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Crystallography technique From Wikipedia, the free encyclopedia
Serial femtosecond crystallography (SFX) is a form of X-ray crystallography developed for use at X-ray free-electron lasers (XFELs).[1][2][3] Single pulses at free-electron lasers are bright enough to generate resolvable Bragg diffraction from sub-micron crystals. However, these pulses also destroy the crystals, meaning that a full data set involves collecting diffraction from many crystals. This method of data collection is referred to as serial, referencing a row of crystals streaming across the X-ray beam, one at a time.
While the idea of serial crystallography had been proposed earlier,[4] it was first demonstrated with XFELs by Chapman et al.[5] at the Linac Coherent Light Source (LCLS) in 2011. This method has since been extended to solve unknown structures, perform time-resolved experiments, and later even brought back to synchrotron X-ray sources.
In comparison to conventional crystallography, where a single (relatively large) crystal is rotated in order to collect a 3D data set, some additional methods have to be developed to measure in the serial mode. First, a method is required to efficiently stream crystals across the beam focus. The other major difference is in the data analysis pipeline. Here, each crystal is in a random, unknown orientation which must be computationally determined before the diffraction patterns from all the crystals can be merged into a set of 3D hkℓ intensities.
The first sample delivery system used for this technique was the Gas Dynamic Virtual Nozzle (GDVN) which generates a liquid jet in vacuum (accelerated by a concentric helium gas stream) containing crystals. Since then, many other methods have been successfully demonstrated at both XFELs and synchrotron sources. A summary of these methods along with their key relative features is given below:
In order to recover a 3D structure from the individual diffraction patterns, they must be oriented, scaled and merged to generate a list of hkℓ intensities. These intensities can then be passed to standard crystallographic phasing and refinement programs. The first experiments only oriented the patterns[13] and obtained accurate intensity values by averaging over a large number of crystals (> 100,000). Later versions correct for variations in individual pattern properties such as overall intensity variations and B-factor variations as well as refining the orientations to fix the "partialities" of the individual Bragg reflections.[14]
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