{"title":"自由空间中由优雅拉盖尔和优雅高斯函数调制的时空艾里光束","authors":"Xiaping Zhang","doi":"10.1109/ICISCT47635.2019.9011988","DOIUrl":null,"url":null,"abstract":"Airy elegant Gaussian beam is the airy beam which is modulated by the elegant Gaussian. According to the (2+1)D paraxial wave equation describing the wave propagation of the electric field, Airy elegant Gaussian solution to the paraxial wave equation in spatial field are accessed. The solution of the Airy-Elegant-Largeurre-Gaussian(AiELG) beam, which is the spatiotemporal Airy elegant Gaussian beam modulated by the elegant Larguerre function, can be accessed by solving the (3+1)D Schrödinger equation in the free space. We found that their intensity profiles are determined by three parameters: the azimuthal mode number, the radial mode number and the modulation depth. It is worth mentioning that the radial mode number of AiELG wave packet will change in propagation.","PeriodicalId":170576,"journal":{"name":"2019 International Conference on Information Science and Communications Technologies (ICISCT)","volume":"57 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2019-11-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"1","resultStr":"{\"title\":\"Spatiotemporal Airy beam modulated by elegant Laguerre and elegant Gaussian function in free space\",\"authors\":\"Xiaping Zhang\",\"doi\":\"10.1109/ICISCT47635.2019.9011988\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Airy elegant Gaussian beam is the airy beam which is modulated by the elegant Gaussian. According to the (2+1)D paraxial wave equation describing the wave propagation of the electric field, Airy elegant Gaussian solution to the paraxial wave equation in spatial field are accessed. The solution of the Airy-Elegant-Largeurre-Gaussian(AiELG) beam, which is the spatiotemporal Airy elegant Gaussian beam modulated by the elegant Larguerre function, can be accessed by solving the (3+1)D Schrödinger equation in the free space. We found that their intensity profiles are determined by three parameters: the azimuthal mode number, the radial mode number and the modulation depth. It is worth mentioning that the radial mode number of AiELG wave packet will change in propagation.\",\"PeriodicalId\":170576,\"journal\":{\"name\":\"2019 International Conference on Information Science and Communications Technologies (ICISCT)\",\"volume\":\"57 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2019-11-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"1\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"2019 International Conference on Information Science and Communications Technologies (ICISCT)\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/ICISCT47635.2019.9011988\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"2019 International Conference on Information Science and Communications Technologies (ICISCT)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/ICISCT47635.2019.9011988","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Spatiotemporal Airy beam modulated by elegant Laguerre and elegant Gaussian function in free space
Airy elegant Gaussian beam is the airy beam which is modulated by the elegant Gaussian. According to the (2+1)D paraxial wave equation describing the wave propagation of the electric field, Airy elegant Gaussian solution to the paraxial wave equation in spatial field are accessed. The solution of the Airy-Elegant-Largeurre-Gaussian(AiELG) beam, which is the spatiotemporal Airy elegant Gaussian beam modulated by the elegant Larguerre function, can be accessed by solving the (3+1)D Schrödinger equation in the free space. We found that their intensity profiles are determined by three parameters: the azimuthal mode number, the radial mode number and the modulation depth. It is worth mentioning that the radial mode number of AiELG wave packet will change in propagation.