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 Results for DC.creator="C." AND DC.creator="M." AND DC.creator="Weeks" in section 16.1.12 of volume F
Computer programs for dual-space phasing
Sheldrick, G. M., Gilmore, C. J., Hauptman, H. A., Weeks, C. M., Miller, R. and Usón, I.  International Tables for Crystallography (2012). Vol. F, Section 16.1.12, pp. 426-429 [ doi:10.1107/97809553602060000850 ]
... sigma] is the standard deviation of the map density andwhere M is the number of observable reflections within the resolution sphere ... the heaviest atom in the E map with perfect phases; c is the cycle number.where B is the usual overall temperature ... It is also available as part of the BnP package (Weeks et al., 2002) that was produced in collaboration with ...

SUPERFLIP: charge flipping
Sheldrick, G. M., Gilmore, C. J., Hauptman, H. A., Weeks, C. M., Miller, R. and Usón, I.  International Tables for Crystallography (2012). Vol. F, Section 16.1.12.6, pp. 428-429 [ doi:10.1107/97809553602060000850 ]
... a previously unsolvable structure becomes solvable by the modified algorithm. (c) for |FH| unobserved. (d) for H = 0. In other words ... Se atoms is reported in the same paper. References Dumas, C. & van der Lee, A. (2008). Macromolecular structure by charge ...

HySS
Sheldrick, G. M., Gilmore, C. J., Hauptman, H. A., Weeks, C. M., Miller, R. and Usón, I.  International Tables for Crystallography (2012). Vol. F, Section 16.1.12.5, p. 428 [ doi:10.1107/97809553602060000850 ]
... Radhakannan, T., McCoy, A. J., Read, R. J., Storoni, L. C., Romo, T. D., Sacchettini, J. C. & Terwilliger, T. C. (2007). Automated structure determination with Phenix. In Evolving ...

SnB and BnP
Sheldrick, G. M., Gilmore, C. J., Hauptman, H. A., Weeks, C. M., Miller, R. and Usón, I.  International Tables for Crystallography (2012). Vol. F, Section 16.1.12.4, p. 428 [ doi:10.1107/97809553602060000850 ]
... It is also available as part of the BnP package (Weeks et al., 2002) that was produced in collaboration with the ... http://www.hwi.buffalo.edu/BnP/ . References Miller, R., Shah, N., Green, M. L., Furey, W. & Weeks, C. M. (2007). Shake-and-Bake on the ...

SHELX
Sheldrick, G. M., Gilmore, C. J., Hauptman, H. A., Weeks, C. M., Miller, R. and Usón, I.  International Tables for Crystallography (2012). Vol. F, Section 16.1.12.3, p. 428 [ doi:10.1107/97809553602060000850 ]
... SHELX/ . References Fu, Z.-Q., Chrzas, J., Sheldrick, G. M., Rose, J. & Wang, B.-C. (2007). A parallel program using SHELXD for quick heavy ... Appl. Cryst. 40, 387-390. Schneider, T. R. & Sheldrick, G. M. (2002). Substructure solution with SHELXD. Acta Cryst. D58, ...

IL MILIONE
Sheldrick, G. M., Gilmore, C. J., Hauptman, H. A., Weeks, C. M., Miller, R. and Usón, I.  International Tables for Crystallography (2012). Vol. F, Section 16.1.12.2, pp. 427-428 [ doi:10.1107/97809553602060000850 ]
... package can be obtained from http://www.ic.cnr.it . References Burla, M. C., Caliandro, R., Camalli, M., Carrozzini, B., Cascarano, G. L., De Caro, L., Giacovazzo, ...

ACORN
Sheldrick, G. M., Gilmore, C. J., Hauptman, H. A., Weeks, C. M., Miller, R. and Usón, I.  International Tables for Crystallography (2012). Vol. F, Section 16.1.12.1, pp. 426-427 [ doi:10.1107/97809553602060000850 ]
... sigma] is the standard deviation of the map density andwhere M is the number of observable reflections within the resolution sphere ... the heaviest atom in the E map with perfect phases; c is the cycle number.where B is the usual overall temperature ... package at http://www.ccp4.ac.uk . References Dodson, E. J. & Woolfson, M. M. (2009). ACORN2: new developments of the ACORN ...

CRUNCH2 - Karle-Hauptman determinants
Sheldrick, G. M., Gilmore, C. J., Hauptman, H. A., Weeks, C. M., Miller, R. and Usón, I.  International Tables for Crystallography (2012). Vol. F, Section 16.1.12.7, p. 429 [ doi:10.1107/97809553602060000850 ]
CRUNCH2 - Karle-Hauptman determinants 16.1.12.7. CRUNCH2 - Karle-Hauptman determinants The program CRUNCH2 is quite different to the other programs mentioned in this section. With the exception of some E-map recycling at the end to complete a substructure, CRUNCH2 operates entirely in reciprocal space by maximizing higher-order Karle-Hauptman determinants ...

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