2011
DOI: 10.1134/s1054660x11150163
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Atom state evolution and collapse in ultracold gases during light scattering into a cavity

Abstract: We consider the light scattering from ultracold atoms trapped in an optical lattice inside a cavity.In such a system, both the light and atomic motion should be treated in a fully quantum mechanical way. The unitary evolution of the light-matter quantum state is shown to demonstrate the nontrivial phase dependence, quadratic in the atom number. This is essentially due to the dynamical self-consistent nature of the light modes assumed in our model. The collapse of the quantum state during the photocounting proc… Show more

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Cited by 25 publications
(32 citation statements)
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“…Here, we focus on a system dynamics during a single run of the optical measurement (i.e. the continuous detection of scattered photons), without taking the average (expectation values) over many realizations as we were doing so far [57][58][59][60]. Indeed, the result of a singlerun measurement is important, as it is the first result one obtains in an experiment before the averaging procedure.…”
Section: Single-run Measurements and Measurement-based Preparatiomentioning
confidence: 99%
See 1 more Smart Citation
“…Here, we focus on a system dynamics during a single run of the optical measurement (i.e. the continuous detection of scattered photons), without taking the average (expectation values) over many realizations as we were doing so far [57][58][59][60]. Indeed, the result of a singlerun measurement is important, as it is the first result one obtains in an experiment before the averaging procedure.…”
Section: Single-run Measurements and Measurement-based Preparatiomentioning
confidence: 99%
“…Surprisingly, when δz < 1, the final collapse is even faster than √ τ , due to the discreteness of p(z, m, t) [60]. Measuring the photon number m and time t, one can determine z 1 of a quantum trajectory.…”
Section: A Measurement-induced Number Squeezingmentioning
confidence: 99%
“…This can be achieved using traveling waves as mode functions for the probe and the cavity (i.e. ( ) · = u r e l k r i l ), where the wave vectors k 0 and k 1 are orthogonal, corresponding to the detection of the photons scattered in the diffraction minimum and the operator [66][67][68][69][70]. Alternatively, one can obtain the same spatial mode structure considering standing waves (i.e.…”
Section: Effective Dynamics Of the Macroscopic Spatial Modesmentioning
confidence: 99%
“…Uniting these fields [4,5] broadens both, and goes beyond the cases when either the light or matter are treated classically. Experimental [6][7][8][9][10][11] and theoretical works in this regime have revealed many interesting phenomena, such as the preparation of atomic states and dynamics [12][13][14][15][16][17][18][19], non-destructive measurement [20][21][22][23][24], many-body light-matter entanglement [23], self-organisation, and other new quantum phases [25][26][27][28][29][30][31][32][33][34][35][36].…”
Section: Introductionmentioning
confidence: 99%