研究目的
To develop a mathematical analysis framework for the adequate description of the modes of lasers on the threshold of non-attenuated in time light emission, focusing on open dielectric resonators equipped with active regions filled with gain material.
研究成果
The study presents a general framework of GCFEP and links it to LEP as a full-wave classical electromagnetic theory of laser modes on threshold. It highlights the main steps in the conversion of GFEP and LEP for a 2-D laser with a partial active region to a set of four coupled boundary integral equations of the Muller type. The study demonstrates that a hole of a suitable radius and located at a certain place can lead to a notable growth of the directivity of lasing mode with the conservation of its low threshold.
研究不足
The laser model presented possesses full mathematical rigor for the analysis of the on-threshold laser modes but is not able to reveal time dynamics of lasing and does not account for the non-linear effects. A lesser limitation is the assumption that the material gain index in active region does not depend on the wavelength.