Technical Support Information
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Overlay 29 10 11 12 13 14 15 16 17 18 19 20 29 30 40 41 IOp(2/9)Printing of distance and angle matrices. 0 Default: same as 2. 1 Do not print the distance matrix. 2 Print distance matrix. 00 Default: same as 20. 10 Do not print the angle matrix. 20 Print the angle matrix, using z-matrix connectivity if possible. 30 Use cutoffs instead of the z-matrix for determining which angles to print. 000 Default: same as 100. 100 Do not print dihedral angles. 200 Print dihedral angles, using the z-matrix for connectivity info. 300 Print dihedral angles, using a distance cutoff for connectivity info. 0000 Default: print only for small cases 1000 Do not print the cartesian coordinates in the input orientation 2000 Do print the cartesian coordinates in the input orientation IOp(2/10)TETRAHEDRAL ANGLE FIXING 0 Default (don't test). 1 ANGLES WITHIN 0.001 DEGREE OF 109.471 WILL BE SET TO ACOS(-1/3). 2 DO NOT TEST FOR SUCH ANGLES. IOp(2/11)PRINTING OF Z-MATRIX AND RESULTANT COORDINATES. 0 Default (print if 50 atoms or less) 1 Print 2 Don't print IOp(2/12)CROWDING ABORT CONTROL 0 Default (same as 1). 1 Abort the run for zero atomic distances only 2 Abort the run if any atoms are within 0.5 A. 3 Do not abort the run regardless of 0 distances. IOp(2/13)PUNCH COORDINATES. 0 NO 1 YES, IN 'ATOMS' FORMAT (3E20.12).
NOTE, ATOMS WILL NOT TAKE THE ATOMIC 2 YES, IN FORMAT SUITABLE
FOR COORD INPUT TO Gaussian. THE ATOMIC IOp(2/14)Internal coordinate linear independance. 0 Default (same as 2). 1 Perform the test, but do not abort the job. 2 Do not perform the test. 3 If internal coordinates are in use, test the variables for linear independance and abort the job if they are dependant. 10 Compute nuclear forces as
well as second derivatives for the test. This is not correct for the linear 100 Abort the job if the number of z-matrix
variables is not exactly the number of degrees of freedom IOp(2/15)SYMMETRY CONTROL. -1 Turns on symmetry; same as 0 for molecules but turns on assignment of space group ops. for PBC. 0 Leave symmetry in whatever state it is presently in. 1 Unconditionally turn symmetry
off. Note that symm is still called, and will determine the framework
group. 2 Bring the molecule to a symmetry orientation, but then disable further use of symmetry. 3 Don't even call symm. 4 Call Symm once with loose cutoffs, symmetrize the resulting coordinates, then confirm symmetry with tight cutoffs. 5 Recover the previous symmetry operations from the rwf, and confirm that the new structure has the same symmetry. 6 Same as 5, but get symmetry info from the chk. 00 Default (10) 10 Do re-orientation for PBC. 20 Suppress re-orientation for PBC. 100 Turn on symmetry operations for PBC. IOp(2/16)action taken if the point group changes during an optimization. 0 Default (3). 1 Keep going. 2 Keep going and leave symmetry on, using the old symmetry. 3 Keep going and leave symmetry on, using the new symmetry. 4 Abort the job. IOp(2/17)Tolerance for distance comparisons in symmetry determination. 0 Default (determined in the symmetry package, currently 1.d-8). N>0 10**-N. N<0 10**N, use same tolerance for orientation. IOp(2/18)Tolerance for non-distance comparisons in symmetry determination. 0 Default (determined in the symmetry package, currently 1.d-7). N>0 10**-N. N<0 10**N, use same tolerance for orientation. IOp(2/19)Largest allowed point group, as Hollerith string. IOp(2/20)Number (1-3 for X-Z) of axis to help specify which subgroup of the type specified in IOp(19) to use. IOp(2/29)Update of coordinates from current Z-matrix. 0 Default (1) 1 No. 2 Yes, but remove z-matrix. 3 Yes. IOp(2/30)Read in vector of atom types (for debugging). 0 No 1 Yes, format (50I2) IOp(2/40)Save (initial) structure and possible constraints in rwf 698: 0 Default (No). 1 Yes. 2 Pick up structure from rwf698 on the chk file. 3 Read in structure from input stream. IOp(2/41)Force constants for Harmonic constraints. -2 Read in force constants for each cartesian coordinates -1 No constraints. 0 Default (no constraint unless reading constraint from chk file). N N/1000 Hartree/Bohr**2 |