2010
DOI: 10.1088/1367-2630/12/9/093023
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Manipulation of quantum state transfer in cold Rydberg atom collisions

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Cited by 17 publications
(24 citation statements)
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“…Figure 5 shows the time-resolved ion signal for 63S 1/2 at a dc electric field of ε = 267 mV/cm and a fixed delay time of 6 µs. A possible explanation is that the electric field induces nonadiabatic transition by forming energy crossings,and the influence of the dc Stark effect on the nonadiabatic multichannel decay of quasimolecules has been investigated [27]. The other possible reason is that pairs of 63S 1/2 states are energetically degenerate with closer attractive pairs states for certain electric fields, and the electric field leads to l and n mixing between dipole-dipole coupled states.…”
Section: Resultsmentioning
confidence: 99%
“…Figure 5 shows the time-resolved ion signal for 63S 1/2 at a dc electric field of ε = 267 mV/cm and a fixed delay time of 6 µs. A possible explanation is that the electric field induces nonadiabatic transition by forming energy crossings,and the influence of the dc Stark effect on the nonadiabatic multichannel decay of quasimolecules has been investigated [27]. The other possible reason is that pairs of 63S 1/2 states are energetically degenerate with closer attractive pairs states for certain electric fields, and the electric field leads to l and n mixing between dipole-dipole coupled states.…”
Section: Resultsmentioning
confidence: 99%
“…The Coulomb potential frequently appears in studies of nonadiabatic transitions in molecular physics [1,15,19]. Moreover, if one of the levels is degenerate before a molecular collision or an application of a time-dependent field, this degeneracy experiences fan-like spitting, as in Rydberg's atoms due to the Stark effect [20]. Hence, the LZC-model represents an important class of processes in atomic and molecular physics.…”
mentioning
confidence: 99%
“…As we have shown in our recent work [17], this is strong evidence that a two-body interaction dominates the dynamics. We show that the multistate nature of the Rydberg atom pair interaction potentials [15,18,19] can be used to explain the observed line broadening while maintaining consistency with the quadratic scaling of the product yield with Rydberg state population. The explanation of the line broadening spectra at high densities requires that a Rydberg atom blockade be taken into account [20,21], but does not require the introduction of more than a two-body interaction between a pair of atoms.…”
mentioning
confidence: 66%
“…σ is the spectral linewidth including the laser linewidth and the linewidth of 5P 3/2 . P pair is the pair-state correlation function [18]. At the laser intensities and densities used in the experiment, saturation must be considered.…”
mentioning
confidence: 99%