Accurate computational simulations of perturbed Chen–Lee–Liu equation
This research aims to look into alternative unique solitary wave solutions to the perturbed Chen–Lee–Liu (CLL) equation to explain the kinetic and physical aspects of an optical fiber pulse. The perturbed CLL equation is one of the most well-known icon models derived from the well-known Schrödinger...
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| Published in | Results in physics Vol. 45; p. 106227 |
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| Main Authors | , , |
| Format | Journal Article |
| Language | English |
| Published |
Elsevier B.V
01.02.2023
Elsevier |
| Subjects | |
| Online Access | Get full text |
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| Abstract | This research aims to look into alternative unique solitary wave solutions to the perturbed Chen–Lee–Liu (CLL) equation to explain the kinetic and physical aspects of an optical fiber pulse. The perturbed CLL equation is one of the most well-known icon models derived from the well-known Schrödinger equation. Two different analytical methodologies are used to develop novel solitary wave solutions. These responses are then thoroughly evaluated using a well-known numerical approach to establish their underlying veracity. Various graphics are used to show the pulse wave analysis process and outcomes in an optical cable. We show how scientifically unique the study is by explaining the comparison figure that was made from our data and has been used in many recent research studies
•Study of perturbed Chen–Lee–Liu equation.•Analytical and numerical novel constructed results.•Investigating the obtained results’ accuracy.•Explaining the obtained solutions through some distinct types of sketches. |
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| AbstractList | This research aims to look into alternative unique solitary wave solutions to the perturbed Chen–Lee–Liu (CLL) equation to explain the kinetic and physical aspects of an optical fiber pulse. The perturbed CLL equation is one of the most well-known icon models derived from the well-known Schrödinger equation. Two different analytical methodologies are used to develop novel solitary wave solutions. These responses are then thoroughly evaluated using a well-known numerical approach to establish their underlying veracity. Various graphics are used to show the pulse wave analysis process and outcomes in an optical cable. We show how scientifically unique the study is by explaining the comparison figure that was made from our data and has been used in many recent research studies This research aims to look into alternative unique solitary wave solutions to the perturbed Chen–Lee–Liu (CLL) equation to explain the kinetic and physical aspects of an optical fiber pulse. The perturbed CLL equation is one of the most well-known icon models derived from the well-known Schrödinger equation. Two different analytical methodologies are used to develop novel solitary wave solutions. These responses are then thoroughly evaluated using a well-known numerical approach to establish their underlying veracity. Various graphics are used to show the pulse wave analysis process and outcomes in an optical cable. We show how scientifically unique the study is by explaining the comparison figure that was made from our data and has been used in many recent research studies •Study of perturbed Chen–Lee–Liu equation.•Analytical and numerical novel constructed results.•Investigating the obtained results’ accuracy.•Explaining the obtained solutions through some distinct types of sketches. |
| ArticleNumber | 106227 |
| Author | Zhang, Xiao Khater, Mostafa M.A. Attia, Raghda A.M. |
