius. The two hand-written copies of the rotation -
XtalResidual and RingOptimizer - take the discrete part as four constants next to
cos_rot3/sin_rot3, since it acts in the detector frame where rot3 acts in the
laboratory and cannot be folded into it. RingOptimizer needs it despite being a
radial fit: it fits the tilt, and the discrete part changes which way the tilt
tips a ring.

Carried as two optional CBOR keys and two detectorSpecific datasets, both
back-compatible; the NXmx module axis vectors and the translation direction stop
being hardcoded and are computed from it, reproducing today's values exactly at
the identity. GetPoniRotMatrix is renamed GetDetectorMatrix, because it is no
longer only the PONI rotation.

Co-Authored-By: Claude Opus 5 (1M context) <noreply@anthropic.com>
Claude-Session: https://claude.ai/code/session_01Lc5JG6kJqZoCWaoZ43JGTW
2026-08-29 23:00:35 +02:00