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Conical intersections energy parameters

Table 8-1. S, energy and Cremer-Pople parameters for the ring puckering conical intersections in aminopyrimidine, pyridone and pyrrole. Energies relative to the S0 energy in the ground state equilibrium geometry. The values in parenthesis are the CP parameters for the equivalent MXSs in 9H-adenine using the geometries given in [5]... Table 8-1. S, energy and Cremer-Pople parameters for the ring puckering conical intersections in aminopyrimidine, pyridone and pyrrole. Energies relative to the S0 energy in the ground state equilibrium geometry. The values in parenthesis are the CP parameters for the equivalent MXSs in 9H-adenine using the geometries given in [5]...
Fig. 3 First-order conical intersection picture plot of the 3-coordinate model potential energy surface (3) along coordinates and Q 2 (a) and and (b). Parameter values a = b = c = 0.2 a = 0.2 p = 0.25... Fig. 3 First-order conical intersection picture plot of the 3-coordinate model potential energy surface (3) along coordinates and Q 2 (a) and and (b). Parameter values a = b = c = 0.2 a = 0.2 p = 0.25...
Reactions in which structural change is simultaneously occurring in more than one structural parameter can be depicted as interaction between surfaces with coordinates described by the structural parameters. For many photochemical reactions it has been found that transfer from an excited to a ground state involves a conical intersection (Cl), which can be thought of as a funnel that permits transition from one energy surface (state) to another. The efficiency of the transformation depends on the structural similarity between the excited state and the corresponding ground state molecular ensemble. There can be a number of CIs for the excited states of a typical polyatomic molecule. The transition occurs without luminescence. Conical... [Pg.1079]

In Eqs. (54c) and (69), the parameters s, g and h are used to determine the energies and derivative couplings near a point of conical intersection. Below we compare these perturbative results with those of ab initio calculations at (trans, p, 2.95). Figures 4 depicts the g h plane for this point. From this figure it is seen that the coupling mode, y, has a" synunetry and therefore is the unique internal a" coordinate. The tuning mode x has a symmetry and tends to decrease i (C-N) and increase ZNCO. [Pg.88]

Fig. 7. The excited-state reaction path of the penta-2,4-dienimminium cation intercepts the conical intersection point CI700 located ca. 5 kcal mol above the minimum-energy conical intersection CIq2o. FC— Cl7oo MEP ( i open diamonds and So full diamonds), Cl7oo Cl92o MEP (5i open circles and So full circles). The values of the relevant structural parameters are given in A and degrees. Fig. 7. The excited-state reaction path of the penta-2,4-dienimminium cation intercepts the conical intersection point CI700 located ca. 5 kcal mol above the minimum-energy conical intersection CIq2o. FC— Cl7oo MEP ( i open diamonds and So full diamonds), Cl7oo Cl92o MEP (5i open circles and So full circles). The values of the relevant structural parameters are given in A and degrees.
Fig. 20. Schematic representation of the reaction coordinate for tryptophan fluorescence quenching induced by hydrogen transfer and aborted decarboxylation. The electronic nature of the Si surface changes character along the Si path due to two avoided crossings between jSi and S2 The first one occurs between the covalent state and the ionic La state along the reaction coordinate that interconverts the i9i-Min and. Si-Exc minima. The second one occurs between the ionic La state and the biradical Bi, state along the tautomerization coordinate that leads to the excited-state tautomerized form S -Taut. This point does not corresponds to a minimum on the potential-energy surface and it is found that evolution along a decarboxylation coordinate leads to a -Si /-So conical intersection, where efficient radiationless decay to the ground state takes place. The values of the relevant structural parameters are given in A. Data from Ref. 102. Fig. 20. Schematic representation of the reaction coordinate for tryptophan fluorescence quenching induced by hydrogen transfer and aborted decarboxylation. The electronic nature of the Si surface changes character along the Si path due to two avoided crossings between jSi and S2 The first one occurs between the covalent state and the ionic La state along the reaction coordinate that interconverts the i9i-Min and. Si-Exc minima. The second one occurs between the ionic La state and the biradical Bi, state along the tautomerization coordinate that leads to the excited-state tautomerized form S -Taut. This point does not corresponds to a minimum on the potential-energy surface and it is found that evolution along a decarboxylation coordinate leads to a -Si /-So conical intersection, where efficient radiationless decay to the ground state takes place. The values of the relevant structural parameters are given in A. Data from Ref. 102.

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