Abstract
We propose an approach based on random matrix theory to calculate the temporal second-order intensity correlation function g((2))(t) of the radiation emitted by random lasers and random fiber lasers. The multimode character of these systems, with a relevant degree of disorder in the active medium, and a large number of random scattering centers substantially hinder the calculation of g((2))(t). Here, we apply in a photonic system the universal statistical properties of Ginibre's non-Hermitian random matrix ensemble to obtain g((2))(t). Excellent agreement is found with time-resolved measurements for several excitation powers of an erbium-based random fiber laser. We also discuss the extension of the random matrix approach to address the statistical properties of general disordered photonic systems with various Hamiltonian symmetries.
Dokumententyp: | Zeitschriftenartikel |
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Fakultät: | Physik |
Themengebiete: | 500 Naturwissenschaften und Mathematik > 530 Physik |
ISSN: | 2469-9926 |
Sprache: | Englisch |
Dokumenten ID: | 113335 |
Datum der Veröffentlichung auf Open Access LMU: | 02. Apr. 2024, 07:47 |
Letzte Änderungen: | 02. Apr. 2024, 07:47 |