2015
DOI: 10.1103/physrevb.92.035305
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Robust platform for engineering pure-quantum-state transitions in polariton condensates

Abstract: We report on pure-quantum-state polariton condensates in optical annular traps. The study of the underlying mechanism reveals that the polariton wavefunction always coalesces in a single purequantum-state that, counter-intuitively, is always the uppermost confined state with the highest overlap to the exciton reservoir. The tunability of such states combined with the short polariton lifetime allows for ultrafast transitions between coherent mesoscopic wavefunctions of distinctly different symmetries rendering … Show more

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Cited by 63 publications
(78 citation statements)
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“…Using a non-resonant continuous wave (CW) linearly polarized pump spatially shaped in the form of an annular ring and focused on the sample surface through a 0.4 numerical aperture (NA) objective, we create the Ψ 00 coherent state in the optically induced trap, as shown schematically in Fig.1a [29]. The S + and S − components of the emission below and above threshold are resolved with the use of a λ/4 wave-plate and a linear polariser and are then used to reconstruct a real space image of the S z stokes component [30].…”
Section: Resultsmentioning
confidence: 99%
“…Using a non-resonant continuous wave (CW) linearly polarized pump spatially shaped in the form of an annular ring and focused on the sample surface through a 0.4 numerical aperture (NA) objective, we create the Ψ 00 coherent state in the optically induced trap, as shown schematically in Fig.1a [29]. The S + and S − components of the emission below and above threshold are resolved with the use of a λ/4 wave-plate and a linear polariser and are then used to reconstruct a real space image of the S z stokes component [30].…”
Section: Resultsmentioning
confidence: 99%
“…Numerous examples of these interactions have been studied, ranging from polariton condensate interacting with an exciton reservoir in nonresonant excitation experiments [44][45][46][47][48][49] to spinor interactions in resonant [50][51][52][53][54][55] or nonresonant excitation [56,57]. They are, however, different in nature from the spinor effects induced by the effective magnetic field caused by TE-TM splitting of the microcavity mode [58][59][60] or by the birefringence field induced by disorder [61,62].…”
Section: Theoretical Modelmentioning
confidence: 99%
“…1(b,c)] and real-space images of the spatial probability distribution for the exciton-polariton condensate, as seen in Figs 1, 2 and 3. Above the threshold pump power, exciton-polaritons occupy multiple eigenstates of the optically defined trap222428293032 in the shape of the rectangular potential, which are resolved by analysing the spectrum of the photoluminescence with the aid of energy tomography. Here, the tomography refers to the process of the real-space imaging of the condensate probability density by capturing the near-field emission after it passes through the spectrometer.…”
Section: Methodsmentioning
confidence: 99%