Molecular symmetry group theory

Symmetiy Relations. Each normal coordinate and every wavefunction involving products of the normal coordinates, must transform under the symmetry operations of the molecule as one of the symmetry species of the molecular point group. The ground-state function in Eq. (3 a) is a Gaussian exponential function that is quadratic in Q, and examination shows that this is of Xg symmetry for each normal coordinate, since it is unchanged by any of the symmetry operations. From group theory the symmetry of a product of two functions is deduced from the symmetry species for each function by a systematic procedure discussed in detail in Refs. 4, 5,7, and 9. The results for the D i, point group apphcable to acetylene can be summarized as follows ... [Pg.427]

Mezey, P.G. (1987b). The Shape of Molecular Charge Distributions Group Theory without Symmetry. J.Comput.Chem., 8,462-469. [Pg.617]

Mezey PG. The shape of molecular charge distributions group theory without symmetry. J Comput Chem 1987 8 462 -69. [Pg.364]

When the Colonel was asked about teaching and research some time ago he replied "They are one and the same. When I do research, I get materials for my lectures, and when I teach I get ideas for my research. Many of us have also learned from the Colonel how much one can teach while seeming to merely inquire about the day s research progress. Certainly, his research provided the rest of us with material for our teaching, and in many areas. His work on boranes and on carboxypeptidase are the standard textbook treatments already. He used group theory and symmetry extensively in his research., and his Harvard course on Molecular Symmetry and Molecular Orbitals provided a perspective not available from any of the standard texts. Writing - of papers, of books, of... [Pg.14]

APPENDIX. GROUP THEORY AND SYMMETRY IN THE BRILLOUIN ZONE AS APPLIED TO LATTICE DYNAMICS OF MOLECULAR SOLIDS... [Pg.293]

Atoms have complete spherical synnnetry, and the angidar momentum states can be considered as different synnnetry classes of that spherical symmetry. The nuclear framework of a molecule has a much lower synnnetry. Synnnetry operations for the molecule are transfonnations such as rotations about an axis, reflection in a plane, or inversion tlnough a point at the centre of the molecule, which leave the molecule in an equivalent configuration. Every molecule has one such operation, the identity operation, which just leaves the molecule alone. Many molecules have one or more additional operations. The set of operations for a molecule fonn a mathematical group, and the methods of group theory provide a way to classify electronic and vibrational states according to whatever symmetry does exist. That classification leads to selection rules for transitions between those states. A complete discussion of the methods is beyond the scope of this chapter, but we will consider a few illustrative examples. Additional details will also be found in section A 1.4 on molecular symmetry. [Pg.1134]

We now turn to electronic selection rules for syimnetrical nonlinear molecules. The procedure here is to examme the structure of a molecule to detennine what synnnetry operations exist which will leave the molecular framework in an equivalent configuration. Then one looks at the various possible point groups to see what group would consist of those particular operations. The character table for that group will then pennit one to classify electronic states by symmetry and to work out the selection rules. Character tables for all relevant groups can be found in many books on spectroscopy or group theory. Ftere we will only pick one very sunple point group called 2 and look at some simple examples to illustrate the method. [Pg.1135]

It is recommended that the reader become familiar with the point-group symmetry tools developed in Appendix E before proceeding with this section. In particular, it is important to know how to label atomic orbitals as well as the various hybrids that can be formed from them according to the irreducible representations of the molecule s point group and how to construct symmetry adapted combinations of atomic, hybrid, and molecular orbitals using projection operator methods. If additional material on group theory is needed. Cotton s book on this subject is very good and provides many excellent chemical applications. [Pg.149]

Vincent, A. (2000) Molecular Symmetry and Group Theory, 2nd edn., John Wiley, Chichester. [Pg.102]

The first line indicates that the syrrumetry could not be determined for this state (the symmetry itself is given as Sym). We will need to determine it ourselves. Molecular symmetry in excited states is related to how the orbitals transform with respect to the ground state. From group theory, we know that the overall symmetry is a function of symmetry products for the orbitals, and that only singly-occupied orbitals are... [Pg.225]

A nonlinear molecule of N atoms with 3N degrees of freedom possesses 3N — 6 normal vibrational modes, which not all are active. The prediction of the number of (absorption or emission) bands to be observed in the IR spectrum of a molecule on the basis of its molecular structure, and hence symmetry, is the domain of group theory [82]. Polymer molecules contain a very high number of atoms, yet their IR spectra are relatively simple. This can be explained by the fact that the polymer consists of identical monomeric units (except for the end-groups). [Pg.312]

It should be noted that the trace of a matrix that represents a given geo] operation is equal to 2 cos y 1, the choice of signs is appropriate to or improper operations. Furthermore, it should be noted that the aim direction of rotation has no effect on the value of the trace, as a inverse sense corresponds only to a change in sign of the element sin y. TE se operations and their matrix representations will be employed in the following chapter, where the theory of groups is applied to the analysis of molecular symmetry. [Pg.92]

We therefore conclude that, for a combination of model, numerical and conceptual reasons the OHAO basis is well-adapted to a theory of valence. The hybrid orbital basis (for simple molecules) has a distinctive symmetry property it carries a permutation representation of the molecular symmetry group the equivalent orbitals are always sent into each other, never into linear combinations of each other. This simple fact enables the hybrid orbital basis to be studied in a way which is physically more transparent than the conventional AO basis. [Pg.64]

Symmetry-forbidden transitions. A transition can be forbidden for symmetry reasons. Detailed considerations of symmetry using group theory, and its consequences on transition probabilities, are beyond the scope of this book. It is important to note that a symmetry-forbidden transition can nevertheless be observed because the molecular vibrations cause some departure from perfect symmetry (vibronic coupling). The molar absorption coefficients of these transitions are very small and the corresponding absorption bands exhibit well-defined vibronic bands. This is the case with most n —> n transitions in solvents that cannot form hydrogen bonds (e 100-1000 L mol-1 cm-1). [Pg.30]

How does one determine the symmetry number As illustrated in the section above it is equal to the number of rotations that take the molecule into itself. Another and very attractive method is based on the use of group theory. Students who have taken a course in inorganic chemistry have been introduced to group theory. If the reader is uncomfortable with this topic the next few paragraphs can be skipped, especially since this method of finding molecular symmetry numbers need not to be used for finding the ratios of symmetry numbers, Si/s2, required to understand isotopomer fractionation. [Pg.111]

A Straightforward answer to the above question would be a consideration of molecular symmetry. According to group theory, doubly degenerate molecular orbitals, denoted by the symbol e, can arise if a given molecule has one three-fold or higher axis of rotation, or if it has Djj symmetry. It is well... [Pg.187]

Symmetry The word symmetry means the same measure, which denotes harmony and beauty of the parts. It also plays a very important role in molecular architecture and material properties. The study of molecular symmetry is through a branch of group theory, that is, the point groups of rotations that leave one point... [Pg.98]

Part of a three-volume set covering applications of group theory to physics. The articles by McIntosh and by Wulfman are well worth reading. They contain relatively short and self-contained presentations of material about symmetries of atomic and molecular systems that is difficult to find elsewhere in comparably accessible form. [Pg.120]

The presentation here is short, and limited to those aspects of symmetry and group theory that are directly useful in interpreting molecular structure and spectroscopy. Nevertheless I hope that the reader will begin to sense some of the beauty of the subject. Symmetry is at the heart of our understanding of the physical laws of nature. If a reader is happy with what appears in this book, I must count this a success. But if the book motivates a reader to move deeper into the subject, I shall be gratified. [Pg.130]

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