| Author_xml | – sequence: 1 givenname: Mostafa M.A. orcidid: 0000-0001-8466-168X surname: Khater fullname: Khater, Mostafa M.A. email: mostafa.khater2024@yahoo.com, mostafa.khater2024@xzhmu.edu.cn organization: School of Medical Informatics and Engineering, Xuzhou Medical University, 209 Tongshan Road, 221004, Xuzhou, Jiangsu Province, PR China – sequence: 2 givenname: Xiao surname: Zhang fullname: Zhang, Xiao email: zhangxiao@xzhmu.edu.cn organization: School of Medical Informatics and Engineering, Xuzhou Medical University, 209 Tongshan Road, 221004, Xuzhou, Jiangsu Province, PR China – sequence: 3 givenname: Raghda A.M. surname: Attia fullname: Attia, Raghda A.M. email: raghda.attia2024@yahoo.com organization: School of Medical Informatics and Engineering, Xuzhou Medical University, 209 Tongshan Road, 221004, Xuzhou, Jiangsu Province, PR China |
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| Keywords | Optic soliton Semi-analytical solution Perturbed Chen–Lee–Liu equation 35Q51 35Q60 35C08 Traveling wave solution 35E05 |
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| References | Khater, Park, Lu, Attia (b4) 2020; 2020 Khater (b30) 2023 Khater, Park, Lu, Attia (b3) 2020; 2020 Khater (b20) 2022; 163 Khater, Lu, Attia (b5) 2019; 33 Khater (b22) 2022 Jiong (b34) 2003; 309 Baskonus, Osman, Ramzan, Tahir, Ashraf (b26) 2021; 53 Khater (b15) 2022; 36 Khater (b32) 2022; 162 Khater (b10) 2021; 35 Khater, Mohamed, Attia (b2) 2021; 144 Khater (b25) 2022; 162 Khater (b24) 2022; 54 Khater (b14) 2022; 157 Khater (b16) 2022 Khater (b21) 2022 Khater, Lu (b13) 2021; 35 Khater, Ahmed, El-Shorbagy (b7) 2021; 22 Khater, Alabdali, Mashat, Salama (b18) 2022; 30 Esen, Ozdemir, Secer, Bayram (b27) 2021; 245 Khater (b33) 2022; 157 Khater, Mousa, El-Shorbagy, Attia (b8) 2021; 22 Khater (b23) 2022; 137 Yue, Khater, Attia, Lu (b6) 2020; 2020 Khater (b11) 2021; 35 Houwe, Abbagari, Almohsen, Betchewe, Inc, Doka (b28) 2021; 53 Khater, Attia, Lu (b1) 2018; 24 Khater, Attia, Park, Lu (b12) 2020; 18 Khater, Attia, Lu (b9) 2019; 21 Khater, Lu (b17) 2022; 33 Noeiaghdam, Sidorov, Wazwaz, Sidorov, Sizikov (b35) 2021; 9 Yokuş, Durur, Duran (b29) 2021; 53 Khater (b19) 2022 Biswas (b31) 2018; 172 Khater (10.1016/j.rinp.2023.106227_b12) 2020; 18 Khater (10.1016/j.rinp.2023.106227_b24) 2022; 54 Khater (10.1016/j.rinp.2023.106227_b15) 2022; 36 Khater (10.1016/j.rinp.2023.106227_b20) 2022; 163 Jiong (10.1016/j.rinp.2023.106227_b34) 2003; 309 Khater (10.1016/j.rinp.2023.106227_b13) 2021; 35 Khater (10.1016/j.rinp.2023.106227_b19) 2022 Houwe (10.1016/j.rinp.2023.106227_b28) 2021; 53 Noeiaghdam (10.1016/j.rinp.2023.106227_b35) 2021; 9 Khater (10.1016/j.rinp.2023.106227_b32) 2022; 162 Khater (10.1016/j.rinp.2023.106227_b14) 2022; 157 Khater (10.1016/j.rinp.2023.106227_b11) 2021; 35 Khater (10.1016/j.rinp.2023.106227_b7) 2021; 22 Khater (10.1016/j.rinp.2023.106227_b17) 2022; 33 Khater (10.1016/j.rinp.2023.106227_b1) 2018; 24 Khater (10.1016/j.rinp.2023.106227_b5) 2019; 33 Khater (10.1016/j.rinp.2023.106227_b22) 2022 Khater (10.1016/j.rinp.2023.106227_b2) 2021; 144 Khater (10.1016/j.rinp.2023.106227_b33) 2022; 157 Esen (10.1016/j.rinp.2023.106227_b27) 2021; 245 Khater (10.1016/j.rinp.2023.106227_b9) 2019; 21 Khater (10.1016/j.rinp.2023.106227_b30) 2023 Biswas (10.1016/j.rinp.2023.106227_b31) 2018; 172 Khater (10.1016/j.rinp.2023.106227_b23) 2022; 137 Baskonus (10.1016/j.rinp.2023.106227_b26) 2021; 53 Khater (10.1016/j.rinp.2023.106227_b8) 2021; 22 Khater (10.1016/j.rinp.2023.106227_b21) 2022 Yue (10.1016/j.rinp.2023.106227_b6) 2020; 2020 Khater (10.1016/j.rinp.2023.106227_b10) 2021; 35 Khater (10.1016/j.rinp.2023.106227_b18) 2022; 30 Khater (10.1016/j.rinp.2023.106227_b25) 2022; 162 Yokuş (10.1016/j.rinp.2023.106227_b29) 2021; 53 Khater (10.1016/j.rinp.2023.106227_b3) 2020; 2020 Khater (10.1016/j.rinp.2023.106227_b4) 2020; 2020 Khater (10.1016/j.rinp.2023.106227_b16) 2022 |
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| SubjectTerms | Optic soliton Perturbed Chen–Lee–Liu equation Semi-analytical solution Traveling wave solution |
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| Title | Accurate computational simulations of perturbed Chen–Lee–Liu equation |
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