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窄脊型波导半导体激光器偏振与横模关系研究OA北大核心CSTPCD

Study on the relationship between polarization and transverse modes of narrow ridge waveguide semiconductor lasers

中文摘要英文摘要

基于有效折射率法建立了窄脊型波导数值计算模型,通过实验研究了InGaAs量子阱窄脊型波导半导体激光器偏振特性与横模之间的关系.根据理论计算,脊型波导中类TM模式在慢轴方向的有效折射率差更大,类TM模式的限制因子比类TE模式的限制因子更大、更容易出现慢轴高阶模式;而随着脊型波导的高度增加,快轴高阶模式被截断,类TE00模式的限制因子逐渐增加至与类TM00模式相近,慢轴高阶模式因其大的散射损耗被抑制,理论上可实现高偏振度、高光束质量激光输出.在实验方面,利用量子阱材料的增益偏振特性,通过脊型高度与宽度的设计,制备了高偏振度、基横模的窄脊型波导半导体激光器.

A numerical calculation model of the narrow ridge waveguide was established based on the effective refrac-tive index method.The relationship between the polarization characteristics and the transverse mode of the InGaAs quantum well narrow ridge waveguide semiconductor laser was studied experimentally.According to theoretical calcula-tions,the effective refractive index difference of the TM-like mode in the ridge waveguide is larger in the direction of the slow axis.The confinement factors of the TM-like mode are larger than those of the TE-like mode,and the slow-ax-is high-order mode is more likely to appear.As the height of the ridge waveguide increases,the fast-axis high-order modes are truncated,and the confinement factor of the TE00-like mode gradually increases to be similar to that of the TM00-like mode.The slow-axis high-order mode is suppressed due to its large scattering loss,theoretically achieving high polarization,and near diffraction limit beam-quality laser output.In terms of experiments,a narrow ridge wave-guide semiconductor laser with a high polarization extinction ratio and a fundamental transverse mode was fabricated by the gain polarization characteristics of quantum well materials and by designing the height and width of the ridge.

宋梁;高平宽;王欣阳;高松信;唐淳;贺钰雯;王浩淼;周坤;杜维川;李弋;何林安;胡耀;张亮

中国工程物理研究院 应用电子学研究所,四川 绵阳 621900||中国工程物理研究院 高能激光重点实验室,四川 绵阳 621900

物理学

半导体激光器光束质量偏振度有效折射率法波导模式分析

semiconductor lasersbeam qualitypolarization extinction ratioeffective refractive index methodwaveguide mode analysis

《红外与毫米波学报》 2024 (002)

158-165 / 8

10.11972/j.issn.1001-9014.2024.02.003

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