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Groups operations

Nuclear pemuitations in the N-convention (which convention we always use for nuclear pemuitations) and rotation operations relative to a nuclear-fixed or molecule-fixed reference frame, are defined to transfomi wavefunctions according to (equation Al.4.56). These synnnetry operations involve a moving reference frame. Nuclear pemuitations in the S-convention, point group operations in the space-fixed axis convention (which is the convention that is always used for point group operations see section Al.4.2,2 and rotation operations relative to a space-fixed frame are defined to transfomi wavefiinctions according to (equation Al.4.57). These operations involve a fixed reference frame. [Pg.155]

A detailed discussion of the relation between MS group operations and point group operations is given in section... [Pg.182]

Periodic boundary conditions can also be used to simulate solid state con dition s although TlyperChem has few specific tools to assist in setting up specific crystal symmetry space groups. The group operation s In vert, Reflect, and Rotate can, however, be used to set up a unit cell manually, provided it is rectangular. [Pg.201]

The equivalence of the pairs of Cartesian coordinate displacements is a result of the fact that the displacement vectors are connected by the point group operations of the C2v group. In particular, reflection of Axr through the yz plane produces - Axr, and reflection of AyL through this same plane yields AyR. [Pg.352]

Don t worry about how we eonstruet Ti, T2, and T3 yet. As will be demonstrated later, we form them by using symmetry projeetion operators defined below) We determine how the "T" basis funetions behave under the group operations by allowing the operations to aet on the 8j and interpreting the results in terms of the Ti. In partieular. [Pg.587]

Just as the individual orbitals formed a basis for aetion of the point-group operators, the eonfigurations (N-orbital produets) form a basis for the aetion of these same point-group operators. Henee, the various eleetronie eonfigurations ean be treated as funetions on whieh S operates, and the maehinery illustrated earlier for deeomposing orbital symmetry ean then be used to earry out a symmetry analysis of eonfigurations. [Pg.595]

The role of symmetry in determining whether such integrals are non-zero can be demonstrated by noting that the integrand, considered as a whole, must contain a component that is invariant under all of the group operations (i.e., belongs to the totally... [Pg.596]

The systematic application of both antithetic steps will now be exemplified with the admittedly trivial synthesis of 3-methylbutanal (isovaleraldehyde). Functional group operations would yield the following alternative target molecules ... [Pg.196]

Multiplication of Co-Representation Matrices.—We have referred above to the representations of nonunitary groups as co-representations. This distinction is made because the co-representation matrices for the group operators do not multiply in the same way as do the operators themselves.5 As will be seen below, this is a direct result of the fact that some of the operators in the group are antilinear. Consider that is the a 6 basis function of the i411 irreducible co-representation of G. The co-representation matrices D (u) and D (a) may be defined such that... [Pg.731]

For a review of space group operator rotation, see G. F. Koster, Solid State Physics, 5, 173 (1958). [Pg.742]

Shatenshtein et al.5 5 5- 591 have also measured rate coefficients for dedeuteration of thiophen derivatives by lithium or potassium l-butoxides in dimethyl sulphoxide or l-butyl alcohol (70 vol. %) in diglyme (Table 178). Interestingly, the 2 position is more reactive than the 3 position and this was reasonably attributed to the —I effect of the hetero sulphur atom. The methyl substituent lowers the reactivity of the 2 position from each position in accord with its +1 effect and consequently the effect was greatest from the 3 position. However, the deactivation from the 5 position was greater than from the 4 position, and this was incorrectly attributed to the +M effect of methyl group operating from the 5 position since... [Pg.270]

The details of the operation Rr can be further speeified by the 3x3 matrix which represents the operation R in a suitably chosen coordinate system [2], in which also the vector r is expressed. For the operation on a function of r we need the inverse of the space group operation,... [Pg.130]

A transformation of the number density matrix N under a space group operation means that both variables are transformed ... [Pg.130]

If the density is invariant under the space group operation R m we have with (III.4) and (111.17b),... [Pg.133]

In the case of a perfect crystal the Hamiltonian commutes with the elements of a certain space group and the wave functions therefore transform under the space group operations accorc g to the irreducible representations of the space group. Primarily this means that the wave functions are Bloch functions labeled by a wave vector k in the first Brillouin zone. Under pure translations they transform as follows... [Pg.134]

Similar studies were carried out with methoxycyclohexanones.138 3-Methoxy groups showed no evidence of chelation effects with these reagents and the 2-methoxy group showed an effect only with Zn(BH4)2. This supports the suggestion that the effect of the hydroxy groups operates through deprotonated alkoxide complexes. [Pg.414]

A further property of die dieter tables arises from the fact that every symmetry group has an irreducible representation that is invariant under all of die group operations. This irreducible representation is a one-by-one unit matrix (the number one) for every class of operation. Obviously, the characters, are all then equal to one. AS this irreducible representation is by convention taken to be the first row of all Character tables consists solely of ones. The significance of the character tables will become more apparent by consideration of an example. [Pg.105]

Robin Clark s group operates from University College in London their Website http //www.chem.ucl.ac.uk/resources/raman/speclib.html is informative, and contains links to many spectra. The Raman spectrum of malachite is interpreted in M. Schmidt and H. D. Lutz, Physics and Chemistry of Minerals, 1993, 20, 27. [Pg.560]

The first is a simple list of three integers, and the second is a list of lists, each of which is a simple list of three integers. The parentheses serve to enclose the lists. Such lists ideally match the permutation notation for group operations which are employed in these programs. For example, to represent the permutation of the integers 1 and 2 in a list of integers (123) one writes. [Pg.177]

To verify that the product formula for characters holds even for functions that transform according to representations of higher dimensions, suppose that the functions /i, /2 / and gi, g2 . gn form bases for n— and m—dimensional representations of a group. Thus under any group operation A, each fi is transformed into a linear combination of all the fk,k = 1,... n and similarly each gj is transformed into a linear combination of all the gi,l = 1,... n. [Pg.95]

This example suggests the general definition of the character projection operator, Vr, to project out that component of a function which transforms according to irreducihle representation F (The group operations are denoted hy Oj,j = 1,... /t. /i is the number of elements of the group.)... [Pg.114]

The reader shonld note carefully the two different uses of the symbol a here. One is a group operation, the other the state designation of an orbital. [Pg.49]


See other pages where Groups operations is mentioned: [Pg.144]    [Pg.145]    [Pg.147]    [Pg.245]    [Pg.265]    [Pg.992]    [Pg.129]    [Pg.819]    [Pg.623]    [Pg.108]    [Pg.255]    [Pg.325]    [Pg.24]    [Pg.26]    [Pg.58]    [Pg.221]    [Pg.236]    [Pg.419]    [Pg.163]    [Pg.184]    [Pg.42]    [Pg.94]    [Pg.177]    [Pg.197]   
See also in sourсe #XX -- [ Pg.389 ]




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Group theory symmetry operators

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Point Groups and Symmetry Operations

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Point groups operators

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Symmetry operators and point groups

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