Cavity solitons (CSs) are bright intensity peaks over a dark homogeneous background. They arise in the coherent field transmitted by nonlinear optical resonators, and are generated through diffraction-mediated light-matter interaction which leads to field self-localization within the cavity. CSs have been experimentally demonstrated in broad area, driven vertical cavity surface emitting laser (VCSELs) below and above threshold. In a laser with a saturable absorber (LSA) it is possible to achieve the optimal condition where CSs coexist with a dark state of pure spontaneous emission corresponding to a laser below threshold. Under this condition the contrast between the CSs and the homogeneous background is maximum. On the other hand, since such a device is able to generate CSs without an external holding beam, it is the realization of a Cavity Soliton Laser (CSL).

Moving cavity solitons in a cavity soliton laser / Prati, F; Aghdami, Km; Tissoni, G; Brambilla, Massimo; Lugiato, La. - (2009), p. 5194554. (Intervento presentato al convegno CLEO/Europe - EQEC 2009 - European Conference on Lasers and Electro-Optics and the European Quantum Electronics Conference tenutosi a Munich - Germany nel 14-19 Giugno 2009) [10.1109/CLEOE-EQEC.2009.5194554].

Moving cavity solitons in a cavity soliton laser

BRAMBILLA, Massimo;
2009-01-01

Abstract

Cavity solitons (CSs) are bright intensity peaks over a dark homogeneous background. They arise in the coherent field transmitted by nonlinear optical resonators, and are generated through diffraction-mediated light-matter interaction which leads to field self-localization within the cavity. CSs have been experimentally demonstrated in broad area, driven vertical cavity surface emitting laser (VCSELs) below and above threshold. In a laser with a saturable absorber (LSA) it is possible to achieve the optimal condition where CSs coexist with a dark state of pure spontaneous emission corresponding to a laser below threshold. Under this condition the contrast between the CSs and the homogeneous background is maximum. On the other hand, since such a device is able to generate CSs without an external holding beam, it is the realization of a Cavity Soliton Laser (CSL).
2009
CLEO/Europe - EQEC 2009 - European Conference on Lasers and Electro-Optics and the European Quantum Electronics Conference
978-142444080-1
Moving cavity solitons in a cavity soliton laser / Prati, F; Aghdami, Km; Tissoni, G; Brambilla, Massimo; Lugiato, La. - (2009), p. 5194554. (Intervento presentato al convegno CLEO/Europe - EQEC 2009 - European Conference on Lasers and Electro-Optics and the European Quantum Electronics Conference tenutosi a Munich - Germany nel 14-19 Giugno 2009) [10.1109/CLEOE-EQEC.2009.5194554].
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/11589/17856
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