Počet záznamů: 1  

Optical theorem helps understand thresholds of lasing in microcavities with active regions

  1. 1.
    SYSNO ASEP0437137
    Druh ASEPJ - Článek v odborném periodiku
    Zařazení RIVJ - Článek v odborném periodiku
    Poddruh JČlánek ve WOS
    NázevOptical theorem helps understand thresholds of lasing in microcavities with active regions
    Tvůrce(i) Smotrova, E. I. (UA)
    Byelobrov, V. (UA)
    Benson, T. M. (GB)
    Čtyroký, Jiří (URE-Y) RID
    Sauleau, R. (FR)
    Nosich, A. I. (UA)
    Celkový počet autorů6
    Zdroj.dok.IEEE Journal of Quantum Electronics - ISSN 0018-9197
    Roč. 47, č. 1 (2011), s. 20-30
    Poč.str.11 s.
    Forma vydáníTištěná - P
    Jazyk dok.eng - angličtina
    Země vyd.US - Spojené státy americké
    Klíč. slovaEigenvalue problem ; lasing threshold ; microcavity laser
    Vědní obor RIVJA - Elektronika a optoelektronika, elektrotechnika
    CEZAV0Z20670512 - URE-Y (2005-2011)
    UT WOS000283938500001
    EID SCOPUS78149245297
    DOI https://doi.org/10.1109/JQE.2010.2055836
    AnotaceWithin the framework of the recently proposed approach to view the lasing in open microcavities as a linear eigenproblem for the Maxwell equations with exact boundary and radiation conditions, we study the correspondence between the modal thresholds and field overlap coefficients. Macroscopic gain is introduced into the cavity material within the active region via the active imaginary part of the refractive index. Each eigenvalue is constituted of two positive numbers, namely, the lasing wavenumber and the threshold value of material gain. This approach yields clear insight into the lasing thresholds of individual modes. The Optical Theorem, if applied to the lasing-mode field, puts the familiar "gain=loss" condition on firm footing. It rigorously quantifies the role of the spatial overlap of the mode E-field with the active region, whose shape and location are efficient tools of the threshold manipulation. Here, the effective mode volume in open resonator is introduced from first principles. Examples are given for the 1-D cavities equipped with active layers and distributed Bragg reflectors and 2-D cavities with active disks and annular Bragg reflectors
    PracovištěÚstav fotoniky a elektroniky
    KontaktPetr Vacek, vacek@ufe.cz, Tel.: 266 773 413, 266 773 438, 266 773 488
    Rok sběru2015
Počet záznamů: 1  

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