Small Molecule Serial Crystallography

Small Molecule Serial Crystallography

Structural Dynamics: Small Molecule Serial Crystallography Jason Benedict University at Buffalo Structural Dynamics Quantifying time-dependent phenomena in crystalline materials Flexible Guest crystals Exchange Nature 495, 80–84 (07 March 2013) Nature Chemistry 7, 65–72 (2015) Photochemical Catalysis reactions Charge transport J. Am. Chem. Soc., 2012, 134 J. Org. Chem. 9, 3311- (31), pp 12932–12935 3666 (2008) X-ray Diffraction – The Basics Structural Dynamics Quantifying time-dependent phenomena in crystalline materials Flexible Guest crystals Exchange Nature 495, 80–84 (07 March 2013) Nature Chemistry 7, 65–72 (2015) Photochemical Catalysis reactions Charge transport J. Am. Chem. Soc., 2012, 134 J. Org. Chem. 9, 3311- (31), pp 12932–12935 3666 (2008) Structural Dynamics Today In-situ crystal diffraction Benedict Group and Environmental Control Cell (ECC) ChemMatCARS •Vacuum, gas, solution and humidity J. Appl. Cryst.(2015), 48, 578-581 Environmental control cells (ECCs) Study crystalline nanoporous materials under ‘real world’ conditions Structural Dynamics Gases and liquids as chemical stimuli Approaching ‘real time’ structural information about guest and framework – solving single crystal structures! Structural Dynamics • How do water molecules leave? • Stepwise? • Simultaneous? • What is the relationship between compression of a-axis and dehydration? • Dynamic in situ X-ray Trihydrate (one coordinated water Anhydrous Diffraction experiments and two ‘free’ water molecules) should address both Space group P21/푐 Space group P21/푐 questions! a = 12.4381 Å a = 11.078 Å b = 7.6827 Å b = 7.761 Å c = 15.8704 Å c = 15.945 Å β = 106.1466 ° β = 106.829 ° Structural Dynamics 108 • Carefully controlled flow 16 rates of dry nitrogen gas 107 trigger the dehydration. 106 14 • Note the large change in 105 β and a! 12 104 Beta • ‘Slice up’ the data to yield single crystal Vector Length (Å) Length Vector 103 10 structures 102 8 • Faster data collection = 101 shorter time to collect 6 100 complete data set 0 2000 4000 6000 8000 10000 Time (sec) A B C beta Structural Dynamics Jump to the conclusion…. “trihydrate” “dihydrate” “anhydrous” P21/c P21/c P21/c a = 12.607 Å a = 11.165 Å a = 11.326 Å b = 7.685 Å b = 7.766 Å b = 7.694 Å c = 15.926 Å c = 15.784 Å c = 15.83 Å β = 106.527° β = 103.19° β = 106.49° V = 1479 Å3 V = 1332 Å3 V = 1323 Å3 Un-twist Twist and compress (slow simultaneous loss (Rapid loss of single water) of remaining two waters) • More complex motion than predicted by ex situ measurements • 2-step activation process • Room temperature activation Structural Dynamics Tomorrow: Small Molecule Serial Crystallography • What is it? • Technique developed by structural biologists • Datasets consist of single images collected from tens or hundreds of thousands of single crystals • New sample delivery methods • New data analysis methods • Why would you do this? • Only method capable of obtaining time-resolved data on: • Irreversible processes • Applies to process and damage • Sub-micron crystals Trends in Biochemical Sciences, September 2017, Vol. 42, No. 9 Trends in Biochemical Sciences, September 2017, Vol. 42, No. 9 Tens of thousands to hundreds of thousands to millions of frames of data each from a crystal of unknown size and orientation must be turned into a single data set of indexed intensities Many of these data analysis tools – built for macromolecular crystals – will not work on crystals with small- to medium-sized unit cells New computational tools required! Structural Dynamics Tomorrow: Small Molecule Serial Crystallography • So what does NSF ChemMatCARS need from you? 365 nm >615 nm • What are your Structural Dynamics Dreams? • What are your systems of interest? • What are your physical processes of interest? • What crystalline thing would you want to watch? • What would you need to make your Structural Dynamics Dreams come true? Structural Dynamics X-ray Chopper Proposed High‐speed Jülich Chopper Profs. Philip Coppens and Jason Benedict Isolating single X-ray pulses is critical for time- U. Buffalo resolved studies. The width of the X-ray pulse limits the temporal resolution of the experiment. Time-resolved Crystallography • Timing FPGA (field-programmable gate array ) Commissioning in 2017-3 Select single pulses • Some operational modes requires disk change plus extensive Provide an adjustable time window realignment (several hours) • 190 ns and 20 µs in duration. • For experiments that do not require single X-ray pulses, the Easy select single pulses, and longer chopper must be completely removed from beam path temporal resolution by adjusting Soon to-be–obsolete table height. • Code to operate not compatible with the APS-U time Fully compatible with FPGA structure • May not be possible to integrate into FPGA.

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