2000
DOI: 10.1039/b002675l
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Boltzmann wavepacket dynamics of tunnelling of molecules through symmetric and asymmetric energy barriers on non-periodic potential functions

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Cited by 8 publications
(16 citation statements)
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References 11 publications
(7 reference statements)
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“…Eigenfunctions (4) and energies of the corresponding time-independent states are determined by diagonalization of the Hamiltonian matrix (2).…”
Section: Methodsmentioning
confidence: 99%
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“…Eigenfunctions (4) and energies of the corresponding time-independent states are determined by diagonalization of the Hamiltonian matrix (2).…”
Section: Methodsmentioning
confidence: 99%
“…It has a significant influence on the structure of molecular spectra [1]. A dynamic description of the tunneling process is more complete than the traditional solution of the steady-state Schrödinger equation because it can follow in detail the evolution of fragments of the molecular system and its coupling with the variable electromagnetic field of a light wave.The dynamics of wavepackets tunneling through potential barriers, their coupling with external fields, and the effect of asymmetry in the potential function on the formation and structure of vibrational spectra have recently been widely studied [2][3][4][5][6][7][8][9]. However, most of these studies [2, 4, 6-9] are dedicated to tunneling in a non-periodic potential, a typical example of which is the inversion potential of ammonia.…”
mentioning
confidence: 99%
“…6 Results and discussion Fig.1 shows that the parameters of the potential (2) can be chosen to provide good description of the energy levels structure for a set of specific experimental data. In Fig.1 the energy levels for the inversion of the ammonia molecule NH 3 (experimental data determined with help of microwave and IR spectroscopy are taken from [7], [32]) are presented. The energy levels for the inversion mode of NH 3 form a pair of doublets within the wells.…”
Section: Symmetric Potentialmentioning
confidence: 99%
“…The energy levels for the inversion mode of NH 3 form a pair of doublets within the wells. For the ground-state splitting the values E 1 − E 0 = 0.66 ÷ 0.8 cm −1 are given in the literature [32], [7], [8]. To be specific we choose the value E 1 − E 0 = 0.76 cm −1 .…”
Section: Symmetric Potentialmentioning
confidence: 99%
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