Programs in Physics & Physical Chemistry
|[Licence| Download | New Version Template] aecz_v2_0.tar.gz(910 Kbytes)|
|Manuscript Title: Heuristic computation of the rovibrational G matrix in optimized molecule-fixed axes. Gmat 2.1|
|Authors: M.E. Castro, A. Niño, C. Muñoz-Caro|
|Program title: Gmat 2.1|
|Catalogue identifier: AECZ_v2_0|
Distribution format: tar.gz
|Journal reference: Comput. Phys. Commun. 181(2010)1471|
|Programming language: Standard ANSI C++.|
|Operating system: Linux, Windows.|
|Keywords: Rovibrational G matrix, Rotation matrix, Optimal Euler angles, Unambiguous molecule-fixed axes.|
|PACS: 02.50.Ga, 02.60.Pn, 33.20.Vq, 87.55.kd.|
Does the new version supersede the previous version?: Yes
Nature of problem:
When building molecular rovibrational Hamiltonians, the kinetic terms depend on the molecule-fixed axes orientation. Thus, an appropriate orientation can significantly simplify the treatment of pure rotation and rovibrational coupling. The kinetic terms are collected in the rovibrational G matrix. Thus, selection of an appropriate molecule-fixed reference frame is equivalent to localize the axes that minimize specific G matrix elements. From this standpoint, three different kinds of molecule-fixed axes are of interest: first, axes minimizing pure rotational elements of the G matrix; second, axes minimizing all the rovibrational G matrix elements; third, axes minimizing simultaneously pure rotational + rovibrational coupling elements.
In order to carry out the optimal selection of molecule-fixed axes, we add a hybrid method of minimization to the capabilities included in the first version of the program . Thus, we minimize specific elements of the rovibrational G matrix. To such an end, we apply a heuristic global optimization strategy, simulated annealing , followed by a Powell's local minimization .We also include a procedure to ensure that the same minimum is used when several molecular configurations are considered. In addition, an unambiguous molecule-fixed axes ordering is implemented.
Reasons for new version:
The previous version of the program, Gmat 1.0, works in principal axes of inertia. Although this axes system is adequate for pure vibrational Hamiltonians, it is not always optimal for the construction of general rovibrational Hamiltonians. However, implementing the methods presented here, we can obtain molecule-fixed axes minimizing pure rotational or/and rovibrational interactions in the G matrix. In this form, we can derive the simplest analytical form of the rovibrational Hamiltonian.
Summary of revisions:
Some new methods have been introduced:
The sample tests take a few seconds to execute.
|||M.E. Castro, A. Niño, C. Muñoz-Caro, Comput. Phys. Comm. 180 (2009) 1183|
|||S. Kirkpatrick, C.D. Gelatt Jr.; M.P. Vecchi, Science 220:4598 (1983) 671|
|||W.H. Press, B.P. Flannery, S.A. Teukolsky, W.T. Vetterling, Numerical Recipes. The Art of Scientific Computing (Cambrige University Press, Cambridge, 2007)|
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