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Positive width function and energy indeterminacies in ammonia molecule

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dc.contributor.author Douvropoulos, TG en
dc.date.accessioned 2014-03-01T02:44:55Z
dc.date.available 2014-03-01T02:44:55Z
dc.date.issued 2007 en
dc.identifier.issn 0020-7608 en
dc.identifier.uri https://dspace.lib.ntua.gr/xmlui/handle/123456789/32018
dc.subject Action en
dc.subject Ammonia en
dc.subject Complex poles en
dc.subject Double well en
dc.subject Energy variations en
dc.subject Inversion frequency en
dc.subject Positive width function en
dc.subject Tunneling en
dc.subject Tunneling time en
dc.subject Turning points en
dc.subject.classification Chemistry, Physical en
dc.subject.classification Mathematics, Interdisciplinary Applications en
dc.subject.classification Physics, Atomic, Molecular & Chemical en
dc.subject.other Eigenvalues and eigenfunctions en
dc.subject.other Electron tunneling en
dc.subject.other Energy conservation en
dc.subject.other Energy gap en
dc.subject.other Green's function en
dc.subject.other Nitrogen en
dc.subject.other Semiconductor quantum wells en
dc.subject.other Complex poles en
dc.subject.other Double well en
dc.subject.other Energy indeterminacies en
dc.subject.other Energy spectrum en
dc.subject.other Inversion frequency en
dc.subject.other Path integral theory en
dc.subject.other Positive width function en
dc.subject.other Tunneling time en
dc.subject.other Ammonia en
dc.title Positive width function and energy indeterminacies in ammonia molecule en
heal.type conferenceItem en
heal.identifier.primary 10.1002/qua.21243 en
heal.identifier.secondary http://dx.doi.org/10.1002/qua.21243 en
heal.language English en
heal.publicationDate 2007 en
heal.abstract A recently published methodology based on the semiclassical path integral theory was applied in a double well structure and gave the analytic form of the system's Green's function. This type of potential can describe the ammonia molecule as far as the motion of the nitrogen atom perpendicular to the hydrogen plane is discussed. Because of the fact that a double well describes a bound system and correspondingly stationary states (constructed by the symmetric and antisymmetric superposition of the eigenstates of the two unperturbed wells), it was expected that the energy spectrum would be real, in a form of doublets due to the splitting effect that takes place. However, the result was a pair of complex poles, which had a clearly positive imaginary part for each member. The present work explains the role of the imaginary parts of the complex poles as the decay rate of quantities defined as the energy indeterminacies, which are directly related to the fact that energy is not well determined in a classically forbidden region of motion. These quantities come as a function of (d kappa)/dE, which is the derivative of the classical action inside the potential barrier, with respect to energy. The major contribution comes from the turning points, and then the imaginary parts are responsible, not only for the conservation of energy, but for the correct sign of time as well. In this way, a different approach for the tunneling process is adopted, in which the entry or exit of the particle from the potential barrier takes place inside a neighborhood of the turning point, as though the latter was broadened and fluctuating. The magnitude of the previously mentioned decay rate is equal to omega/pi, where omega is the frequency of the classical oscillations inside one well. In contrast, the inversion frequency is generated by the part of the complex pole that is unrelated to (d kappa)/dE and is much smaller in magnitude than the classical frequency, since it is given as omega/pi exp(-kappa). In this way, the period of the energy fluctuations is much smaller than the internal period of the system produced by the oscillating communication of the two classically allowed regions of motion. (c) 2006 Wiley Periodicals, Inc. en
heal.publisher WILEY-BLACKWELL en
heal.journalName International Journal of Quantum Chemistry en
dc.identifier.doi 10.1002/qua.21243 en
dc.identifier.isi ISI:000245839300003 en
dc.identifier.volume 107 en
dc.identifier.issue 8 en
dc.identifier.spage 1673 en
dc.identifier.epage 1687 en


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