grid scan: say how the stationary spindle angle is stated, and pin it
A grid scan is a set of stills at a stationary spindle, and the angle it stood at is what relates one grid to another taken elsewhere on the circle. Users were finding an all-zero omega in the file and concluding the angle could not be recorded at all. It already can, and has since the goniometer and the grid scan stopped being alternatives: send the axis with step 0 and its start angle, and that angle is written per image into the NXmx sample chain, read back by reader/, and taken by dials.import as a set of stills. Measured on a generated 12-image grid: the placeholder file carries omega = 0 x 12, the same file with the axis sent at step 0 carries omega = 90 x 12, and dials.import reports "still: 1, sweep: 0" for both. Nothing in the code needed changing, so nothing was; what was missing was that nobody could tell, and that no test held the behaviour down. So: the API and the HDF5 documentation now say it in as many words, and three tests pin the three legs the value crosses - the OpenAPI request (which used to drop the grid scan whenever an axis was present, unpinned until now), the CBOR start message, and the file round trip. Also corrects a claim two comments and the HDF5 page were making. NXmx can express "no rotation" perfectly well - a sample may depend_on "." - so the placeholder is not there for the standard's sake. It is there because dxtbx cannot read a sample chain of translations alone: strip the rotation axis from a grid scan master and dials.import dies in get_dxtbx_goniometer with a matmul dimension mismatch. Recorded so nobody removes the placeholder on the strength of the standard. One thing the change does not fix, because it cannot: a stationary angle is invisible to DIALS when a grid scan is present. dxtbx picks the first varying axis as the scan axis, which is a grid translation, so the oscillation reads (0, 0); and with exactly one rotation axis in the chain it builds a single-axis goniometer whose fixed rotation is the identity, never consulting the angle. The same angle IS visible when it is the only candidate (oscillation reads (90, 0)) or when a Smargon head puts a second rotation axis in the chain (the setting rotation then carries it). The value is in the file and correct either way.
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# GridScan
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Definition of a grid scan. May be combined with a goniometer axis: a grid is often collected at a particular head position, and a stationary axis records where that was.
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Definition of a grid scan. Combine it with a goniometer axis to state the angle the spindle stood at: send `goniometer` with `step` 0 and the `start` angle of the grid scan, and that angle is written per image into the NXmx sample transformation chain. Without one the spindle is recorded at 0, which says that nobody stated an angle rather than that the spindle stood at 0.
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## Properties
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@@ -7,7 +7,7 @@ Definition of a crystal rotation axis
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Name | Type | Description | Notes
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------------ | ------------- | ------------- | -------------
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**name** | **str** | Name of rotation axis (e.g., omega, phi) | [optional] [default to 'omega']
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**step** | **float** | Angle step (per image) in degrees |
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**step** | **float** | Angle step (per image) in degrees. 0 for an axis that does not turn: the axis then records the angle the spindle stood at, which is how a grid scan or a set of stills states its head position. |
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**start** | **float** | Start angle in degrees | [optional] [default to 0]
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**vector** | **List[float]** | Rotation axis |
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**helical_step_um** | **List[float]** | Translation (per image) for helical scan | [optional]
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