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II electronic states

The expressions for the rotational energy levels (i.e., also involving the end-over-end rotations, not considered in the previous works) of linear triatomic molecules in doublet and triplet II electronic states that take into account a spin orbit interaction and a vibronic coupling were derived in two milestone studies by Hougen [72,32]. In them, the isomorfic Hamiltonian was inboduced, which has later been widely used in treating linear molecules (see, e.g., [55]). [Pg.510]

Figure 9. Energy difference (absolute value) between the components of the X II electronic State of HCCS as a function of coordinates p, P2, and y. Curves represent the square root of the second of functions given by Eq. (77) (with e, = —0.011, 2 = 0.013, 8,2 = 0.005325) for fixed values of coordinates p, and P2 (attached at each curve) and variable Y = 4>2 Here y = 0 corresponds to cis-planar geometry and y = 71 to trans-planar geometry. Symbols results of explicit ab initio calculations. Figure 9. Energy difference (absolute value) between the components of the X II electronic State of HCCS as a function of coordinates p, P2, and y. Curves represent the square root of the second of functions given by Eq. (77) (with e, = —0.011, 2 = 0.013, 8,2 = 0.005325) for fixed values of coordinates p, and P2 (attached at each curve) and variable Y = 4>2 Here y = 0 corresponds to cis-planar geometry and y = 71 to trans-planar geometry. Symbols results of explicit ab initio calculations.
Hamiltonian equations, 627-628 perturbative handling, 641-646 II electronic states, 631-633 vibronic coupling, 630-631 ABC bond angle, Renner-Teller effect, triatomic molecules, 611-615 ABCD bond angle, Renner-Teller effect, tetraatomic molecules, 626-628 perturbative handling, 641-646 II electronic states, 634-640 vibronic coupling, 630-631 Abelian theory, molecular systems, Yang-Mills fields ... [Pg.66]

II electronic states, 634-640 theoretical background, 625-626 triatomic molecules, 611-615 pragmatic models, 620-621 Ab initio multiple spawning (AIMS) conical intersection location, 491-492 direct molecular dynamics, 411-414 theoretical background, 360-361 Adiabatic approximation geometric phase theory ... [Pg.66]

Hamiltonian equations, 627-628 II electronic states, 632-633 triatomic molecules, 587-598 minimal models, 615-618 Hartree-Fock calculations ... [Pg.80]

HCCS radical, Renner-Teller effect, tetraatomic molecules, II electronic states, 633-640 H2D molecule, non-adiabatic coupling, two-state molecular system, 107-109 HD2 molecule, permutational symmetry isotopomers, 713-717 potential energy surfaces, 692-694 Heaviside function ... [Pg.80]

II electronic states, 638-640 vibronic coupling, 628-631 triatomic molecules, 594-598 Hamiltonian equations, 612-615 pragmatic models, 620-621 Kramers doublets, geometric phase theory linear Jahn-Teller effect, 20-22 spin-orbit coupling, 20-22 Kramers-Kronig reciprocity, wave function analycity, 201 -205 Kramers theorem ... [Pg.83]

A electronic states, 647—653 II electronic states, 641-646 triatomic molecules, minimal models, 615-618... [Pg.92]

Appendix A Perturbative Handling of the Renner-Teller Effect and Spin-Orbit Coupling in II Electronic States of Tetraatomic Molecules... [Pg.584]

As in the case of II electronic states of tetraatomic molecules, because of generally high degeneracy of zeroth-order vibronic leves only several particular (but important) coupling cases can be handled efficiently in the framework of the perturbation theory. We consider the following particular cases ... [Pg.647]

As is well known, linear molecules represent an exception of the JT theorem. The degeneracy of II electronic states is lifted in second order of the bending amplitude, the degeneracy of A electronic states is lifted in fourth order, etc., see [35-38] for reviews. [Pg.89]

Figure 3. Low-energy vibronic spectrum in a II electronic state of a linear triatomic molecule, computed for various values of the Renner parameter 6 and spin-orbit constant Aso (in cm ). The spectrum shown in the center of figure (e = —0.17, Aso = —37cm ) corresponds to the A II state of NCN [28,29]. The zero on the energy scale represents the minimum of the potential energy surface. Solid lines K = 0 vibronic levels dashed lines K = 1 levels dash-dotted lines K = 2 levels dotted lines K = 3 levels. Spin-vibronic levels are denoted by the value of the corresponding quantum number P P = + S note that S is in this case spin quantum number). Figure 3. Low-energy vibronic spectrum in a II electronic state of a linear triatomic molecule, computed for various values of the Renner parameter 6 and spin-orbit constant Aso (in cm ). The spectrum shown in the center of figure (e = —0.17, Aso = —37cm ) corresponds to the A II state of NCN [28,29]. The zero on the energy scale represents the minimum of the potential energy surface. Solid lines K = 0 vibronic levels dashed lines K = 1 levels dash-dotted lines K = 2 levels dotted lines K = 3 levels. Spin-vibronic levels are denoted by the value of the corresponding quantum number P P = + S note that S is in this case spin quantum number).
In this section, we consider II electronic state (A = 1) of ABBA type molecules. The additional Hamiltonian H is of the form... [Pg.631]

In the lowest order (quadratic) approximation for II electronic states of asymmetrical (ABCD) tetraatomics, the electronic matrix elements (60) have the forms [18,152,153] ... [Pg.634]


See other pages where II electronic states is mentioned: [Pg.492]    [Pg.492]    [Pg.517]    [Pg.92]    [Pg.92]    [Pg.93]    [Pg.95]    [Pg.95]    [Pg.100]    [Pg.100]    [Pg.103]    [Pg.106]    [Pg.286]    [Pg.583]    [Pg.584]    [Pg.590]    [Pg.599]    [Pg.600]    [Pg.600]    [Pg.625]    [Pg.635]    [Pg.349]    [Pg.311]    [Pg.314]    [Pg.138]    [Pg.27]    [Pg.29]    [Pg.2]    [Pg.583]    [Pg.584]    [Pg.599]    [Pg.600]    [Pg.600]    [Pg.616]    [Pg.625]   
See also in sourсe #XX -- [ Pg.634 , Pg.635 , Pg.636 , Pg.637 , Pg.638 , Pg.639 ]




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