2020
DOI: 10.1103/physreva.101.052508
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Spontaneous emission and energy shifts of a Rydberg rubidium atom close to an optical nanofiber

Abstract: In this paper, we report on numerical calculations of the spontaneous emission rates and Lamb shifts of a 87 Rb atom in a Rydberg-excited state (n 30) located close to a silica optical nanofiber. We investigate how these quantities depend on the fiber's radius, the distance of the atom to the fiber, the direction of the atomic angular momentum polarization, as well as the different atomic quantum numbers. We also study the contribution of quadrupolar transitions, which may be substantial for highly polarizable… Show more

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Cited by 31 publications
(24 citation statements)
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“…We take into account the contributions of electric dipole transitions but neglect the contributions of electric quadrupole transitions. We note that this approximation is valid when the atom is not highly excited and the atom-to-body distance is not too small [38].…”
Section: B Casimir-polder Potential Of a Multilevel Alkali-metal Atommentioning
confidence: 99%
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“…We take into account the contributions of electric dipole transitions but neglect the contributions of electric quadrupole transitions. We note that this approximation is valid when the atom is not highly excited and the atom-to-body distance is not too small [38].…”
Section: B Casimir-polder Potential Of a Multilevel Alkali-metal Atommentioning
confidence: 99%
“…Such effects have been studied for a large number of systems [30,31]. In the particular case of an atom near a nanofiber, the modifications of the radiative decay have been investigated in the context of a two-level atom [32][33][34] as well as a realistic multilevel alkali-metal atom [19,[35][36][37][38]. The shift in the energy level of the atom caused by the presence of the body depends on the position of the atom and is known as the Casimir-Polder potential.…”
Section: Introductionmentioning
confidence: 99%
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“…For example, inside a homogeneous dielectric medium with refractive index n, the spontaneous decay rate Γ med of an atomic dipole equals (Glauber and Lewenstein, 1991;Scheel et al, 1999) Γ med nΓ air (1) to a very good approximation, where Γ air denotes the corresponding free space decay rate. However, deriving the local density of states of the EM field in more complex scenarios, which involves the calculation of the imaginary parts of the dyadic Green's function (Novotny and Hecht, 2006;Scheel and Buhmann, 2008;Bennett and Buhmann, 2020;Stourm et al, 2020), can be computationally challenging. Although such calculations can aid the design of photonic devices, they do not provide much physical intuition.…”
Section: Introductionmentioning
confidence: 99%