2017
DOI: 10.1103/physrevlett.118.133604
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Two-Photon Blockade in an Atom-Driven Cavity QED System

Abstract: Photon blockade is a dynamical quantum-nonlinear effect in driven systems with an anharmonic energy ladder. For a single atom strongly coupled to an optical cavity, we show that atom driving gives a decisively larger optical nonlinearity than cavity driving. This enhances single-photon blockade and allows for the implementation of two-photon blockade where the absorption of two photons suppresses the absorption of further photons. As a signature, we report on three-photon antibunching with simultaneous two-pho… Show more

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Cited by 253 publications
(201 citation statements)
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“…blet, indicating a suppression of multiple excitations which is indeed due to a single-photon blockade [86]. On the other hand, the g (2) (0) function of the two-photon QRM is always larger than 1 (super-Poissonian statistics), which is an indication of a higher-photon number in the cavity output field.…”
Section: Qubit Drivingmentioning
confidence: 97%
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“…blet, indicating a suppression of multiple excitations which is indeed due to a single-photon blockade [86]. On the other hand, the g (2) (0) function of the two-photon QRM is always larger than 1 (super-Poissonian statistics), which is an indication of a higher-photon number in the cavity output field.…”
Section: Qubit Drivingmentioning
confidence: 97%
“…out < 1 (threephoton correlation function) [86]. These conditions indicate two-photon bunching and three-photon antibunching, respectively.…”
Section: Qubit Drivingmentioning
confidence: 98%
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“…In order to account for this effect, we calculate the overlap of the excited states in the sector with n+1 photons with the ground state of the manifold with n photons, f ñ | n . First of all, we notice that the overlap between the excited states with k quasiparticle excitations of only one type, and the ground state in the neighboring sector, is equal to zero for any number of excitations (k>0): In these expressions one can recognise the overlap between the ground states of adjacent photonic manifolds, given by equation (14).…”
Section: Perspectivesmentioning
confidence: 99%
“…1 , are assisted by matrix elements of the perturbation ¢ H , which are smaller than the one connecting the two ground states. This is shown in the appendix: equations (A5) and (A6) display the matrix elements for the transition between the ground state and these two excited ones, and they should be compared with equation (14), reporting the overlap between ground states. The overlaps involving excited states are always smaller by a factor proportional to increasing powers of f f -+ ( ) tanh n n 1 (a quantity always smaller than one) as higher excited states are considered.…”
Section: Landau-zener (Lz) Theory Of the Photons' Staircasementioning
confidence: 99%