2004
DOI: 10.1103/physreva.69.043408
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Analytical investigation of one-dimensional Rydberg atoms interacting with half-cycle pulses

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Cited by 23 publications
(34 citation statements)
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“…We have chosen to work with three different values of q, 0.0010, 0.0016 and 0.0020 a.u., and used dotted, solid and dashed lines to represent the corresponding curves for |T n n |. Note that q = 0.0016 a.u., corresponds to qn 2 = 1, a relation often used in the weak electric field limit [6] when only a few neighbouring states are populated. From this figure we see that the curves for |T n n | becomes more and more peaked at the centre (n = 25) and flat on the wings as the value of q decreases.…”
Section: Evolution Of Wave Packets and Related Observablesmentioning
confidence: 99%
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“…We have chosen to work with three different values of q, 0.0010, 0.0016 and 0.0020 a.u., and used dotted, solid and dashed lines to represent the corresponding curves for |T n n |. Note that q = 0.0016 a.u., corresponds to qn 2 = 1, a relation often used in the weak electric field limit [6] when only a few neighbouring states are populated. From this figure we see that the curves for |T n n | becomes more and more peaked at the centre (n = 25) and flat on the wings as the value of q decreases.…”
Section: Evolution Of Wave Packets and Related Observablesmentioning
confidence: 99%
“…In particular, x ii calculated using (5) exhibits an awkward singularity although i|x|i represents a well-defined function. We note that the expression for T n n evaluated in the semiclassical approximation by the method of stationary phase is free from this problem and has been used by Bersons and Veilande [6] to reproduce experimental results of Wetzels et al [9] on the interaction of Rydberg atoms with half-cycle pulses. It is quite straightforward however to derive an exact expression for the transition matrix element that can be used to evaluate the limit in (5) unambiguously for both f = i and f = i.…”
Section: Introductionmentioning
confidence: 96%
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“…transferred to the atom from HCP. For the 1D case, it was derived by Bersons and Veilande [5], although their formula needs to be multiplied by nn :…”
Section: Rydberg Wave Packet Dynamicsmentioning
confidence: 99%
“…The one-dimensional atomic model is an excellent approximation for the Rydberg atom in the extreme Stark states and can faithfully mimic many properties of three--dimensional atoms [5]. Moreover, in this case one can construct an exact analytical expression for the wave packet irrespective of whether it is formed by the impact of a single HCP or two time delayed HCPs [6,7].…”
Section: Introductionmentioning
confidence: 99%