Intensity measurements

Author(s):  
David Blow

Once a suitable crystal has been obtained, a molecular structure investigation requires measurement of the intensities of as many Bragg reflections as possible. In this chapter, some of the options that must be decided by the experimenter will be considered, and some of the criteria used to assess the accuracy and completeness of the data will be presented. The experimenter has to make a number of strategic decisions in collecting the crystal intensity data. These include: • What X-ray source should be used? • What X-ray detector should be used? • Under what conditions should the crystal be maintained? • How long should each crystal be exposed? • What data collection technique will be used? • What resolution limit should be applied? The choice of source and detector will depend largely on what is available, but the major decision is whether to use facilities in the home laboratory or whether to use a synchrotron at a central facility. The energy released by absorption of X-rays in a crystal inevitably damages it. The process of radiation damage increases crystal disorder and reduces the intensity of scattering. The experimenter will ultimately have to abandon data collection from the damaged and disordered crystal. Under ideal experimental conditions, all the useful diffraction data can be obtained from a crystal long before radiation damage takes its toll, and radiation damage does not create a practical problem. At the other end of the scale, it may be necessary to combine the measurements from many crystals in order to obtain a complete set of diffracted intensities. There is no definite criterion to decide when a crystal is so badly damaged that it must be discarded. But if the measurements are going to be of highest quality, any observable change is bad news. The most serious effects occur in the part of the diffraction pattern at the highest observed resolution, where the observed intensities of the Bragg reflections will be altered most rapidly. The first observable effect of radiation damage is usually a reduction of high angle intensities due to increased disorder.

2018 ◽  
Vol 25 (6) ◽  
pp. 1803-1818 ◽  
Author(s):  
Amane Kobayashi ◽  
Yuki Takayama ◽  
Koji Okajima ◽  
Mao Oide ◽  
Takahiro Yamamoto ◽  
...  

X-ray diffraction imaging is a technique for visualizing the structure of biological cells. In X-ray diffraction imaging experiments using synchrotron radiation, cryogenic conditions are necessary in order to reduce radiation damage in the biological cells. Frozen-hydrated biological specimens kept at cryogenic temperatures are also free from drying and bubbling, which occurs in wet specimens under vacuum conditions. In a previous study, the diffraction apparatus KOTOBUKI-1 [Nakasako et al. (2013), Rev. Sci. Instrum. 84, 093705] was constructed for X-ray diffraction imaging at cryogenic temperatures by utilizing a cryogenic pot, which is a cooling device developed in low-temperature physics. In this study a new cryogenic pot, suitable for tomography experiments, has been developed. The pot can rotate a biological cell over an angular range of ±170° against the direction of the incident X-ray beam. Herein, the details and the performance of the pot and miscellaneous devices are reported, along with established experimental procedures including specimen preparation. The apparatus has been used in tomography experiments for visualizing the three-dimensional structure of a Cyanidioschyzon merolae cell with an approximate size of 5 µm at a resolution of 136 nm. Based on the experimental results, the necessary improvements for future experiments and the resolution limit achievable under experimental conditions within a maximum tolerable dose are discussed.


2013 ◽  
Vol 46 (4) ◽  
pp. 1225-1230 ◽  
Author(s):  
Oliver B. Zeldin ◽  
Markus Gerstel ◽  
Elspeth F. Garman

RADDOSE-3D allows the macroscopic modelling of an X-ray diffraction experiment for the purpose of better predicting radiation-damage progression. The distribution of dose within the crystal volume is calculated for a number of iterations in small angular steps across one or more data collection wedges, providing a time-resolved picture of the dose state of the crystal. The code is highly modular so that future contributions from the community can be easily integrated into it, in particular to incorporate online methods for determining the shape of macromolecular crystals and better protocols for imaging real experimental X-ray beam profiles.


2014 ◽  
Vol 70 (a1) ◽  
pp. C19-C19
Author(s):  
Soichi Wakatsuki

X-ray free electron lasers (XFEL) have shown the promise of providing new opportunities in structural biology research with their extremely high peak brilliance and short pulses. It is reaching the stage where biologically important questions can be tackled using XFEL based on the "diffract-before-destroy" concept. The first part of this presentation will focus on macromolecular crystallography using XFEL with results obtained at LCLS so far and future scope. R&D efforts being pursued at SLAC/LCLS include new beam modes, (two-color beam for de novo phasing, wider bandwidth for SAXS/WAXS and spectroscopy), beam multiplexing, a dedicated new station for in-air data collection, next generation detectors, data analysis incorporating pulse-by-pulse spectrometer measurements and post refinement. These projects are being pursued in collaboration with many groups locally and globally with a goal to provide integrated facilities for cutting edge structural biology research. For example, two-color self-seeded XFEL mode is being developed for simultaneous recording of diffraction data at two energies in order to optimize the dispersive difference between the two wavelengths for phasing. Another area of collaborative effort is a development of dedicated station for in-air data collection with a variety of sample delivery schemes. The second part will discuss a possible roadmap towards atomic resolution single particle imaging using XFEL. Here, key questions are ·Can XFEL single particle 3D structural analysis at atomic resolution be done? ·What is the pulse characteristics required? ·Can we overcome the radiation damage at soft X-ray regime? ·What is the highest resolution attainable in comparison with cryoEM? A workshop at LCLS is being organized to discuss these questions in 4 areas: radiation damage, image reconstruction algorithm, beam modes and instrumentation, sample delivery and heterogeneity. The outcome of the workshop and follow-up discussions will be presented.


