2018
DOI: 10.1063/1.5034066
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Multi-contact switch using double-dressing regularity of probe, fluorescence, and six-wave mixing in a Rydberg atom

Abstract: In this paper, we study the realization of a multi-contact switch using the double-dressing regularity of probe, fluorescence, and six-wave mixing signals in a five-level Rb atomic system. For the first time, we compare the dressing regularity of Rydberg states by observing electromagnetically induced transparency and signals. With the scanning probe and dressing fields, both large and small line shifts in signals are observed. The small line shifts are induced by double-dressed line shifts. Also, the big line… Show more

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Cited by 8 publications
(7 citation statements)
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“…In experiment, the laser beams required in this protocol can be derived from external cavity semiconductor lasers (ECDLs), which are applied in many experimental schemes related to Rydberg atom. [67][68][69] The coupled Rabi frequencies of the lasers and the corresponding transitions are Ω i = 𝜇 i E i ∕ℏ, where 𝜇 i is the electronic dipole moment between different energy levels, 𝜇 i ∝ √ 3𝜀 0 ℏ𝜆 3 (2J ′ + 1)∕32𝜋 4 𝜏(2J + 1); 𝜏 ∝ n 3 is the lifetime of energy level; E i is the electric field intensity of laser beam i. We can conclude that Ω i ∝ n −3∕2 .…”
Section: Rydberg State and Laser Beam Considerationsmentioning
confidence: 99%
See 1 more Smart Citation
“…In experiment, the laser beams required in this protocol can be derived from external cavity semiconductor lasers (ECDLs), which are applied in many experimental schemes related to Rydberg atom. [67][68][69] The coupled Rabi frequencies of the lasers and the corresponding transitions are Ω i = 𝜇 i E i ∕ℏ, where 𝜇 i is the electronic dipole moment between different energy levels, 𝜇 i ∝ √ 3𝜀 0 ℏ𝜆 3 (2J ′ + 1)∕32𝜋 4 𝜏(2J + 1); 𝜏 ∝ n 3 is the lifetime of energy level; E i is the electric field intensity of laser beam i. We can conclude that Ω i ∝ n −3∕2 .…”
Section: Rydberg State and Laser Beam Considerationsmentioning
confidence: 99%
“…[67] The mapping signals of strong vdW interactions induced Rydberg blockade information and three coexisting EIT windows based on Rydberg blockade have been observed in experiment. [68] Moreover, in the scheme, [69] by observing EIT and signals in the dressing regularity of a five-level 85 Rb atomic system, the dressing regularity of Rydberg states has been compared, and the regularity can be used to realize multi-contact switch. On the other hand, the experimental EIT process studied well in refs.…”
Section: Rydberg State and Laser Beam Considerationsmentioning
confidence: 99%
“…We solve the density-matrix equations and get elements (0) ,… (3) step by step. [28] The third-order nonlinear susceptibility…”
Section: Biphotons Temporal Correlation In the Photon Coincidence Coumentioning
confidence: 99%
“…We solve the density‐matrix equations and get elements ρ (0) ,… ρ (3) step by step. [ 28 ] The third‐order nonlinear susceptibility χaS2false(3false) and χaS3false(3false) of SFWM 1 and SFWM 2 can be χaS2/3(3)=Nμ13μ23μ24μ14ε03false(Δ1iΓ31false)δ2/3inormalΓ21d2/3D2/3where d 2 and D 2 are the terms of χaS2false(3false), d 3 and D 3 are the terms of χaS3false(3false); N is atomic density; μ ij are the electric dipole matrix elements; ε 0 is the vacuum permittivity; ℏ is Planck constant; ∆ i = ω ij − ω i is detuning defined as the difference between the resonant transition frequency ω ij and laser frequency ω i of E i ; Γ ij = ( Γ i + Γ j )/2 is the decoherence rate between | i > and | j >; δ i represents the deviations window around the corresponding central frequency ϖ Si of generated photons, and therefore, ω Si can be written as ω Si = ϖ Si + δ i ( i = 1, 2, 3) with | δ i |≪ ω Si . When we only consider the strong dressing effect of E 2 , the terms d 2/3 and D 2/3 can express as d 2/3 = | Ω 2 2 |/( δ 2/3 + Δ 2 − i Γ 41 ); D 2 = δ 2 + Δ 2 − i Γ 41 ; D 3 = δ 3 + Δ 3 − i Γ 41 ; Ω i = μ ij E i /ℏ is the Rabi frequency.…”
Section: Biphotons Temporal Correlation In the Photon Coincidence Coumentioning
confidence: 99%
“…In recent years, metallo-organic coordination polymers have attracted considerable interest due to their diverse structures and potential applications in fluorescence, magnetic materials, gas adsorption, catalysis and medicine and so forth. [1][2][3][4][5][6] The synthesis of coordination polymers with specific functions has gradually become a research hotspot in the field of material chemistry. 7 From the perspective of crystal engineering, the most useful and facile way to construct coordination complexes is to adopt a suitable ligand to connect metal centers.…”
Section: Introductionmentioning
confidence: 99%