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Candidate cell filtering called acos three times per candidate to turn dot products into degrees, then compared those against the min/max angle bounds. acos is strictly decreasing on [-1, 1], so "angle outside [min, max]" is exactly "cosine outside [cos(max), cos(min)]" with the ends swapped - the bounds convert once, and the three acos calls per candidate disappear. The same loop also re-derived every already-accepted candidate's unit cell on each new triple, inside the duplicate scan: three more acos each, for every candidate accepted so far. Those cells are now kept alongside the candidates. Measured on de-novo serial stills, where the indexer runs once per image: 34.43 s -> 14.17 s on one dataset and 21.92 s -> 6.59 s on another, with the indexing rate and the merged reflection count unchanged (one gained 0.25 points of indexing rate). acos had been 40% of the whole process there. Scope is narrower than that number suggests, and worth stating: the win is on the de-novo path, which Auto selects for stills only when NO cell is known. With a known cell Auto picks ffbidx, which reaches the same filter but feeds it few candidates - measured neutral there (+0.5% instructions, -1.6% wall, identical output), and that path already runs 14x faster in absolute terms. Rotation runs the indexer twice per dataset rather than per image, so it is unaffected: the full 37-crystal battery is identical, crystal for crystal. Comparing cosines instead of angles can only move a candidate that sits on the bound, so the filter's behaviour is unchanged except at that measure-zero boundary. Co-Authored-By: Claude Opus 5 (1M context) <noreply@anthropic.com>
Jungfraujoch
Application to receive data from the PSI JUNGFRAU and EIGER detectors.
All documentation is now placed in docs/ subdirectory and for the current version hosted on Jungfraujoch Read The Docs page.
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