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134  MACROMOLECULAR CRYS TALLOGRAPHY

        Stanley, 1963), has proved to be quite powerful  computer programs such as MULTAN (Main et al.,
        and efficient as an optimization method when used  1980) and SHELXS (Sheldrick, 1990), can provide
        to reduce the value of the minimal function. For  solutions for structures containing less than 100–150
        example, a typical phase-refinement stage consists  unique non-hydrogen atoms. With few exceptions,
        of three iterations or scans through the reflection  however, phase refinement alone is not sufficient
        list, with each phase being shifted a maximum of  to solve larger structures. In such cases, successful
                     ◦
        two times by 90 in either the positive or negative  applications require a dual-space optimization pro-
        direction during each iteration. The refined value  cedure that has come to be known as Shake-and-Bake
        for each phase is selected, in turn, through a pro-  (Weeks et al 1994; Miller et al., 1993). Shake-and-
        cess that involves evaluating the minimal function  Bake is also a powerful method for smaller struc-
        using the original phase and each of its shifted val-  tures and substructures, effectively avoiding most
        ues (Weeks et al., 1994). The phase value that results  cases of false minima. The distinctive feature of
        in the lowest minimal-function value is chosen at  this procedure is the repeated and unconditional
        each step. Refined phases are used immediately in  alternation of reciprocal-space phase refinement
        the subsequent refinement of other phases.    (Shaking) with a complementary real-space process
                                                     that seeks to improve phases by applying con-
                                                     straints (Baking). The Shake-and-Bake algorithm was
        9.3.3 Dual-space optimization
                                                     implemented first in SnB and then independently
        Conventional reciprocal-space direct methods,  in SHELXD. Although both reciprocal-space opti-
        implementing  tangent-formula  refinement  in  mization methods are available in both programs,



                                           Start

                      2               1
                        Generate         Normalize
                        invariants         data
                      3                                   7
                        Generate            Yes             Another  No  Manual
                          trial                                          stop
                                                             trial?
                                    FFT
                      4
                         Refine                Pick
                         phases Yes      FFT-1 peaks
                                  Another
                                   cycle?
                                                        No
                                                               No
                                     No
                             5                            6            Automated
                                                Solution     Auto
                               Compute FOMs                               stop
                                                 found?  Yes  run?  Yes
        Figure 9.2 A flow chart for structure solution using the direct-methods algorithm, Shake-and-Bake. Steps 1 and 2 involve computation of the
        normalized structure-factor magnitudes and generation of the triplet structure invariants, respectively. Step 3 is the start of the outer or trial
        structure loop in which trial structures consisting of randomly positioned atoms are generated and tested. Step 4 is the inner or Shake-and-Bake
        cycle which consists of a phase-refinement step involving either tangent-formula refinement or parameter-shift optimization of the minimal
        function, a Fourier transform resulting in an electron-density map, selection of the largest peaks on the map, and an inverse Fourier transform to
        generate new phases by means of a structure-factor calculation assuming these peaks to be atoms. The number of such cycles and the number of
        peaks used in the structure-factor calculation depend on the number of atoms to be located (Table 9.4). Step 5 is the evaluation of the refined
        trial structures based on the values of the figures of merit (see Section 9.4) to determine which trials, if any, are solutions. If solutions are being
        recognized automatically (Step 6), the substructure determination is terminated as soon as the first solution is found. Otherwise,
        processing continues (Step 7) until a predetermined number of trial structures are completed.
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