search direct {} end :== delta= --{Angular grid step interval} t1min= t1max= t2min= t2max= t3min= t3max= --{The sampling is equidistant in this Euler angle range using the interval delta: t1min, t1max = theta1 minimum and maximum values t2min, t2max = theta2 minimum and maximum values t3min, t3max = theta3 minimum and maximum values} tpmin= tpmax= tmmin= tmmax= t2min= t2max= --{The sampling will be by the quasi-orthogonal method of Lattman. The interval delta is used for theta2 tpmin, tpmax = theta+ minimum and maximum values t2min, t2max = theta2 minimum and maximum values tmmin, tmmax = theta- minimum and maximum values} psimin= psimax= phimin= phimax= kappamin= kappamax= --{The sampling will by spherical polar angles psimin, psimax = psi minimum and maximum values phimin, phimax = phi minimum and maximum values kappamin, kappamax = kappa minimum and maximum values} output= --{Rotation function output filename.} list= --{File for list of highest peaks.} nlist= --{Specifies the number of highest peaks of the rotation function that will be listed.} epsilon= --{Epsilon for cluster analysis. This defines a matrix norm to determine whether two rotation matrices are close. The default value is reasonable for 10 degree grids.} symbol= --{Root name for the symbol table. If blank to table is created (this is the default.} symmetry=?|reset| --{Define symmetry operators which are required for proper grouping of symmetry related peaks during cluster analysis.} ? --{Prints current parameters and options.} --{The following symbols are created upon completion: $_nlist - number of peaks $_rfvalue_ - rotation function value $_theta1_ - for Eulerian and Lattman mode $_theta2_ - for Eulerian and Lattman mode $_theta3_ - for Eulerian and Lattman mode $_phi_ - for spherical polar angle mode $_psi_ - for spherical polar angle mode $_kappa_ - for spherical polar angle mode where runs through the clustered peak list.} --{The target for the direct rotation search is the current xray target which must be defined.}