Hi Sjors
Yeah - I’d worked that out from the paper. I can see the C4 implementation is nearly but not quite right; If I allow a search of twist and rise, it will proceed going up and down in value and gradually drift way from the correct values producing smooth tubes that are low resolution correct but featureless.
It was more the implementation of the revised and newly defined p 1_4 values I’ve been thinking.
Do I take the p twist and rise values, impose these in the helical reconstruction of the existing C4/helical class and then rerun at the same time but using C1 symmetry? Or is there a specific p** symmetry operator I need to use?
Cheers
Rich
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