Single photon transport properties in coupled cavity arrays nonlocally coupled to a two-level atom in the presence of dissipation

Abstract

Single photon transport properties in coupled cavity arrays nonlocally coupled to a two-level atom in the presence of dissipation * Hai Lian(海 莲) a) , Tan Lei(谭 磊) a)b) † , Feng Jin-Shan(冯金山) a) , Xu Wen-Bin(徐文斌) a) , and Wang Bin(王 彬) a) a)

Scattering of a single photon in a one-dimensional coupled resonator waveguide with a Λ-type emitter assisted by an additional cavity

“…[2,3] Among them, scattering of single photons in a one-dimensional waveguide or coupled resonator waveguide (CRW) is one of the most promising candidates. [4][5][6][7][8][9][10][11][12][13][14][15][16][17][18][19][20] In particular, to realize single photon quantum switching, Sun et al used a two-level atom coupled to a one-dimensional (1D) coupled resonator waveguide to control the coherent transport of a single photon. [21] They also realized a single-photon quantum switch in cross-resonator arrays with a Λ-type atom which is localized in the intersectional resonator using the Fano-Feshbach effect based on the dark state of the Λ-type atom.…”

Controllable double electromagnetically induced transparency in a closed four-level-loop cavity–atom system

“…The interaction of two-level atoms and an optical cavity is the basic physical situation about cavity-QED first introduced by Jaynes and Cummings. [7] It is interesting to extend studies of cavity-QED to the interactions of cavity modes and multilevel atoms, [8,9] such as the intracavity electromagnetically induced transparency (EIT) in three-level or four-level atoms confined in an optical cavity, Fano-type interference in a three-level V-type atom-cavity system, and optical bistability in four-level atoms coupled with an optical cavity. [10][11][12][13][14][15][16] Cavity-QED with atomic systems has been an active area of research during the last few decades.…”

Multiphoton Controllable Transport between Remote Resonators

“…In addition to offering an effective platform to simulate quantum many-body phenomena such as Mott-superfluid and topological effects [33][34][35][36], the CRAs have been previously considered for controllable transport of photons by making use of the photon-atom scattering [22,[37][38][39][40][41]. Despite such substantial developments, prior work on controllable photon transport has typically focused upon either single photons [22,38,[42][43][44] or nearby CRAs [45][46][47][48][49].…”