Data processing

AE Austin Echelmeier
JV Jorvani Cruz Villarreal
MM Marc Messerschmidt
DK Daihyun Kim
JC Jesse D. Coe
DT Darren Thifault
SB Sabine Botha
AE Ana Egatz-Gomez
SG Sahir Gandhi
GB Gerrit Brehm
CC Chelsie E. Conrad
DH Debra T. Hansen
CM Caleb Madsen
SB Saša Bajt
JM J. Domingo Meza-Aguilar
DO Dominik Oberthür
MW Max O. Wiedorn
HF Holger Fleckenstein
DM Derek Mendez
JK Juraj Knoška
JM Jose M. Martin-Garcia
HH Hao Hu
SL Stella Lisova
AA Aschkan Allahgholi
YG Yaroslav Gevorkov
KA Kartik Ayyer
SA Steve Aplin
HG Helen Mary Ginn
HG Heinz Graafsma
AM Andrew J. Morgan
DG Dominic Greiffenberg
AK Alexander Klujev
TL Torsten Laurus
JP Jennifer Poehlsen
UT Ulrich Trunk
DM Davide Mezza
BS Bernd Schmidt
MK Manuela Kuhn
RF Raimund Fromme
JS Jolanta Sztuk-Dambietz
NR Natascha Raab
SH Steffen Hauf
AS Alessandro Silenzi
TM Thomas Michelat
CX Chen Xu
CD Cyril Danilevski
AP Andrea Parenti
LM Leonce Mekinda
BW Britta Weinhausen
GM Grant Mills
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The KDO8PS diffraction patterns collected were identified and calibrated using Cheetah71. For hit-finding, a minimum of 2 connected pixels with a count above a threshold of 500 ADU with a minimum signal-to-noise ratio of 8 was considered a peak, and an image containing at least 10 such peaks was classified as a hit. From the ~4,100,000 images collected, 37,000 were classified as hits, which corresponds to an average hit rate of 0.9%.

Approximately 46% of the identified hits could be indexed and the Bragg reflections integrated using the software package CrystFEL (version 0.8.0)55, based on the peak locations found by Cheetah. Indexing was performed by CrystFEL’s indexamajig sequentially trying XGANDALF72, DirAx73, MOSFLM74 and XDS75 requiring a cubic body-centered lattice and unit cell parameters of a = b = c = 118 Å and α=β=γ=90° (Supplementary Fig. 5). The indexamajig integration radii were set to 2, 3, 4 pixels and indexing solutions were checked by ensuring that they accounted for at least 50% of the observed peaks (option “check-peaks”).

The indexed patterns were further processed with ambigator76 to resolve the indexing ambiguity inherent to the cubic space group I23 for serially collected data. The number of correlation coefficients per crystal was limited to 1000 for speed, and 10 passes of ambiguity resolution were made over all crystals. This resulted in 8315 indexing assignments being changed, corresponding to roughly 50% of the data as expected. The indexed reflections were subsequently scaled and merged using partialator77, applying the unity model (without partiality modeling) over 3 iterations. The intensities were converted to structure factor moduli using truncate (from the CCP4 suite78), and a fraction of 0.1 reflections were included in the generated Rfree set. The L-test implemented in truncate was used to ascertain successful de-twinning of the data (Supplementary Fig. 6).

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