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E/f symmetry

The preceding discussion is focussed on the parity and e/f symmetry of case (a) basis states (Eq. 3.2.4a). Since it is often useful to construct basis sets of the form (ion-core) (Rydberg electron)) where the ion-core can be in cases a+, b+, or c+ and the Rydberg electron can be in cases a, b, c, d, or e (Watson 1999), the effects of cxv(xz) on each of these basis states are summarized here (Field, unpublished) ... [Pg.145]

The 7r2 configuration gives rise to three states, 3E (the lowest state), 1 A, and 1S+ states (see Section 3.2.3). Spin-orbit interaction is possible only between the 3Eq and basis functions that have the same value of fi and the same e/f symmetry (both are e). The other selection rules, AS = 1 and E+ E, are also satisfied. Since AA = AE = 0, only the l2jS2j part of the spin-orbit operator is relevant and, as has been shown in Eq. (3.4.16),... [Pg.201]

For a one-photon, electric dipole transition, the parity selection rule is always + <-> —. In terms of e/f symmetry, Fig. 6.1 illustrates a 1II — 1E+ transition with rotational lines Q/e, Pee, and Ree-... [Pg.359]

Electronic absorption spectra are produced when electromagnetic radiation promotes the ions from their ground state to excited states. For the lanthanides the most common of such transitions involve excited states which are either components of the ground term or else belong to excited terms which arise from the same 4f" configuration as the ground term. In either case the transitions therefore involve only a redistribution of electrons within the 4f orbitals (i.e. f—>f transitions) and so are orbitally forbidden just like d—>d transitions. In the case of the latter the rule is partially relaxed by a mechanism which depends on the effect of the crystal field in distorting the symmetry of the metal ion. However, it has already been pointed out that crystal field effects are very much smaller in the case of ions and they... [Pg.1243]

The last decade has witnessed an unprecedented strengthening of the bone between theory and experiment in organic chemistry. Much of this success may be credited to the development of widely applicable, unifying concepts, such as the symmetry rules of Woodward and Hoffmann, and the frontier orbital thee>ry of Eukui. Whereas the the ore tical emphasis had historically been on detailed structure and spectroscopy, the new methods are de signe d to solve pre)blems e>f special importance to organic chemists reactivity, stereochemistry, and mechanisms. [Pg.312]

As already described in part 2.3.2 for a set of pairs (R, a) (Fig. 3 a) the remaining geometric variables were optimized in keeping with a symmetry restriction (Fig. 3 b). The energy function E = f(R, a) obtained here in the gas phase is presented in Fig. 4 as a graphic representation of isoenergetic lines above the R-a-plane. Tire points marked by Roman numerals are minimas (educts I products III, IV, V) and the saddle... [Pg.218]

Valeev, E. F., Schaefer III, H. F., 1998, The Protonated Water Dimer Brueckner Methods Remove the Spurious C] Symmetry Minimum , J. Chem. Phys., 108, 7197. [Pg.303]

Fig. 4 Cationic structure of 4. a Stereo view of the structure of the octahedron with only two of the vertices, b Ellipsoid and c space-tilling representations of 4. d Huge LngCui2 octahedral core Emcapsulates a CIO anion, e f Coordination environment of Tb3+ and the outer Cu2+ ions in the two vertices. The symmetry codes of a and b are z, x — 1, y+ 1 and y + 1, z — 1, x, respectively. The dashed line represents the weak coordination bonding... Fig. 4 Cationic structure of 4. a Stereo view of the structure of the octahedron with only two of the vertices, b Ellipsoid and c space-tilling representations of 4. d Huge LngCui2 octahedral core Emcapsulates a CIO anion, e f Coordination environment of Tb3+ and the outer Cu2+ ions in the two vertices. The symmetry codes of a and b are z, x — 1, y+ 1 and y + 1, z — 1, x, respectively. The dashed line represents the weak coordination bonding...
Figure 7.2 The different symmetry elements of the center ABg. (a) A trigonal axis, C3 (b) A binary axis, C2. (c) A symmetry axis belonging to both the 6C4 and SCj classes, (d) A symmetry plane, au- (e, f) Two of the six aj, reflection planes, (g) A view down the C3 axis in (a) to show a roto-reflection operation, S. ... Figure 7.2 The different symmetry elements of the center ABg. (a) A trigonal axis, C3 (b) A binary axis, C2. (c) A symmetry axis belonging to both the 6C4 and SCj classes, (d) A symmetry plane, au- (e, f) Two of the six aj, reflection planes, (g) A view down the C3 axis in (a) to show a roto-reflection operation, S. ...
With the prospect for realizing a symmetry restriction based on - S established, it is interesting to consider the possible magnitude of the effect. For 02, J - 5" is a well-defined quantum number with odd and even values corresponding to e and/parity label states respectively. The e/f notation refers to the... [Pg.176]

A summary of the symmetry analysis for the various isotopomers is presented in Table 5 where, in keeping with the conclusions of the general analysis, only ground vibrational states of the reactants are considered. Inspection of Table 5 indicates that isotopic substitution that preserves the CO2 centrosymmetry lifts the restriction based on I while preserving the restriction based on the e parity label state. Because C substitution will always preserve molecular centrosymmetry, the symmetry analysis predicts that ( 02)2 clusters containing a C isotope could show at most a formation-rate enhancement of a factor of two above that of (002)2- Also, because this symmetry restriction is independent of the detailed nature of the quantum states of the COj ions, the C SIKIE is predicted to be independent of the way in which the ion is prepared (i.e., E. Conversely, Table 5 indicates that when the COj centrosymmetry is removed, there are no symmetry restrictions to cluster formation. The extent to which the formation of (002)2 containing a ion will be enhanced above that of ( 62)2 depends on the e/f parity label state distribution of the CO2 ions, which, as was demonstrated in the O2/O2 study,can depend on E. ... [Pg.182]

