2022
DOI: 10.1103/physreva.105.013109
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Blackbody-radiation-induced facilitated excitation of Rydberg atoms in optical tweezers

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Cited by 20 publications
(13 citation statements)
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“…For our parameters and assuming a phase-noise-free laser, we expect a dressed (black-body radiation limited) lifetime of τ dr = 1.7 ms. In contrast, the experimentally observed lifetime is reduced to 70µs (for ∆ ↓ = −2π • 0.6 MHz and Ω ↓ = 2π • 0.4 MHz) due to laser noise [43]. Atom loss due to excitation to Rydberg pair resonances is weak, as shown in Fig.…”
Section: Rydberg Laser Setupmentioning
confidence: 85%
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“…For our parameters and assuming a phase-noise-free laser, we expect a dressed (black-body radiation limited) lifetime of τ dr = 1.7 ms. In contrast, the experimentally observed lifetime is reduced to 70µs (for ∆ ↓ = −2π • 0.6 MHz and Ω ↓ = 2π • 0.4 MHz) due to laser noise [43]. Atom loss due to excitation to Rydberg pair resonances is weak, as shown in Fig.…”
Section: Rydberg Laser Setupmentioning
confidence: 85%
“…We load 39 K atoms into the traps by alternating trapping and cooling light with a frequency of 1.4 MHz [44], one order of magnitude faster than the radial trapping frequency of ω r = 2π • 158 kHz (ω z = 2π • 25 kHz). On average, 50 % of the traps are filled with a single atom [42,43], and the experimental cycle rate is 1 Hz.…”
Section: Experimental Sequencementioning
confidence: 99%
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“…This additional loss could be associated with off-resonant excitation by the near-resonant sideband, depended on the detuning ∆ and the power in the sideband, and was independent of the macrodimer coupling. Possible origins include collective loss channels found in other Rydberg dressing experiments operating at high densities, potentially triggered by black-body radiation [8,29,30], as well as phase noise on the laser [31].…”
Section: (C))mentioning
confidence: 93%
“…Let us finally comment on possible decoherence mechanisms of the hydrogen-like Rydberg states of a given n-manifold. First, radiative decay due to spontaneous emission and black body radiation is a well known source of decoherence in Rydberg experiments [96][97][98]. However, similar to experiments with circular Rydberg states [60,99], black body radiation can be suppressed in a cryogenic environment, while at the same time spontaneous emission is strongly reduced for all states with m l > l * since the primary decay channels to energetically low-lying states are dipole-forbidden (for further details see App.…”
Section: Nonhydrogenic Atoms and The Electron Spinmentioning
confidence: 99%