2021
DOI: 10.1103/physrevlett.126.043602
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Tunable Chiral Bound States with Giant Atoms

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Cited by 127 publications
(94 citation statements)
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“…While the interaction at each atom-field coupling point can still be well described by the dipole approximation, the atoms in these systems can no longer be viewed as points and the phase accumulations of photons between different coupling points should be taken into account. To date, there have been a variety of intriguing phenomena witnessed in giant-atom structures, such as frequency-dependent Lamb shifts and relaxation rates [8], decoherence-free interatomic interactions [9,[11][12][13][14], unconventional bound states [15][16][17][18][19][20][21], and phase-controlled frequency conversions [22,23]. Most recently, giant atoms have also been extended to the nonperturbative regime [24], to chiral quantum optics [12-15, 25, 26], and to synthetic dimensions [27].…”
Section: Introductionmentioning
confidence: 99%
“…While the interaction at each atom-field coupling point can still be well described by the dipole approximation, the atoms in these systems can no longer be viewed as points and the phase accumulations of photons between different coupling points should be taken into account. To date, there have been a variety of intriguing phenomena witnessed in giant-atom structures, such as frequency-dependent Lamb shifts and relaxation rates [8], decoherence-free interatomic interactions [9,[11][12][13][14], unconventional bound states [15][16][17][18][19][20][21], and phase-controlled frequency conversions [22,23]. Most recently, giant atoms have also been extended to the nonperturbative regime [24], to chiral quantum optics [12-15, 25, 26], and to synthetic dimensions [27].…”
Section: Introductionmentioning
confidence: 99%
“…In the past few years, nonchiral giant atoms have been well investigated [54], which demonstrated a series of intriguing interference effects such as frequency-dependent Lamb shift and relaxation rate [55], decoherence-free interatomic interactions [56][57][58], and oscillating bound states [59]. Most recently, the concept of chiral quantum optics has also been brought to giant-atom structures [60][61][62], which shows the possibility of combining the advantages of the two paradigms. Here, we study the nonreciprocal singlephoton frequency conversion of the chiral Λ-type giant atom in both the Markovian and non-Markovian regimes, which are defined depending on whether the propagation time of photons between different atom-waveguide coupling points is negligible or not.…”
Section: Introductionmentioning
confidence: 99%
“…Usually, the photon bound state is exponentially localized and isotropic around the emitter, which limits the form of dipole-dipole interactions [3,4]. However, through properly modifying the photonic bath, photon bound states can be anisotropic [8][9][10][11], power-law scaling [6,7,12], and even phase tunable [13][14][15][16]. These special bound states can be used to study more exotic many-body phases.…”
Section: Introductionmentioning
confidence: 99%