Y. Yıldırım, E. Topkara, A. Biswas, H. Triki, M. Ekici, P. Guggilla, S. Khan, M. Belić
{"title":"二次-三次非线性光孤子摄动与偏振","authors":"Y. Yıldırım, E. Topkara, A. Biswas, H. Triki, M. Ekici, P. Guggilla, S. Khan, M. Belić","doi":"10.30970/JPS.25.2001","DOIUrl":null,"url":null,"abstract":"This paper recovers a full spectrum of optical solitons that are generated by the combined e(cid:27)ects of dispersion and nonlinearity of the pulse propagation. The quadratic(cid:21)cubic form of the nonlinear refractive index is incorporated in the governing nonlinear Schr(cid:4)odinger equation, which governs the dynamics of the soliton transmission across trans-continental and transoceanic distances. The model is considered with a nonlinear chromatic dispersion that is required to sustain for smooth transmission of soliton pulses in optical (cid:28)bers, couplers, PCF, magneto-optic waveguides, crystals, metamaterials, metasurfaces, birefringent (cid:28)bers, DWDM systems and other form of waveguides. Solitons in birefringent (cid:28)bers as well as solitons in polarization preserving (cid:28)bers are considered. The governing model is treated with Hamiltonian type perturbation terms. The perturbation terms are with full intensity. The model is studied for the intensity count m = 1 . The adopted integration algorithm is the sine-Gordon equation method that reveals single form soliton solutions as well as dual-form soliton solutions. These solitons are dark soliton, singular soliton, bright soliton and combo singular soliton. Also, dark soliton represents a kink/anti-kink solitary wave or a shock wave in (cid:29)uid dynamics. The respective constraint conditions are also in place to guarantee the existence of such solitons.","PeriodicalId":43482,"journal":{"name":"Journal of Physical Studies","volume":"282 1","pages":""},"PeriodicalIF":0.7000,"publicationDate":"2021-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"1","resultStr":"{\"title\":\"Optical soliton perturbation and polarization with quadratic--cubic nonlinearity by sine-Gordon equation approach\",\"authors\":\"Y. Yıldırım, E. Topkara, A. Biswas, H. Triki, M. Ekici, P. Guggilla, S. Khan, M. Belić\",\"doi\":\"10.30970/JPS.25.2001\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"This paper recovers a full spectrum of optical solitons that are generated by the combined e(cid:27)ects of dispersion and nonlinearity of the pulse propagation. The quadratic(cid:21)cubic form of the nonlinear refractive index is incorporated in the governing nonlinear Schr(cid:4)odinger equation, which governs the dynamics of the soliton transmission across trans-continental and transoceanic distances. The model is considered with a nonlinear chromatic dispersion that is required to sustain for smooth transmission of soliton pulses in optical (cid:28)bers, couplers, PCF, magneto-optic waveguides, crystals, metamaterials, metasurfaces, birefringent (cid:28)bers, DWDM systems and other form of waveguides. Solitons in birefringent (cid:28)bers as well as solitons in polarization preserving (cid:28)bers are considered. The governing model is treated with Hamiltonian type perturbation terms. The perturbation terms are with full intensity. The model is studied for the intensity count m = 1 . The adopted integration algorithm is the sine-Gordon equation method that reveals single form soliton solutions as well as dual-form soliton solutions. These solitons are dark soliton, singular soliton, bright soliton and combo singular soliton. Also, dark soliton represents a kink/anti-kink solitary wave or a shock wave in (cid:29)uid dynamics. The respective constraint conditions are also in place to guarantee the existence of such solitons.\",\"PeriodicalId\":43482,\"journal\":{\"name\":\"Journal of Physical Studies\",\"volume\":\"282 1\",\"pages\":\"\"},\"PeriodicalIF\":0.7000,\"publicationDate\":\"2021-01-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"1\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Journal of Physical Studies\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.30970/JPS.25.2001\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q3\",\"JCRName\":\"PHYSICS, MULTIDISCIPLINARY\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of Physical Studies","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.30970/JPS.25.2001","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q3","JCRName":"PHYSICS, MULTIDISCIPLINARY","Score":null,"Total":0}
Optical soliton perturbation and polarization with quadratic--cubic nonlinearity by sine-Gordon equation approach
This paper recovers a full spectrum of optical solitons that are generated by the combined e(cid:27)ects of dispersion and nonlinearity of the pulse propagation. The quadratic(cid:21)cubic form of the nonlinear refractive index is incorporated in the governing nonlinear Schr(cid:4)odinger equation, which governs the dynamics of the soliton transmission across trans-continental and transoceanic distances. The model is considered with a nonlinear chromatic dispersion that is required to sustain for smooth transmission of soliton pulses in optical (cid:28)bers, couplers, PCF, magneto-optic waveguides, crystals, metamaterials, metasurfaces, birefringent (cid:28)bers, DWDM systems and other form of waveguides. Solitons in birefringent (cid:28)bers as well as solitons in polarization preserving (cid:28)bers are considered. The governing model is treated with Hamiltonian type perturbation terms. The perturbation terms are with full intensity. The model is studied for the intensity count m = 1 . The adopted integration algorithm is the sine-Gordon equation method that reveals single form soliton solutions as well as dual-form soliton solutions. These solitons are dark soliton, singular soliton, bright soliton and combo singular soliton. Also, dark soliton represents a kink/anti-kink solitary wave or a shock wave in (cid:29)uid dynamics. The respective constraint conditions are also in place to guarantee the existence of such solitons.