Abstract

Although the success of molecular-replacement techniques requires the solution of a six-dimensional problem, this is often subdivided into two three-dimensional problems. REMO09 is one of the programs which have adopted this approach. It has been revisited in the light of a new probabilistic approach which is able to directly derive conditional distribution functions without passing through a previous calculation of the joint probability distributions. The conditional distributions take into account various types of prior information: in the rotation step the prior information may concern a non-oriented model molecule alone or together with one or more located model molecules. The formulae thus obtained are used to derive figures of merit for recognizing the correct orientation in the rotation step and the correct location in the translation step. The phases obtained by this new version of REMO09 are used as a starting point for a pipeline which in its first step extends and refines the molecular-replacement phases, and in its second step creates the final electron-density map which is automatically interpreted by CAB, an automatic model-building program for proteins and DNA/RNA structures.

Highlights

  • Molecular-replacement (MR) techniques (Rossmann & Blow, 1962; Rossmann, 1972, 1990) aim at phasing an unknown target structure using a known search molecule

  • For each test structure we show MRP, the average phase error/weighted average phase error in degrees at the end of REMO09; SYN, the average phase error in degrees at the end of the SYNERGY step; and MA, the ratio ‘number of C atoms within 0.6 Adistance from the published positions/number of C atoms in the asymmetric unit’

  • (i) Of the 38 nucleic acids only 20 are automatically solved: 16 of the 18 failures may be ascribed to the limited effectiveness of our default MOLREP procedure and two to CAB (PDB entries 3tok, for which SYN = 47, and 4gsg, for which SYN = 55); (ii) 14 of the 38 nucleic acid structures remained unsolved by both pipelines

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Summary

Symbols and abbreviations

T, tp: the numbers of atoms in the asymmetric units of the target and model structure, respectively. N = mt, Np = mtp: the numbers of atoms in the unit cells of the target structure and model structure, respectively. It is supposed, for the sake of simplicity, that all of the atoms are in general positions. Rpj are the atomic positions of the model structure when it has been well oriented and lFoc=atPedms.1⁄41. Árj is the misfit between the atomic position rj in the target and the corresponding rpj in the model structure. The scattering power at a given sin / for the target and model structure, respectively.

Introduction
General features of REMO09
Pm jEpsj2
Applications
Conclusions
Full Text
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