2012
DOI: 10.1364/ol.37.002811
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Coherence time measurements using a single detector with variable time resolution

Abstract: We present a simple technique for measuring coherence times for stationary light fields using a single detector with tunable time resolution. By measuring the equal-time second-order correlation function at varying instrument response functions it is possible to determine the coherence time and also the shape of the temporal decay without the need to record time-resolved data. The technique is demonstrated for pseudothermal light. Possible applications for dynamic light scattering and photon statistics measure… Show more

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Cited by 6 publications
(4 citation statements)
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“…By varying the detector response time (or bin size) around the period of expected coherence time one can estimate the coherence time and g (2) (0) [153]. g (2) (0) < 1 is a signature of non-classical (quantum nature) of the light [22, Fig.…”
Section: Squeezed States Of Ultra-weak Photon Emission ?mentioning
confidence: 99%
See 1 more Smart Citation
“…By varying the detector response time (or bin size) around the period of expected coherence time one can estimate the coherence time and g (2) (0) [153]. g (2) (0) < 1 is a signature of non-classical (quantum nature) of the light [22, Fig.…”
Section: Squeezed States Of Ultra-weak Photon Emission ?mentioning
confidence: 99%
“…In [152], authors introduced second order correlation function at zero time lag g (2) (τ = 0) to estimate non-classicality of UPE. By varying the detector response time (or bin size) around the period of expected coherence time one can estimate the coherence time and g (2) (0) [153]. g (2) (0) < 1 is a signature of non-classical (quantum nature) of the light [22, Fig.…”
Section: Squeezed States Of Ultra-weak Photon Emission ?mentioning
confidence: 99%
“…In bimodal lasers, the gain competition [21,22], dissipative mode coupling [23], temporal mode-switching [24], intermode kinetics [25], external feedback [26], mode coupling [27,28] and a short-pumppulse-induced quench [29,30] can lead to superthermal photon autocorrelations. Besides these quantum effects, which are known to produce superthermal photon bunching, there are also pseudo thermal light sources [31][32][33], which emit intense light with g (2) = 2 or even exceeding this value [34,35].…”
Section: Introductionmentioning
confidence: 99%
“…The active medium consists of a single layer of self-assembled AlGaInAs quantum dots with a density of ≈ 6 × 10 9 cm −2 . The sample was mounted on the cold finger of a helium-flow cryostat and kept at a temperature of 10 K. For nonresonant optical excitation, we use a Martienssen lamp [21] consisting of laser light provided by a Ti-sapphire laser emitting pulses with a duration of ≈ 100 fs at a repetition rate of 75.39 MHz and a wavelength of 790 nm scattered by a rotating ground glass disk as our pseudothermal light source [22]. The laser light is focused onto the ground glass disk using a 50 mm focal length lens.…”
mentioning
confidence: 99%