Tuncay Aktosun, Abdon E. Choque-Rivero, Ivan Toledo, Mehmet Unlu
{"title":"一类三阶常线性微分算子的孤子解","authors":"Tuncay Aktosun, Abdon E. Choque-Rivero, Ivan Toledo, Mehmet Unlu","doi":"10.1111/sapm.70057","DOIUrl":null,"url":null,"abstract":"<div>\n \n <p>Explicit solutions to the related integrable nonlinear evolution equations are constructed by solving the inverse scattering problem in the reflectionless case for the third-order differential equation <span></span><math>\n <semantics>\n <mrow>\n <msup>\n <mi>d</mi>\n <mn>3</mn>\n </msup>\n <mi>ψ</mi>\n <mo>/</mo>\n <mi>d</mi>\n <msup>\n <mi>x</mi>\n <mn>3</mn>\n </msup>\n <mo>+</mo>\n <mi>Q</mi>\n <mspace></mspace>\n <mi>d</mi>\n <mi>ψ</mi>\n <mo>/</mo>\n <mi>d</mi>\n <mi>x</mi>\n <mo>+</mo>\n <mi>P</mi>\n <mspace></mspace>\n <mi>ψ</mi>\n <mo>=</mo>\n <msup>\n <mi>k</mi>\n <mn>3</mn>\n </msup>\n <mi>ψ</mi>\n </mrow>\n <annotation>$d^3\\psi /dx^3+Q\\,d\\psi /dx+P\\,\\psi =k^3\\psi$</annotation>\n </semantics></math>, where <span></span><math>\n <semantics>\n <mi>Q</mi>\n <annotation>$Q$</annotation>\n </semantics></math> and <span></span><math>\n <semantics>\n <mi>P</mi>\n <annotation>$P$</annotation>\n </semantics></math> are the potentials in the Schwartz class and <span></span><math>\n <semantics>\n <msup>\n <mi>k</mi>\n <mn>3</mn>\n </msup>\n <annotation>$k^3$</annotation>\n </semantics></math> is the spectral parameter. The input data set used to solve the relevant inverse problem consists of the bound-state poles of a transmission coefficient and the corresponding bound-state dependency constants. Using the time-evolved dependency constants, explicit solutions to the related integrable evolution equations are obtained. In the special cases of the Sawada–Kotera equation and the modified bad Boussinesq equation, the method presented here explains the physical origin of the constants appearing in the relevant <span></span><math>\n <semantics>\n <mi>N</mi>\n <annotation>$\\mathbf {N}$</annotation>\n </semantics></math>-soliton solutions algebraically constructed, but without any physical insight, by the bilinear method of Hirota. </p></div>","PeriodicalId":51174,"journal":{"name":"Studies in Applied Mathematics","volume":"154 6","pages":""},"PeriodicalIF":2.3000,"publicationDate":"2025-06-17","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Soliton Solutions Associated With a Class of Third-Order Ordinary Linear Differential Operators\",\"authors\":\"Tuncay Aktosun, Abdon E. Choque-Rivero, Ivan Toledo, Mehmet Unlu\",\"doi\":\"10.1111/sapm.70057\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div>\\n \\n <p>Explicit solutions to the related integrable nonlinear evolution equations are constructed by solving the inverse scattering problem in the reflectionless case for the third-order differential equation <span></span><math>\\n <semantics>\\n <mrow>\\n <msup>\\n <mi>d</mi>\\n <mn>3</mn>\\n </msup>\\n <mi>ψ</mi>\\n <mo>/</mo>\\n <mi>d</mi>\\n <msup>\\n <mi>x</mi>\\n <mn>3</mn>\\n </msup>\\n <mo>+</mo>\\n <mi>Q</mi>\\n <mspace></mspace>\\n <mi>d</mi>\\n <mi>ψ</mi>\\n <mo>/</mo>\\n <mi>d</mi>\\n <mi>x</mi>\\n <mo>+</mo>\\n <mi>P</mi>\\n <mspace></mspace>\\n <mi>ψ</mi>\\n <mo>=</mo>\\n <msup>\\n <mi>k</mi>\\n <mn>3</mn>\\n </msup>\\n <mi>ψ</mi>\\n </mrow>\\n <annotation>$d^3\\\\psi /dx^3+Q\\\\,d\\\\psi /dx+P\\\\,\\\\psi =k^3\\\\psi$</annotation>\\n </semantics></math>, where <span></span><math>\\n <semantics>\\n <mi>Q</mi>\\n <annotation>$Q$</annotation>\\n </semantics></math> and <span></span><math>\\n <semantics>\\n <mi>P</mi>\\n <annotation>$P$</annotation>\\n </semantics></math> are the potentials in the Schwartz class and <span></span><math>\\n <semantics>\\n <msup>\\n <mi>k</mi>\\n <mn>3</mn>\\n </msup>\\n <annotation>$k^3$</annotation>\\n </semantics></math> is the spectral parameter. The input data set used to solve the relevant inverse problem consists of the bound-state poles of a transmission coefficient and the corresponding bound-state dependency constants. Using the time-evolved dependency constants, explicit solutions to the related integrable evolution equations are obtained. In the special cases of the Sawada–Kotera equation and the modified bad Boussinesq equation, the method presented here explains the physical origin of the constants appearing in the relevant <span></span><math>\\n <semantics>\\n <mi>N</mi>\\n <annotation>$\\\\mathbf {N}$</annotation>\\n </semantics></math>-soliton solutions algebraically constructed, but without any physical insight, by the bilinear method of Hirota. </p></div>\",\"PeriodicalId\":51174,\"journal\":{\"name\":\"Studies in Applied Mathematics\",\"volume\":\"154 6\",\"pages\":\"\"},\"PeriodicalIF\":2.3000,\"publicationDate\":\"2025-06-17\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Studies in Applied Mathematics\",\"FirstCategoryId\":\"100\",\"ListUrlMain\":\"https://onlinelibrary.wiley.com/doi/10.1111/sapm.70057\",\"RegionNum\":2,\"RegionCategory\":\"数学\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q1\",\"JCRName\":\"MATHEMATICS, APPLIED\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Studies in Applied Mathematics","FirstCategoryId":"100","ListUrlMain":"https://onlinelibrary.wiley.com/doi/10.1111/sapm.70057","RegionNum":2,"RegionCategory":"数学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"MATHEMATICS, APPLIED","Score":null,"Total":0}
Soliton Solutions Associated With a Class of Third-Order Ordinary Linear Differential Operators
Explicit solutions to the related integrable nonlinear evolution equations are constructed by solving the inverse scattering problem in the reflectionless case for the third-order differential equation , where and are the potentials in the Schwartz class and is the spectral parameter. The input data set used to solve the relevant inverse problem consists of the bound-state poles of a transmission coefficient and the corresponding bound-state dependency constants. Using the time-evolved dependency constants, explicit solutions to the related integrable evolution equations are obtained. In the special cases of the Sawada–Kotera equation and the modified bad Boussinesq equation, the method presented here explains the physical origin of the constants appearing in the relevant -soliton solutions algebraically constructed, but without any physical insight, by the bilinear method of Hirota.
期刊介绍:
Studies in Applied Mathematics explores the interplay between mathematics and the applied disciplines. It publishes papers that advance the understanding of physical processes, or develop new mathematical techniques applicable to physical and real-world problems. Its main themes include (but are not limited to) nonlinear phenomena, mathematical modeling, integrable systems, asymptotic analysis, inverse problems, numerical analysis, dynamical systems, scientific computing and applications to areas such as fluid mechanics, mathematical biology, and optics.