Shneerson V L, Ourmazd A, Saldin D K
Department of Physics, University of Wisconsin-Milwaukee, Milwaukee, WI 53201, USA.
Acta Crystallogr A. 2008 Mar;64(Pt 2):303-15. doi: 10.1107/S0108767307067621. Epub 2008 Feb 19.
It is demonstrated that a common-line method can assemble a three-dimensional oversampled diffracted intensity distribution suitable for high-resolution structure solution from a set of measured two-dimensional diffraction patterns, as proposed in experiments with an X-ray free-electron laser (XFEL) [Neutze et al. (2000). Nature (London), 406, 752-757]. Even for a flat Ewald sphere, it is shown how the ambiguities due to Friedel's law may be overcome. The method breaks down for photon counts below about 10 per detector pixel, almost three orders of magnitude higher than expected for scattering by a 500 kDa protein with an XFEL beam focused to a 0.1 microm diameter spot. Even if 10(3) orientationally similar diffraction patterns could be identified and added to reach the requisite photon count per pixel, the need for about 10(6) orientational classes for high-resolution structure determination suggests that about 10(9) diffraction patterns must be recorded. Assuming pulse and readout rates of approximately 100 Hz, such measurements would require approximately 10(7) s, i.e. several months of continuous beam time.
结果表明,如在X射线自由电子激光(XFEL)实验中所提出的那样[Neutze等人(2000年)。《自然》(伦敦),406,752 - 757],共线方法能够从一组测量得到的二维衍射图样中组装出适合高分辨率结构解析的三维过采样衍射强度分布。即使对于扁平的埃瓦尔德球,也展示了如何克服由于弗里德定律引起的模糊性。该方法在每个探测器像素的光子计数低于约10时失效,这比用聚焦到0.1微米直径光斑的XFEL光束对500 kDa蛋白质进行散射所预期的光子计数高出近三个数量级。即使可以识别并添加10³个取向相似的衍射图样以达到每个像素所需的光子计数,但对于高分辨率结构测定需要约10⁶个取向类别这一情况表明,必须记录约10⁹个衍射图样。假设脉冲和读出速率约为100 Hz,这样的测量将需要约10⁷秒,即连续束流时间约几个月。