2023
DOI: 10.1134/s0021364023601264
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Random Laser Based on Materials in the Form of Complex Network Structures

Abstract: The theory of a random laser with an interface in the form of random or scale-free networks whose nodes are occupied by microcavities with quantum two-level systems has been proposed for the first time. The microcavities are coupled to each other through light-guiding channels forming edges of the network. It has been shown that such a laser has a number of spectral features associated with the statistical properties of the network structure. Among them are the existence of a topologically protected Perron eig… Show more

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Cited by 2 publications
(2 citation statements)
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“…where r = r/κ is the dimensionless control field amplitude. At large enough NEC parameter C Γ 1, coefficient A in ( 47) is essentially positive, and we can obtain significant amplification of macroscopic field within the network structure that is proportional to C Γ κD 0 /2 ∝ k N. In this limit, for the laser average photon number from (45) and (52), we obtain…”
Section: A-class Laser Simulatormentioning
confidence: 84%
See 1 more Smart Citation
“…where r = r/κ is the dimensionless control field amplitude. At large enough NEC parameter C Γ 1, coefficient A in ( 47) is essentially positive, and we can obtain significant amplification of macroscopic field within the network structure that is proportional to C Γ κD 0 /2 ∝ k N. In this limit, for the laser average photon number from (45) and (52), we obtain…”
Section: A-class Laser Simulatormentioning
confidence: 84%
“…It can be assumed that photons scatter along the paths that form random graphs. Recently, in [52], we offered a 2D material for the random laser that exhibits randomly formed networks with nodes that contain two-level systems (atoms, quantum dots, etc.). The network edges represent channels (waveguides) that provide coupling between the nodes.…”
Section: Random Lasersmentioning
confidence: 99%