2013
DOI: 10.1103/physreva.88.063829
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Switching on and off of ultrastrong light-matter interaction: Photon statistics of quantum vacuum radiation

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Cited by 73 publications
(88 citation statements)
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“…In cascaded atomic configurations Ξ [36,37], dark states results from interference effects between vacuum and ground state. These coherent superpositions of vacuum and multiphoton states are decoupled from higher energy levels by adiabatic Raman transitions and leads to the generation of virtual two photon excitations between atomic levels [40][41][42][43]. We use Λ structured atomic configuration together with the coupled cavity system and describe the operators η = α 1 +σ x and α 2 as the bright and dark polaritons interacting with coupling strength c 2 .…”
Section: B Input-output Theory and Effective Modelmentioning
confidence: 99%
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“…In cascaded atomic configurations Ξ [36,37], dark states results from interference effects between vacuum and ground state. These coherent superpositions of vacuum and multiphoton states are decoupled from higher energy levels by adiabatic Raman transitions and leads to the generation of virtual two photon excitations between atomic levels [40][41][42][43]. We use Λ structured atomic configuration together with the coupled cavity system and describe the operators η = α 1 +σ x and α 2 as the bright and dark polaritons interacting with coupling strength c 2 .…”
Section: B Input-output Theory and Effective Modelmentioning
confidence: 99%
“…Different from the generic models [36,37], spontaneous emergence of synchronization [27,52] in the presence of virtual photon conversion [40][41][42][43] makes our model advantageous in coupled cavity systems for switching and sending photons. When the single photon gate field is sent to the coupled cavity system, the incoming field is split into two fields incident both on the left and right cavities by time-reversed process of single-photon generation.…”
Section: B Photon Blockade and Input/output Theorymentioning
confidence: 99%
“…Optomechanics experiments are rapidly approaching the ultrastrong (or single-photon) coupling regime [6,[22][23][24], where the radiation pressure of a single photon displaces the mechanical resonator by more than its zero-point uncertainty [25]. This regime is attracting great interest also in cavity QED because it can give rise to novel quantum effects [26][27][28][29][30]. Realizing this ultrastrong coupling (USC) regime in optomechanical systems will facilitate the creation of quantum mechanical states of the mechanical resonator, as well as the characterization of such states by measuring the cavity photon field [23,25].…”
Section: Introductionmentioning
confidence: 99%
“…The framework here presented is an example of how the USC regime can favor the generation and control of mechanical quantum states. Moreover, the proposed strategy can be applied to other systems such as trapped ions [39] and and cavity QED into the USC regime [26,29,40,41],…”
Section: Introductionmentioning
confidence: 99%
“…However, the ground state can not emit energy, so the output photon flux can not be proportional to á ñ † a a , as in standard input-output theory. Instead, it has been shown [15,40] that the cavity output (which can be detected by a photo-absorber) is proportional to á ñ -+x demonstrates that the photons that contribute to the ground state are not observable physical particles. An analogous situation arises when the photons are coupled to collective matter excitations described by bosonic fields [41].…”
Section: Introductionmentioning
confidence: 99%