2020
DOI: 10.1103/physrevlett.125.253601
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Subradiant Emission from Regular Atomic Arrays: Universal Scaling of Decay Rates from the Generalized Bloch Theorem

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Cited by 37 publications
(19 citation statements)
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“…A similar idea of studying a (different) simpler Hamiltonian was recently used to prove a universal power-law scaling of the decay rates of the singly-excited subradiant states [37]. As in [37] we shall validate our solution by treating the difference between the exact H eff and the approximate H 1 as a perturbation, ∆H = H eff − H 1 , which can also be written in the form of Eq. ( 2) with a dispersion relation δω(k) = ω eff (k) − ω 1 (k).…”
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confidence: 87%
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“…A similar idea of studying a (different) simpler Hamiltonian was recently used to prove a universal power-law scaling of the decay rates of the singly-excited subradiant states [37]. As in [37] we shall validate our solution by treating the difference between the exact H eff and the approximate H 1 as a perturbation, ∆H = H eff − H 1 , which can also be written in the form of Eq. ( 2) with a dispersion relation δω(k) = ω eff (k) − ω 1 (k).…”
mentioning
confidence: 87%
“…Moreover, it implies the existence of free-fermion states with finite decay rates and properties that may hence be observed in the emitted field, which is not an attractive option for the previously discovered subradiant free-fermion states [3][4][5]. Dispersion relations with a higher power law leads to even more subradiant states [37], but they correspond to interacting fermions and do not follow the free-fermion ansatz.…”
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confidence: 97%
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“…The use of optical metasurfaces in quantum technologies still requires a better understanding of their cooperative optical behavior [15,16]. Previous works on cooperative optical phenomena have focused mainly on spontaneous emission effects such as subradiance, superradiance, directional scattering and subradiant excitations [17][18][19][20][21][22][23][24][25][26][27][28][29][30]. These works assume that the photons emitted by the atoms can be distinguished from the photons of the driving laser field.…”
Section: Introductionmentioning
confidence: 99%
“…the distribution of complex momentum κ, parameterized by β k ≡ e ikL0 , on a complex plane [4,6]. To this end, we construct a Bloch state for a complex momentum as a traveling wave Ψκ = (1/ √ N ) N l=1 (β κ ) lb l , obeying, under Hamiltonian (4), the equation of motion [19,38,39]. The dispersion relation…”
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confidence: 99%