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110  MACROMOLECULAR CRYS TALLOGRAPHY

        (Delarue and Dumas, 2004). It is intended to be  derivatives does not allow for a straightforward
        used as a generalization of Rigid Body refinement,  interpretation of the map, it is still possible to use the
        as the six degrees of freedom of global rotation and  experimental phases in conjunction with the model
        translation are also included as Normal Modes of  at hand. Indeed, MR in even a poor experimental
        null frequency. Convincing test cases, as well as real  map will in general give a much stronger signal-to-
        cases, have shown that it works well and, although  noise ratio than regular MR based on structure factor
        it was originally described to work with C-alpha-  moduli only. This can be done in reciprocal space
        only models, it has now been modified to include all  usingananalogofthetranslationfunction, calledthe
        atoms in the refinement and has also been put on line  phased translation function (Bentley, 1997). This is
        as a web-server at http://lorentz.immstr.pasteur.fr  simply a correlation coefficient between maps of the
        (Lindahl et al., 2006).                      model placed at different origins and the experimen-
                                                     tal one. This can be carried out in reciprocal space,
                                                     where all the products of type (|F  |.|F  |) have
        7.11 How to get the best (least-biased)                            ∗   obs  model ∗
        starting phases                              been replaced by Re(F obs .F model ), where F model  is
                                                     the complex conjugate of F model . Once the model
        Once the best possible molecular replacement solu-  has been placed correctly in the unit cell of the
        tion has been found and refined by, for example,  crystal, experimental phases can be combined with
        the CNS simulated annealing protocol in internal  phases from the model, followed by solvent flat-
        coordinates space, there is a need to use the least  tening using a molecular envelope derived directly
        possible biased phases, as recently emphasized in  from the model. This usually results in a much
        Rupp et al. (2002). This is usually done by using  better map. However, the rotation function is still,
        SIGMAA-weighted maps, originally due to Read  in general, no easier to solve than without the exper-
        (Read, 1986, 1990) and implemented in most crys-  imental phases, so one might think that all of this
        tallographic packages (Refmac5 (Murshudov et al.,  is of little use. There is, however, a way out of it,
        1997), CNS (Brünger et al., 1998), etc.). Then, one  which is to scan the entire rotation function space
        can go on and try to use directly automatic con-  with the phased translation search as a score (see
        struction methods such as ARP/wARP (Perrakis  Protocol 7.6). The present author has used it in a
        et al., 2001) or Resolve (Terwilliger, 2003). How-  number of cases with success: it is, in general, com-
        ever, we wish to point out here that there exists  putationally doable and leads to a very clear signal
        a very general formalism based on mean-field the-  (Li de la Sierra et al., 2001; Delarue et al., 2002).
        ory and statistical mechanics (Delarue and Orland,  Another special case where the signal of the rota-
        2000) which, in principle, should allow most of  tion function could be enhanced concerns crystals
        the errors contained in the model phases to be  where the self-rotation function can be interpreted
        eliminated and which points to the use of other  without ambiguity; in this case, the so-called locked
        kinds of weighted coefficients, calculated in a self-  cross-rotation function (Tong and Rossmann, 1997)
        consistent manner, as inputs to the Fourier trans-  allows to search for cross rotations which are com-
        forms to calculate the map. Even though the method  patible with the self rotation function. This usually
        still remains to be implemented in a space-group  results in a much better signal-to-noise ratio.
        general program, preliminary results in the space
        group P2(1)2(1)2(1) show great promise (Delarue,
                                                     7.13 Concluding remarks
        unpublished work).
                                                     It seems pretty clear that easy-to-use and web-
                                                     interfaced, automated protocols will be more and
        7.12 Special cases: phased TF and
        locked RF                                    more useful in the near future. The possibility of
                                                     combining different tools at different steps of the
        If, for some reason, MR failed, leaving no option  integrated process makes it inevitable that more of
        but to look for heavy atom derivatives and if, for  them will be developed and open to the public.
        lack of isomorphism, the phasing power of these  What is good about this kind of approach is that
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