2013
DOI: 10.1103/physreva.88.063644
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Source of entangled atom pairs on demand using the Rydberg blockade

Abstract: Two ultracold atom clouds, each separately in a dipole-blockade regime, realize a source of entangled atom pairs that can be ejected on demand. Entanglement generation and ejection is due to resonant dipole-dipole interactions, while van-der-Waals interactions are predominantly responsible for the blockade that ensures the ejection of a single atom per cloud. A source of entangled atoms using these effects can operate with a 10kHz repetition rate producing ejected atoms with velocities of about 0.5m/s.

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Cited by 12 publications
(16 citation statements)
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References 68 publications
(72 reference statements)
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“…Similar decoherence effects in chemistry might arise for large bond lengths with atypically dense solvents. Our results also open up a research arena on the influence of tunable decoherence on energy transport and atomic motional dynamics in flexible Rydberg aggregates [14,15,[57][58][59] embedded in host atom clouds [67,68]. Additionally, we have shown how temporally localized decoherence pulses can be used as an incoherent means of population redistribution among BO surfaces.…”
mentioning
confidence: 55%
“…Similar decoherence effects in chemistry might arise for large bond lengths with atypically dense solvents. Our results also open up a research arena on the influence of tunable decoherence on energy transport and atomic motional dynamics in flexible Rydberg aggregates [14,15,[57][58][59] embedded in host atom clouds [67,68]. Additionally, we have shown how temporally localized decoherence pulses can be used as an incoherent means of population redistribution among BO surfaces.…”
mentioning
confidence: 55%
“…One way to improve the fidelity of our scheme is searching for suitable Rydberg states with longer lifetime. As in Rost's work [18], a higher fidelity is obtained in the timescale of a few µs with strong and short pulses; however it does not work here because we need to follow the evolution of a quasi-dark eigenstate that means a longer pulse duration will lead to better adiabaticity. So the decay rates of intermediate states must be an obstacle for the performance of the scheme.…”
Section: Fidelity Of Adiabatic Passagementioning
confidence: 96%
“…Note that ω ≫ Ω max (the peak value of Ω(t)) is always kept. Comparing to [18] where the required shapes of microwave and detuning pulses are relatively complicated, the pulses needed in our scheme are more flexible that only should satisfy the adiabatic evolution of |λ a 0 (t) . Based on the analytical expressions of eigenvalues |λ a 0 (t) and |λ a 1 (t) [see Eqs.…”
Section: Chirped Adiabatic Passagementioning
confidence: 99%
“…Further analysis reveals that the underlying exciton state | ϕ rep (R) is adiabatically preserved due to the relatively slow motion R(t) of the atoms. In this scenario, the coherent excitation transport also implies entanglement transport, which could be measured through Belltype inequalities [109]. An additional combination of repulsive van-der-Waals and attractive dipole-dipole interactions can modify exciton states at short distances and form aggregates of actually up to 6 atoms bound in one dimension, enabling studies of their dissociation [43].…”
Section: Adiabatic Excitation Transportmentioning
confidence: 99%