Innovative Uses of Stochastic Photonic Sources

We report on the properties and applications of intense and nonconventional stochastic photonic sources based on amplified spontaneous emission (ASE) [1]. First, we describe the principle of nonlinear intensity filtering using various nonlinear filters (e.g. a modified nonlinear Mach-Zehnder interferometer). The latter can alter the properties of an intense incident ASE source in a controlled manner. In particular, we demonstrated the possibility to tailor the probability density function (PDF) <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$p(I)$</tex> ) (Fig. 1.a) as well as the second- and, in a more general sense, the <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$n$</tex> -th order degree of coherence <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$g^{(n \geq 1)}\left(\tau\right.)$</tex> ) associated with the likelihood and the correlation of the intensity fluctuations, respectively. Depending on the type of filter and its parameters, the resulting random intensity <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$I(t)$</tex> can exhibit large overshoots or smoother fluctuations.

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Published
2025-06-23
DOI
https://doi.org/10.1109/cleo/europe-eqec65582.2025.11111262
Primary Topic
Photonic and Optical Devices
Type
article
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article

Innovative Uses of Stochastic Photonic Sources

Guillaume Walter, Nicolas Valero, Guillaume Duchateau, Denis Marion et al.
Photonic and Optical Devices
article

Innovative Uses of Stochastic Photonic Sources

Guillaume Walter, Nicolas Valero, Guillaume Duchateau, Denis Marion, Jérôme Lhermite, Jean-Christophe Delaanes, Marie Zambelli
article en

Abstract

We report on the properties and applications of intense and nonconventional stochastic photonic sources based on amplified spontaneous emission (ASE) [1]. First, we describe the principle of nonlinear intensity filtering using various nonlinear filters (e.g. a modified nonlinear Mach-Zehnder interferometer). The latter can alter the properties of an intense incident ASE source in a controlled manner. In particular, we demonstrated the possibility to tailor the probability density function (PDF) <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$p(I)$</tex> ) (Fig. 1.a) as well as the second- and, in a more general sense, the <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$n$</tex> -th order degree of coherence <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$g^{(n \geq 1)}\left(\tau\right.)$</tex> ) associated with the likelihood and the correlation of the intensity fluctuations, respectively. Depending on the type of filter and its parameters, the resulting random intensity <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$I(t)$</tex> can exhibit large overshoots or smoother fluctuations.

Centre National de la Recherche Scientifique (FR), Université de Bordeaux (FR), Commissariat à l'Énergie Atomique et aux Énergies Alternatives (FR), Centre Lasers Intenses et Applications (FR)
Openalex Percentile: Top 79%
Photonic and Optical Devices
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