Two important conclusions can be drawn from the simunary of the symmetry analysis of Ar/CO collisions in Table 6. First, no SIKIE is predicted for C substitution because the symmetry of the system is independent of the isotope of carbon involved. Second, because the predicted a based symmetry restrictions for Ar COj cluster formation are identical to those predicted for (002)2, dependence of the magnitude of observed 0 SIKIE on the conditions of CO2 formation is expected. However, the e/f parity label state propensities for El-produced COJ, inferred from 0 SIKIE in (COj) formation, are not sufficient to predict the magnitude of 0 SIKIE in Ar-COj formation because, for above the threshold for Ar formation, COj ions are also produced by the charge-transfer reaction,... [Pg.186]

For simplicity, we add noise in the form of a white noise E,(f) to the third equation of system (42), preserving the original system symmetry. [Pg.515]

The last Eq. (2.66) implies that the mapping on the right hand side generates merely a permutation of the coordinate vectors, i.e. F (F) must be a covering operation of the NC (Xk( F), Zk, Mk. One therefore may state that every fixed point is connected to a covering symmetry operation not contained in ( ). If F E JF"( ) is an isometric transformation with fixed point, then also the period of F... [Pg.20]

Fig. 3. Conformation of the switch-2 cluster and neck linker/neck region in various members of the kinesin superfamily. The upper four panels (A, B, E, F) show crystal structures of N-type kinesins with their motor domain at the N-terminus and the neck at the C-terminus. (C), (D), (G), and (H) show C- and M-type kinesins with their neck N-terminal to the motor domain, except for PoKCBP (G) where the C-terminal neck mimic is shown instead of the N-terminal neck (which is not included in the crystal structure). Each structure is shown in two orientations that differ by a rotation of 90 degrees. Rat conventional kinesin (RnKHC [A]) has been chosen to define standard orientations with the neck helix a7 parallel/perpendicular to the drawing area. Orientations for the other structures have been determined by least-squares superposition of their P-loop regions with that of RnKHC (using 11 Ca-atoms of residues F83-T93 in RnKHC). (B), (C), and (D) show the structures of dimeric constructs with the second motor domain in pale colors. The Ned structure in (C) is 180-degree symmetric the symmetry axis is oblique to the drawing plane and coincides with the axis of the coiled-coil that is formed by the two neck helices. In the asymmetric structure of the Ned N600K mutant (D), the second motor domain (pale) is rotated by about 75 degrees around an axis perpendicular to the coiled-coil. The structures shown in (A), (B), (F), and (G) have their switch-2 cluster in permissive conformation, whereas the conformation of structures (C), (D), (E), and (H) is obstructive, as can be told by observing the slope of the extended switch-2 helix a4. Color code red, switch-2 cluster including the extended... Fig. 3. Conformation of the switch-2 cluster and neck linker/neck region in various members of the kinesin superfamily. The upper four panels (A, B, E, F) show crystal structures of N-type kinesins with their motor domain at the N-terminus and the neck at the C-terminus. (C), (D), (G), and (H) show C- and M-type kinesins with their neck N-terminal to the motor domain, except for PoKCBP (G) where the C-terminal neck mimic is shown instead of the N-terminal neck (which is not included in the crystal structure). Each structure is shown in two orientations that differ by a rotation of 90 degrees. Rat conventional kinesin (RnKHC [A]) has been chosen to define standard orientations with the neck helix a7 parallel/perpendicular to the drawing area. Orientations for the other structures have been determined by least-squares superposition of their P-loop regions with that of RnKHC (using 11 Ca-atoms of residues F83-T93 in RnKHC). (B), (C), and (D) show the structures of dimeric constructs with the second motor domain in pale colors. The Ned structure in (C) is 180-degree symmetric the symmetry axis is oblique to the drawing plane and coincides with the axis of the coiled-coil that is formed by the two neck helices. In the asymmetric structure of the Ned N600K mutant (D), the second motor domain (pale) is rotated by about 75 degrees around an axis perpendicular to the coiled-coil. The structures shown in (A), (B), (F), and (G) have their switch-2 cluster in permissive conformation, whereas the conformation of structures (C), (D), (E), and (H) is obstructive, as can be told by observing the slope of the extended switch-2 helix a4. Color code red, switch-2 cluster including the extended...

See other pages where E/f symmetry is mentioned: [Pg.186]    [Pg.144]    [Pg.146]    [Pg.362]    [Pg.403]    [Pg.404]    [Pg.440]    [Pg.440]    [Pg.186]    [Pg.144]    [Pg.146]    [Pg.362]    [Pg.403]    [Pg.404]    [Pg.440]    [Pg.440]    [Pg.227]    [Pg.777]    [Pg.684]    [Pg.95]    [Pg.200]    [Pg.36]    [Pg.14]    [Pg.185]    [Pg.187]    [Pg.247]    [Pg.26]    [Pg.71]    [Pg.303]    [Pg.20]    [Pg.192]    [Pg.629]    [Pg.528]    [Pg.550]    [Pg.32]    [Pg.212]    [Pg.303]    [Pg.110]    [Pg.110]    [Pg.110]    [Pg.245]    [Pg.137]   
See also in sourсe #XX -- [ Pg.139 ]




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