International
Tables for
Crystallography
Volume F
Crystallography of biological macromolecules
Edited by M. G. Rossmann and E. Arnold

International Tables for Crystallography (2006). Vol. F. ch. 25.2, p. 695

Section 25.2.1.1.1. Isomorphous replacement, anomalous scattering and MAD phasing

W. Fureya*

25.2.1.1.1. Isomorphous replacement, anomalous scattering and MAD phasing

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Heavy-atom-based phasing by the methods of isomorphous replacement (Green et al., 1954[link]) and/or anomalous scattering (Pepinsky & Okaya, 1956[link]) are initiated by reading one or more `scaled' files into the program PHASIT, along with estimates of the heavy-atom or anomalous-scatterer positional, occupancy and thermal parameters. Each input file can contain either isomorphous-replacement, derivative anomalous-scattering or native anomalous-scattering data. MAD (multiple-wavelength anomalous diffraction) data are treated as both isomorphous and anomalous-scattering data, in which case one simply inputs the scattering-factor differences (real part) appropriate for the wavelengths comprising the `isomorphous' data sets and the actual scattering factors (imaginary part) appropriate for the `anomalous' data sets. All possible combinations of isomorphous-replacement data, conventional anomalous-scattering data and MAD data are allowed and can be used simultaneously during phasing.

References

First citation Green, D. W., Ingram, V. M. & Perutz, M. F. (1954). The structure of haemoglobin. IV. Sign determination by the isomorphous replacement method. Proc. R. Soc. London Ser. A, 225, 287–307.Google Scholar
First citation Pepinsky, R. & Okaya, Y. (1956). Determination of crystal structures by means of anomalously scattered X-rays. Proc. Natl Acad. Sci. USA, 42, 286–292.Google Scholar








































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