Steering the Nuclear Motion in Singly Ionized Argon Dimers with Mutually Detuned Laser Pulses

dc.citation.doi10.1103/PhysRevLett.110.033005
dc.citation.issn0031-9007
dc.citation.issue3
dc.citation.jtitlePhysical Review Letters
dc.citation.volume110
dc.contributor.authorWu, J.
dc.contributor.authorMagrakvelidze, M.
dc.contributor.authorVredenborg, A.
dc.contributor.authorSchmidt, L. Ph. H.
dc.contributor.authorJahnke, T.
dc.contributor.authorCzasch, A.
dc.contributor.authorDörner, R.
dc.contributor.authorThumm, U.
dc.date.accessioned2023-12-07T22:12:08Z
dc.date.available2023-12-07T22:12:08Z
dc.date.issued2013-01-18
dc.date.published2013-01-18
dc.description.abstractWe demonstrate that the vibrational nuclear motion of singly ionized argon dimers can be controlled with two ultrashort laser pulses of different wavelengths. In particular, we observe a striking “gap” in the pump-probe-delay-dependent kinetic-energy release spectrum only if the probe-pulse wavelength exceeds the pump-pulse wavelength. This “frustrated dissociation effect” is reproduced by our two-state quantum mechanical model, validating its interpretation as a pump-pulse-initiated population transfer between dipole-coupled Born-Oppenheimer electronic states of the dissociating Ar+2 molecular ion. Our numerical results also reproduce the measured collapse and fractional revival of the oscillating Ar+2 nuclear wave packet, and, for single-pulse dissociation, the decrease of the kinetic-energy release with increasing laser wavelength.
dc.identifier.urihttps://hdl.handle.net/2097/43909
dc.relation.urihttps://link.aps.org/doi/10.1103/PhysRevLett.110.033005
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dc.titleSteering the Nuclear Motion in Singly Ionized Argon Dimers with Mutually Detuned Laser Pulses
dc.typeText

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