[randomize_file_out_normal $file]
Randomizes the calculated pattern Yc using a Normal distribution and writes Yc to the file $file.
[rand_xyz !E]
If continue_after_convergence is defined then rand_xyz is executed at the end of a refinement cycle. It adds to the site fractional coordinate a vector u,the direction of which is random and the magnitude in Å is:
|u| = T rand_xyz
where T is the current temperature. Thus to add a shift to an atom between 0 and 1 Å the following could be used:
temperature 1
site . . . occ 1 C beq 1 rand_xyz = Rand(0,1);
Note that only fractional coordinates (x, y, z) that are independent parameters are randomized.
[r_bragg #]
Reports on the R-Bragg value. R-Bragg is independent of hkl's and thus can be calculated for all phase types that contain phase peaks.
[rebin_with_dx_of !E]
rebin_with_dx_of rebins the observed data, see example CLAY.INP. It can be a function of the reserved parameter X as demonstrated in tof_bank2_1.inp. If rebin_with_dx_of evaluates to a constant then the observed data is re-binned to equal x-axis steps. For observed data that is of unequal x-axis steps then re-binning provides a means of converting to equal x-axis steps.
[rigid]…
[point_for_site $site [ux|ua E] [uy|ub E] [uz|uc E] ]…
[in_cartesian] [in_FC]
[z_matrix $atom_1 [$atom_2 E] [$atom_3 E] [$atom_4 E] ] …
[rotate E [qx|qa E] [qy|qb E] [qz|qc E] ]…
[operate_on_points $sites]
[in_cartesian] [in_FC]
[translate [tx|ta E] [ty|tb E] [tz|tc E] ]…
[operate_on_points $sites]
[rand_xyz #displacement]
[in_cartesian] [in_FC]
[start_values_from_site $unique_site_name]
rigid defines a rigid body and associated translation and rotation operations. These operations are capable of creating and manipulating rigid bodies with hinges (torsion angles).
point_for_site defines a point in space with Cartesian coordinates given by the parameters ux, uy uz. Fractional equivalents can be defined using ua, ub and uc. $site is the site that the point_for_site represents.
z_matrix defines a point in space with coordinates given in Z-matrix format as follows::
rotate rotates point_for_site’s an amount as defined by the rotate E equation around the vector defined by the Cartesian vector qx, qy, qz. The vector can be defined in fractional coordinates using qa, qb and qc instead.
translate performs a translation of point_for_site’s an amount in Cartesian equal to tx, ty, tz. The amount can be defined in fractional coordinates using ta, tb and tc instead.
If in_cartesian or in_FC is defined then the coordinates are interpreted as Cartesian or fractional atomic coordinates, respectively.
rotate and translate operates on any previously defined point_for_site’s; alternatively, point_for_site’s operated on can be identified using the operate_on_points keyword. The operate_on_points keyword must refer to previously defined point_for_site’s (see section 7.6 for a description of how to identify sites).
When continue_after_convergence is defined, rand_xyz processes are initiated after convergence. It introduces a random displacement to the translate fractional coordinates (tx, ty, tz) that are independent parameters. The size of the random displacement is given by the current temperature multiplied by #displacement where #displacement is in Å.
start_values_from_site initializes the values ta, tb, tc with corresponding values taken from the site $unique_site_name.
See section 7.10 for a description of rigid bodies.
[Rp #] [Rs #]
Defines the primary and secondary radius of the diffractometer in mm. The default is 217.5 mm.
[r_p #] [r_p_dash #] [r_wp #] [r_wp_dash #] [r_exp #] [r_exp_dash #] [gof #]
[weighted_Durbin_Watson #]
xdd dependent or global refinement indicators. Keywords ending in “_dash” correspond to background subtracted values, see section 5.6.