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Since the coupling-matrix elements are frequently strongly peaked as a function of the internuclear distance, their direct use in the expansion of the time-dependent Schrödinger equation (2.2) may not be numerically feasible. One customarily performs a unitary transformation from the adiabatic basis to a "diabatic basis" which is defined such that the off-diagonal coupling-matrix elements are zero. In this case, the off-diagonal matrix elements of the Hamiltonian Ĥ are nonzero and cause the coupling between different diabatic states.
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0242460968
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note
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- cluster for the representation of the surface. The zero of energy corresponds to the energy of the ionic state (positive projectile plus neutral surface) at large distance.
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55
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0242713531
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note
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0242713529
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+, we use the cc-pVDZ basis of Ref. [41].
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58
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0242713528
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note
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The identification of the ionic and covalent states is made through the dominant reference configuration in the MR-CI wave function.
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0242460966
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note
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The diabatic curve is approximately constructed from the electron occupation of the different CI configurations. At an avoided crossing, two or several states have strong admixtures of the ionic reference configuration. The diabatic curve of the ionic state connects the two lines that have dominant ionic character on the right/left side of the avoided crossing, respectively.
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