2018
DOI: 10.1103/physrevapplied.9.064030
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Exploring the Photon-Number Distribution of Bimodal Microlasers with a Transition Edge Sensor

Abstract: A photon-number resolving transition edge sensor (TES) is used to measure the photon-number distribution of two microcavity lasers. The investigated devices are bimodal microlasers with similar emission intensity and photon statistics with respect to the photon auto-correlation. Both high-β microlasers show partly thermal and partly coherent emission around the lasing threshold. For higher pump powers, the strong mode of microlaser A emits Poissonian distributed photons while the emission of the weak mode is t… Show more

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Cited by 41 publications
(82 citation statements)
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“…The latter is providing the intracavity photon number (top axis) while the measured photon number which is expected to be on the order of 10 4 in the 15 ns gate is reduced due to losses in the detection path and detector efficiency. We want to point out that despite the attenuation of the signal by approximately 3 orders of magnitude we can still access the underlying photon statistics as it is discussed in a recent publication [42]. (a) clearly reveals the Poissonian statistics of the strong mode with a thermal tail (indicated by significant events for n = 0).…”
Section: Photon Statisticsmentioning
confidence: 95%
“…The latter is providing the intracavity photon number (top axis) while the measured photon number which is expected to be on the order of 10 4 in the 15 ns gate is reduced due to losses in the detection path and detector efficiency. We want to point out that despite the attenuation of the signal by approximately 3 orders of magnitude we can still access the underlying photon statistics as it is discussed in a recent publication [42]. (a) clearly reveals the Poissonian statistics of the strong mode with a thermal tail (indicated by significant events for n = 0).…”
Section: Photon Statisticsmentioning
confidence: 95%
“…In this picture, a coherent (thermal) state of the light field is characterized by a Poissonian (Bose-Einstein) photon distribution function p n . This quantity can be accessed both in theory by using master-equation approaches [25][26][27][28], and in experiment by using photon-number-resolved detection schemes [29,30]. In practice, it is much easier to use the second-order photon autocorrelation function g (2) (0) to characterize the emission, as it can be readily mea-sured using Hanbury Brown and Twiss setups [31].…”
Section: Characterizing the Laser Threshold Beyond The Rate-equatmentioning
confidence: 99%
“…More generally, any experiment where the involved photon numbers are not known beforehand are not faithfully possible using click detectors. This is for instance the case for mixtures of thermal and coherent light states emitted by QD-microlasers [28] or exciton-polariton condensates in microcavities [29], for which our TES detection system has been employed recently. In summary, we employed a state-of-the-art PNR detector system for the quantum metrology of solid-state single-photon sources.…”
Section: Discussionmentioning
confidence: 99%