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States participating in dissociative recombination from lower vibrational states of the H + 2 ion (Guberman 1983). The energy is measured from the ground (v = 0) state X 1 + g of the H 2 molecule.

States participating in dissociative recombination from lower vibrational states of the H + 2 ion (Guberman 1983). The energy is measured from the ground (v = 0) state X 1 + g of the H 2 molecule.

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The reaction of dissociative recombination is investigated taking into account the electron and rotation - vibrational coupling. Basic equations are formulated within the framework of the multichannel quantum-defect theory for the collision T-matrix. Combining the rigorous account of nonadiabatic coupling in the closed channels with respect to smal...

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Context 1
... reaction e − + H + 2 following through the stage of the intermediate complex H * * 2 is not well enough studied even for transitions into the low-lying 1 + g dissociative state (see figure 1), because coupling between the scattering and reaction channels is not yet clear. Moreover, information about contributions of the s-, p-and d-orbitals to this reaction needs additional revising. ...
Context 2
... 1983, Hazi et al 1983, Shimamura et al 1990, Schneider et al 1991, 1992, 1994, Takagi 1993a, and the multitude of references cited therein). The potential curve of this state (see figure 1) crosses the ionic term U i (R) near point R * c = 2.65 au placed in the vicinity of the right-hand classical turning point of the first excited vibrational level v = 1. Therefore, the cross section of the reaction ...
Context 3
... small for v i = 0 and rises appreciably as v i increases. Using the pattern of potential curves displayed in figure 1 we can determine the relation between the scattering channels and channels of reaction (44). On account of weak mixing of s-, p-, and d-orbitals, strictly definitive configurations of the intermediate complex H * * 2 should correspond to partial llwaves of incident electrons in the adiabatic representation (Takagi and Nakamura 1983). ...

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... This operator describes the interaction of the electron with the ion core in an isolated Rydberg configuration e À þ XY þ . Electron parts of matrix elements of the t operator in the mixed basis (14) are diagonal with respect to q and K and are expressed via R-de- ...
... Because the adiabatic basis jJMlKvi is related to channel basis (14) through the unitary transformation [14] as ...
... Because the adiabatic basis jJMlKvi is related to channel basis (14) through the unitary transformation [14] as ...
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... On this basis, the states of a two-atomic molecule are classified by the values of J and L; i.e., the electronic angular momentum l is generally not conserved. The basis functions in the Rydberg states (taking into account the vibrational and rotational motions) are [74] JMrLv; AE j i¼ X l a J l rL JMlLv; AE j i ; ...
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