diff options
author | Thomas White <taw@physics.org> | 2014-04-03 11:45:41 +0200 |
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committer | Thomas White <taw@physics.org> | 2014-04-03 12:54:37 +0200 |
commit | ef7f6088d3b59ed8c346c5d20a8c534e6bf041f8 (patch) | |
tree | 17b8b715abfe77435ed4280eceb3ece37e393346 | |
parent | 1e7a4f59997dea30d0b7aa720684d82fd0d3c9c0 (diff) |
check_hkl: Fix the FIXMEs and calculate B factor
-rw-r--r-- | doc/man/check_hkl.1 | 21 | ||||
-rw-r--r-- | src/check_hkl.c | 121 |
2 files changed, 130 insertions, 12 deletions
diff --git a/doc/man/check_hkl.1 b/doc/man/check_hkl.1 index a0c77566..97787e3b 100644 --- a/doc/man/check_hkl.1 +++ b/doc/man/check_hkl.1 @@ -51,6 +51,27 @@ Fix the upper resolution limit for the resolutions shells, as 1/d in m^-1. .PD Write the statistics in resolution shells to \fIfilename\fR. +.PD 0 +.IP \fB--ltest\fR +.PD +Perform an L-test for twinning. The shell file will contain the values of |L|, N(|L|) and the theoretical values for untwinned and perfectly twinned data. See Padilla and Yeates, Acta Cryst. D59 (2003) p1124. + +.PD 0 +.IP \fB--wilson\fR +.PD +Calculate a Wilson plot. The shell file will contain the values of s^2 and ln(<I>/eE) (and also the shell number and d in Angstroms for your convenience). The B factor will be calculated using data above 3.2 A resolution and displayed on the terminal. + +.PD 0 +.IP \fB--ignore-negs\fR +.PD +Ignore reflections with negative intensities. + +.PD 0 +.IP \fB--zero-negs\fR +.PD +Set to zero the intensities of reflections with negative intensities. + + .SH AUTHOR This page was written by Thomas White. diff --git a/src/check_hkl.c b/src/check_hkl.c index 9c78a42a..f409ef06 100644 --- a/src/check_hkl.c +++ b/src/check_hkl.c @@ -37,6 +37,7 @@ #include <string.h> #include <unistd.h> #include <getopt.h> +#include <gsl/gsl_fit.h> #include "utils.h" #include "statistics.h" @@ -187,6 +188,61 @@ static void l_test(RefList *list, UnitCell *cell, const SymOpList *sym, } +static double get_sfac(char el, double s) +{ + double sfac[9]; + double sf; + double s2 = pow(s/1e10, 2.0); /* s^2 in A^-2 */ + + switch ( el ) { + + case 'C' : + sfac[0] = 2.31000; sfac[1] = 20.8439; + sfac[2] = 1.02000; sfac[3] = 10.2075; + sfac[4] = 1.58860; sfac[5] = 0.568700; + sfac[6] = 0.865000; sfac[7] = 51.6512; + sfac[8] = 0.215600; + break; + + case 'N' : + sfac[0] = 12.2126; sfac[1] = 0.005700; + sfac[2] = 3.13220; sfac[3] = 9.89330; + sfac[4] = 2.01250; sfac[5] = 28.9975; + sfac[6] = 1.16630; sfac[7] = 0.582600; + sfac[8] = -11.529; + break; + + case 'O' : + sfac[0] = 3.04850; sfac[1] = 13.2771; + sfac[2] = 2.28680; sfac[3] = 5.70110; + sfac[4] = 1.54630; sfac[5] = 0.323900; + sfac[6] = 0.867000; sfac[7] = 322.9098; + sfac[8] = 0.250800; + break; + + case 'H' : + sfac[0] = 0.489918; sfac[1] = 20.6593; + sfac[2] = 0.262003; sfac[3] = 7.74039; + sfac[4] = 0.196767; sfac[5] = 49.5519; + sfac[6] = 0.049879; sfac[7] = 2.20159; + sfac[8] = 0.001305; + break; + + default : + ERROR("Unrecognised atom '%c'\n", el); + abort(); + } + + sf = sfac[0] * exp(-sfac[1]*s2); + sf += sfac[2] * exp(-sfac[3]*s2); + sf += sfac[4] * exp(-sfac[5]*s2); + sf += sfac[6] * exp(-sfac[7]*s2); + sf += sfac[8]; + + return sf; +} + + static void wilson_plot(RefList *list, UnitCell *cell, const SymOpList *sym, double rmin_fix, double rmax_fix, int nbins, const char *filename) @@ -196,9 +252,10 @@ static void wilson_plot(RefList *list, UnitCell *cell, const SymOpList *sym, Reflection *refl; RefListIterator *iter; FILE *fh; - double *plot_i; + double *plot_i, *s2; int *plot_n; - int i; + int i, ngen; + SymOpMask *mask; resolution_limits(list, cell, &rmin, &rmax); STATUS("1/d goes from %f to %f nm^-1\n", rmin/1e9, rmax/1e9); @@ -219,42 +276,82 @@ static void wilson_plot(RefList *list, UnitCell *cell, const SymOpList *sym, if ( plot_i == NULL ) return; for ( i=0; i<nbins; i++ ) plot_i[i] = 0.0; + s2 = malloc(nbins*sizeof(double)); + if ( s2 == NULL ) return; + plot_n = calloc(nbins, sizeof(int)); if ( plot_n == NULL ) return; + ngen = num_equivs(sym, NULL); + mask = new_symopmask(sym); + for ( refl = first_refl(list, &iter); refl != NULL; refl = next_refl(refl, iter) ) { signed int h, k, l; - double d, intensity; + double s, intensity, E; int bin; + int e; get_indices(refl, &h, &k, &l); - d = resolution(cell, h, k, l); /* This gives "s" */ + s = resolution(cell, h, k, l); /* This gives "s" directly */ intensity = get_intensity(refl); - bin = (pow(d, 2.0) - s2min)/s2step; + bin = (pow(s, 2.0) - s2min)/s2step; + + special_position(sym, mask, h, k, l); + e = ngen / num_equivs(sym, mask); - /* FIXME: Divide by epsilon and Sigma */ - plot_i[bin] += intensity; + /* Average atoms per residue from Rupp BMC 1st ed p356 */ + E = 5.00*get_sfac('C', s); + E += 1.35*get_sfac('N', s); + E += 1.50*get_sfac('O', s); + E += 8.00*get_sfac('H', s); + + plot_i[bin] += intensity / (e*E); plot_n[bin]++; } - for ( i=0; i<nbins; i++ ) plot_i[i] = log(plot_i[i] / plot_n[i]); + free_symopmask(mask); + + for ( i=0; i<nbins; i++ ) { + plot_i[i] = log(plot_i[i] / plot_n[i]); + s2[i] = s2min + (i+0.5)*s2step; + } fh = fopen(filename, "w"); if ( fh == NULL ) return; - fprintf(fh, " n s^2/A^-2 d/A <I>\n"); + fprintf(fh, " n s^2/A^-2 d/A ln <I>/eE nrefl\n"); for ( i=0; i<nbins; i++ ) { - double s2 = s2min + (i+0.5)*s2step; - fprintf(fh, "%3i %8.6f %8.4f %10f\n", i, - s2/1e20, 0.5e10/sqrt(s2), plot_i[i]); + fprintf(fh, "%3i %8.6f %8.4f %10f %6i\n", i, + s2[i]/1e20, 0.5e10/sqrt(s2[i]), plot_i[i], plot_n[i]); } fclose(fh); + if ( rmax < 3.125e9 ) { + ERROR("Resolution too low to estimate B factor\n"); + } else { + int bs = (pow(3.125e9/2.0, 2.0) - s2min)/s2step + 1; + double lnk, minus2B, cov00, cov01, cov11, sumsq; + double B; + if ( nbins-bs < 3 ) { + ERROR("Not enough bins to estimate B factor\n"); + ERROR("Resolution of data, or number of bins, is too " + "low.\n"); + } else { + gsl_fit_linear(&s2[bs], 1, &plot_i[bs], 1, nbins-bs, + &lnk, &minus2B, &cov00, &cov01, &cov11, + &sumsq); + B = -minus2B/2.0; + STATUS("ln k = %.2f\n", lnk); + STATUS("B = %.2f A^2\n", B*1e20); + } + } + + free(plot_i); free(plot_n); } |