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多晶体法从传统上无法解释的电子密度中提取隐藏的晶体状态。

A multi-crystal method for extracting obscured crystallographic states from conventionally uninterpretable electron density.

机构信息

Structural Genomics Consortium, Nuffield Department of Medicine, University of Oxford, Roosevelt Drive, Oxford OX3 7DQ, UK.

Diamond Light Source Ltd, Harwell Science and Innovation Campus, Didcot OX11 0QX, UK.

出版信息

Nat Commun. 2017 Apr 24;8:15123. doi: 10.1038/ncomms15123.

DOI:10.1038/ncomms15123
PMID:28436492
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC5413968/
Abstract

In macromolecular crystallography, the rigorous detection of changed states (for example, ligand binding) is difficult unless signal is strong. Ambiguous ('weak' or 'noisy') density is experimentally common, since molecular states are generally only fractionally present in the crystal. Existing methodologies focus on generating maximally accurate maps whereby minor states become discernible; in practice, such map interpretation is disappointingly subjective, time-consuming and methodologically unsound. Here we report the PanDDA method, which automatically reveals clear electron density for the changed state-even from inaccurate maps-by subtracting a proportion of the confounding 'ground state'; changed states are objectively identified from statistical analysis of density distributions. The method is completely general, implying new best practice for all changed-state studies, including the routine collection of multiple ground-state crystals. More generally, these results demonstrate: the incompleteness of atomic models; that single data sets contain insufficient information to model them fully; and that accuracy requires further map-deconvolution approaches.

摘要

在大分子晶体学中,除非信号很强,否则很难严格检测到变化的状态(例如配体结合)。由于分子状态在晶体中通常只存在一小部分,因此实验中经常会出现模棱两可(“弱”或“嘈杂”)的密度。现有的方法侧重于生成最大程度准确的图谱,从而使次要状态变得可识别;实际上,这种图谱解释令人失望地主观、耗时且方法上不合理。在这里,我们报告了 PanDDA 方法,该方法通过减去一部分混淆的“基态”,自动揭示变化状态的清晰电子密度-即使是来自不准确的图谱-;通过对密度分布的统计分析,可以客观地识别变化状态。该方法完全通用,意味着所有变化状态研究的新最佳实践,包括常规收集多个基态晶体。更一般地,这些结果表明:原子模型的不完整性;单个数据集包含的信息不足以完全对其进行建模;准确性需要进一步的图谱去卷积方法。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/564e/5413968/b9e306647d98/ncomms15123-f5.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/564e/5413968/73a19fd08ad8/ncomms15123-f1.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/564e/5413968/d12566984c59/ncomms15123-f2.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/564e/5413968/7ea15f95e13a/ncomms15123-f3.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/564e/5413968/3d56bd1b57ba/ncomms15123-f4.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/564e/5413968/b9e306647d98/ncomms15123-f5.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/564e/5413968/73a19fd08ad8/ncomms15123-f1.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/564e/5413968/d12566984c59/ncomms15123-f2.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/564e/5413968/7ea15f95e13a/ncomms15123-f3.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/564e/5413968/3d56bd1b57ba/ncomms15123-f4.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/564e/5413968/b9e306647d98/ncomms15123-f5.jpg

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