The potential energy landscape of atomic and molecular clusters can be very
complex with many minima which can have similar energies, and this complexity
increases rapidly as the size of the clusters increases. Determining the global
minimum of these clusters is challenging since it requires extensive searching
over the potential energy surface. One approach to finding the low energy
structures of these clusters is to perform many geometry optimizations starting
at different initial coordinates. Q-Chem is able to perform such random
searches for molecular clusters containing up to two different molecule types.
In these searches the molecules are subjected to translations and rotations of
their structure to generate a new starting structure. These searches are
initiated by the JOBTYPE = RAND and it is necessary to
specify the number of molecules of the different types and the number of atoms
in the different types of molecules. For the optimization of atomic clusters,
SEARCH_ATOMIC = TRUE and the number of atom swops performed
in the structure generation (N_SWOP) can be specified. Some care has
to be taken with the specification of the input structure in the
$molecule section. All the atoms of the molecules of molecule type 1
must come before those of molecule type 2. Furthermore, the atoms of the same
molecule should be together. For examples of these studies see
J. Chem. Phys.
(2012), 137, pp. 134106. , 292 J. Phys. Chem. A
(2013), 117, pp. 5385. , 293 Phys. Chem. Chem. Phys.
(2013), 15, pp. 16214. , 733 Proc. Roy. Soc. London A
(2018), 376, pp. 20170152. .
$molecule 1 1 N 0.5682008336 0.1585044954 -0.9009280260 O -0.3450383302 -0.5598328271 -0.4634299478 O 1.7303273568 0.3403569345 0.4364171165 H 2.5236300547 -0.2494576134 0.1485689942 H 2.1020812302 1.2823911654 0.2570156558 $end $rem JOBTYPE RAND METHOD B3LYP BASIS STO-3G SCF_CONVERGENCE 6 MAX_SCF_CYCLES 100 NSEARCH 10 N_MOL_TYPE 2 NMOL1 1 N_ATOM_TYPE_1 2 NMOL2 1 N_ATOM_TYPE_2 3 N_MOVES 20 MAXBOX 10000 MIN_SEPARATION 25 MAX_DISPLACE 25 SCF_NOCRASH TRUE TIGHTEN_CONVERG TRUE GEOM_OPT_MAX_CYCLES 200 GEOM_OPT_COORDS 0 GEOM_OPT_TOL_DISPLACEMENT 1000 GEOM_OPT_TOL_GRADIENT 300 GEOM_OPT_TOL_ENERGY 100 $end
$molecule 0 1 He -1.3590894 3.0177788 -0.1662522 He -2.9853158 1.1444488 0.1036005 He 0.5068109 1.3795209 -0.2168151 Ne -1.1002149 -0.5693061 0.0381894 Ne 0.5981676 1.8697812 1.4685618 Ne -1.2376457 1.2597811 -0.0756066 $end $rem JOBTYPE RAND METHOD B3LYP DFT_D EMPIRICAL_GRIMME BASIS STO-3G SCF_CONVERGENCE 6 MAX_SCF_CYCLES 100 NSEARCH 10 SEARCH_ATOMIC TRUE N_SWOP 4 N_MOL_TYPE 2 NMOL1 3 N_ATOM_TYPE_1 1 NMOL2 3 N_ATOM_TYPE_2 1 N_MOVES 20 MAXBOX 10000 MIN_SEPARATION 25 MAX_DISPLACE 25 SCF_NOCRASH TRUE TIGHTEN_CONVERG TRUE USE_INITIAL TRUE GEOM_OPT_MAX_CYCLES 200 GEOM_OPT_COORDS 0 GEOM_OPT_TOL_DISPLACEMENT 1000 GEOM_OPT_TOL_GRADIENT 3000 GEOM_OPT_TOL_ENERGY 1000 $end
Basin hopping (BH) is a more advanced technique for locating
the global minimum on complex potential energy surfaces.
J. Phys. Chem. A
(1997), 5111, pp. 101. The BH algorithm is essentially a combination of the Metropolis sampling technique and a gradient-based local search method. This has the effect of sampling the energy basins, where an energy basin is a certain part of the configuration space around a minimum on the PES that contains all the configurations that will relax into this minimum using downhill relaxations, instead of sampling the configuration space. To enhance the efficiency of the method, BH with occasional jumping is used, 535 Chem. Phys. Lett.
(2004), 399, pp. 396. which incorporates a jumping move in addition to the standard Monte Carlo (MC) moves. Jumping is a MC move without local minimization at infinite temperature and, consequently, is always accepted. When the usual MC moves are rejected a number of times, the system is judged to be trapped at the local minimum. The temperature is raised to , and the MC jumping moves are executed several times to allow the system to escape from the local minimum. This provides an efficient way to escape from a local minimum and to explore the next basin of the valley when it is separated by high barriers. Depending on the size and complexity of the system being studied, a large number of MC_STEPS and/or MC_CYCLES to ensure the global minimum is found.
$molecule 1 1 N 0.5682008336 0.1585044954 -0.9009280260 O -0.3450383302 -0.5598328271 -0.4634299478 O 1.7303273568 0.3403569345 0.4364171165 H 2.5236300547 -0.2494576134 0.1485689942 H 2.1020812302 1.2823911654 0.2570156558 $end $rem JOBTYPE BH METHOD B3LYP BASIS STO-3G SCF_CONVERGENCE 6 MAX_SCF_CYCLES 100 MC_CYCLES 4 MC_STEPS 5 MC_TEMP 300 MAX_DISPLACE 25 MIN_SEPARATION 25 MAXBOX 5000 N_MOVES 20 N_MOL_TYPE 2 NMOL1 1 N_ATOM_TYPE_1 2 NMOL2 1 N_ATOM_TYPE_2 3 N_MOVES 20 MAXBOX 10000 MIN_SEPARATION 25 MAX_DISPLACE 25 SCF_NOCRASH TRUE GEOM_OPT_MAX_CYCLES 200 GEOM_OPT_COORDS 0 GEOM_OPT_TOL_DISPLACEMENT 2000 GEOM_OPT_TOL_GRADIENT 4000 GEOM_OPT_TOL_ENERGY 400 $end