Difference between revisions of "Direct methods"
From Online Dictionary of Crystallography
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== Definition == | == Definition == | ||
| − | + | The family of methods for solving the [[phase problem]] in crystal [[structure determination]]. The phases of scattered diffraction beams cannot be directly observed. However, they can be estimated from probability relationships applied to the phases of the most intense diffraction peaks. The facts that scattering centres in a crystal are discrete atoms (''i.e.'' sources of electron density) and that the electron density must be non-negative are the types of constraints that restrict the possible values of the phases, and allow initial estimates of some of them. | |
| − | + | == See also == | |
| − | + | Direct methods. | |
| + | C. Giacovazzo. ''International Tables for Crystallography'' (2006). Vol. B, ch. 2.2, pp. 210-234 [http://dx.doi.org/10.1107/97809553602060000555 doi:10.1107/97809553602060000555] | ||
| − | + | [[Category: Structure determination]] | |
Revision as of 13:40, 29 March 2008
Direct methods
Other languages
Méthodes directes (Fr). Metodi diretti (It). 直接法 (Ja).
Definition
The family of methods for solving the phase problem in crystal structure determination. The phases of scattered diffraction beams cannot be directly observed. However, they can be estimated from probability relationships applied to the phases of the most intense diffraction peaks. The facts that scattering centres in a crystal are discrete atoms (i.e. sources of electron density) and that the electron density must be non-negative are the types of constraints that restrict the possible values of the phases, and allow initial estimates of some of them.
See also
Direct methods. C. Giacovazzo. International Tables for Crystallography (2006). Vol. B, ch. 2.2, pp. 210-234 doi:10.1107/97809553602060000555