2021 ◽  
Author(s):  
S. L. S. Storm ◽  
D. Axford ◽  
R. L. Owen

AbstractX-ray induced radiation damage is a limiting factor for the macromolecular crystallographer and data must often be merged from many crystals to yield complete datasets for structure solution of challenging samples. Increasing the X-ray energy beyond the typical 10-15 keV range promises to provide an extension of crystal lifetime via an increase in diffraction efficiency. To date however hardware limitations have negated any possible gains. Through the first use of a Cadmium Telluride Eiger2 detector and a beamline optimised for high energy data collection, we show that at higher energies fewer crystals will be required to obtain complete data, as the diffracted intensity per unit dose increases by a factor of more than 3 between 12.4 and 25 keV. Additionally, those higher energy data provide more information, evidenced by an increase in high-resolution limit of up to 0.3 Å, pointing to a high energy future for synchrotron-based macromolecular crystallography.


Author(s):  
Yuki Nakamura ◽  
Seiki Baba ◽  
Nobuhiro Mizuno ◽  
Takaki Irie ◽  
Go Ueno ◽  
...  

Cryocrystallography is a technique that is used more often than room-temperature data collection in macromolecular crystallography. One of its advantages is the significant reduction in radiation damage, which is especially useful in synchrotron experiments. Another advantage is that cryopreservation provides simple storage of crystals and easy transportation to a synchrotron. However, this technique sometimes results in the undesirable adhesion of frost to mounted crystals. The frost produces noisy diffraction images and reduces the optical visibility of crystals, which is crucial for aligning the crystal position with the incident X-ray position. To resolve these issues, a computer-controlled device has been developed that drizzles liquid nitrogen over a crystal to remove frost. It was confirmed that the device works properly, reduces noise from ice rings in diffraction images and enables the centering of crystals with low visibility owing to frost adhesion.


2016 ◽  
Vol 72 (3) ◽  
pp. 388-394 ◽  
Author(s):  
Robin L. Owen ◽  
Darren A. Sherrell

During, or even after, data collection the presence and effects of radiation damage in macromolecular crystallography may not always be immediately obvious. Despite this, radiation damage is almost always present, with site-specific damage occurring on very short time (dose) scales well before global damage becomes apparent. A result of both site-specific radiation damage and derivatization is a change in the relative intensity of reflections. The size and approximate rate of onset of X-ray-induced transformations is compared with the changes expected from derivatization, and strategies for minimizing radiation damage are discussed.


1999 ◽  
Vol 55 (10) ◽  
pp. 1641-1653 ◽  
Author(s):  
Elspeth Garman

The use of cryo-techniques in macromolecular crystallography has increased enormously over the last eight years and has become a vital part of modern X-ray data-collection methods. This paper presents some reasons for the rise in popularity of cryo-techniques and a brief outline of the basic methods, followed by a detailed discussion of factors to be considered when trying to optimize both the quantity and quality of the data collected. As more experimenters at synchrotrons observe significant radiation damage to crystals held near 100 K, the available options for further prolonging crystal lifetime and extending the techniques become worth investigating. Some possibilities and parameters to be considered are presented, although these must remain speculative until more experimental data are available.


2014 ◽  
Vol 70 (a1) ◽  
pp. C35-C35
Author(s):  
Ilme Schlichting

Protein crystallography using synchrotron radiation sources has had tremendous impact on biology, having yielded the structures of thousands of proteins and given detailed insight into their working mechanisms. However, the technique is limited by the requirement for macroscopic crystals, which can be difficult to obtain, as well as by the often severe radiation damage caused in diffraction experiments, in particular when using tiny crystals. To slow radiation damage, data collection is typically performed at cryogenic temperatures. With the advent of X-ray free-electron lasers (FELs) this situation appears remedied. Theoretical considerations had predicted that with sufficiently short pulses useful diffraction data can be collected before the onset of significant radiation damage that ultimately results in Coulomb explosion of the sample. This has been shown recently at the first hard X-ray FEL, the LCLS at Stanford. High resolution data collected of a stream of microcrystals of the model system lysozyme agree well with conventional data collected of a large macroscopic crystal [1] With the demonstration that de-novo phasing is feasible [2], serial femtosecond crystallography has been established as a useful tool for the analysis of tiny crystals [3] and thus the large group of proteins that resist yielding macroscopic crystals such as membrane proteins. In addition to ensure the required fast exchange of the microcrystals upon exposure, liquid jet delivery has the advantage of allowing data collection at room temperature. As demonstrated recently, this is important since structural dynamics and thus the observed conformation is often temperature dependent. Recent results will be described.


2007 ◽  
Vol 63 (3) ◽  
pp. 302-309 ◽  
Author(s):  
A. Meents ◽  
A. Wagner ◽  
R. Schneider ◽  
C. Pradervand ◽  
E. Pohl ◽  
...  

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