{"title":"质中质晶格中波列的分支模式","authors":"Ling Zhang, Shangjiang Guo","doi":"10.1017/prm.2023.130","DOIUrl":null,"url":null,"abstract":"<p>We investigate the existence and branching patterns of wave trains in the mass-in-mass (MiM) lattice, which is a variant of the Fermi–Pasta–Ulam (FPU) lattice. In contrast to FPU lattice, we have to solve coupled advance-delay differential equations, which are reduced to a finite-dimensional bifurcation equation with an inherited Hamiltonian structure by applying a Lyapunov–Schmidt reduction and invariant theory. We establish a link between the MiM lattice and the monatomic FPU lattice. That is, the monochromatic and bichromatic wave trains persist near <span><span><span data-mathjax-type=\"texmath\"><span>$\\mu =0$</span></span><img data-mimesubtype=\"png\" data-type=\"\" src=\"https://static.cambridge.org/binary/version/id/urn:cambridge.org:id:binary:20240110161445970-0774:S0308210523001300:S0308210523001300_inline1.png\"/></span></span> in the nonresonance case and in the resonance case <span><span><span data-mathjax-type=\"texmath\"><span>$p:q$</span></span><img data-mimesubtype=\"png\" data-type=\"\" src=\"https://static.cambridge.org/binary/version/id/urn:cambridge.org:id:binary:20240110161445970-0774:S0308210523001300:S0308210523001300_inline2.png\"/></span></span> where <span><span><span data-mathjax-type=\"texmath\"><span>$q$</span></span><img data-mimesubtype=\"png\" data-type=\"\" src=\"https://static.cambridge.org/binary/version/id/urn:cambridge.org:id:binary:20240110161445970-0774:S0308210523001300:S0308210523001300_inline3.png\"/></span></span> is not an integer multiple of <span><span><span data-mathjax-type=\"texmath\"><span>$p$</span></span><img data-mimesubtype=\"png\" data-type=\"\" src=\"https://static.cambridge.org/binary/version/id/urn:cambridge.org:id:binary:20240110161445970-0774:S0308210523001300:S0308210523001300_inline4.png\"/></span></span>. Furthermore, we obtain the multiplicity of bichromatic wave trains in <span><span><span data-mathjax-type=\"texmath\"><span>$p:q$</span></span><img data-mimesubtype=\"png\" data-type=\"\" src=\"https://static.cambridge.org/binary/version/id/urn:cambridge.org:id:binary:20240110161445970-0774:S0308210523001300:S0308210523001300_inline5.png\"/></span></span> resonance where <span><span><span data-mathjax-type=\"texmath\"><span>$q$</span></span><img data-mimesubtype=\"png\" data-type=\"\" src=\"https://static.cambridge.org/binary/version/id/urn:cambridge.org:id:binary:20240110161445970-0774:S0308210523001300:S0308210523001300_inline6.png\"/></span></span> is an integer multiple of <span><span><span data-mathjax-type=\"texmath\"><span>$p$</span></span><img data-mimesubtype=\"png\" data-type=\"\" src=\"https://static.cambridge.org/binary/version/id/urn:cambridge.org:id:binary:20240110161445970-0774:S0308210523001300:S0308210523001300_inline7.png\"/></span></span>, based on the singular theorem.</p>","PeriodicalId":54560,"journal":{"name":"Proceedings of the Royal Society of Edinburgh Section A-Mathematics","volume":"51 1","pages":""},"PeriodicalIF":1.3000,"publicationDate":"2024-01-11","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Branching patterns of wave trains in mass-in-mass lattices\",\"authors\":\"Ling Zhang, Shangjiang Guo\",\"doi\":\"10.1017/prm.2023.130\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<p>We investigate the existence and branching patterns of wave trains in the mass-in-mass (MiM) lattice, which is a variant of the Fermi–Pasta–Ulam (FPU) lattice. In contrast to FPU lattice, we have to solve coupled advance-delay differential equations, which are reduced to a finite-dimensional bifurcation equation with an inherited Hamiltonian structure by applying a Lyapunov–Schmidt reduction and invariant theory. We establish a link between the MiM lattice and the monatomic FPU lattice. That is, the monochromatic and bichromatic wave trains persist near <span><span><span data-mathjax-type=\\\"texmath\\\"><span>$\\\\mu =0$</span></span><img data-mimesubtype=\\\"png\\\" data-type=\\\"\\\" src=\\\"https://static.cambridge.org/binary/version/id/urn:cambridge.org:id:binary:20240110161445970-0774:S0308210523001300:S0308210523001300_inline1.png\\\"/></span></span> in the nonresonance case and in the resonance case <span><span><span data-mathjax-type=\\\"texmath\\\"><span>$p:q$</span></span><img data-mimesubtype=\\\"png\\\" data-type=\\\"\\\" src=\\\"https://static.cambridge.org/binary/version/id/urn:cambridge.org:id:binary:20240110161445970-0774:S0308210523001300:S0308210523001300_inline2.png\\\"/></span></span> where <span><span><span data-mathjax-type=\\\"texmath\\\"><span>$q$</span></span><img data-mimesubtype=\\\"png\\\" data-type=\\\"\\\" src=\\\"https://static.cambridge.org/binary/version/id/urn:cambridge.org:id:binary:20240110161445970-0774:S0308210523001300:S0308210523001300_inline3.png\\\"/></span></span> is not an integer multiple of <span><span><span data-mathjax-type=\\\"texmath\\\"><span>$p$</span></span><img data-mimesubtype=\\\"png\\\" data-type=\\\"\\\" src=\\\"https://static.cambridge.org/binary/version/id/urn:cambridge.org:id:binary:20240110161445970-0774:S0308210523001300:S0308210523001300_inline4.png\\\"/></span></span>. Furthermore, we obtain the multiplicity of bichromatic wave trains in <span><span><span data-mathjax-type=\\\"texmath\\\"><span>$p:q$</span></span><img data-mimesubtype=\\\"png\\\" data-type=\\\"\\\" src=\\\"https://static.cambridge.org/binary/version/id/urn:cambridge.org:id:binary:20240110161445970-0774:S0308210523001300:S0308210523001300_inline5.png\\\"/></span></span> resonance where <span><span><span data-mathjax-type=\\\"texmath\\\"><span>$q$</span></span><img data-mimesubtype=\\\"png\\\" data-type=\\\"\\\" src=\\\"https://static.cambridge.org/binary/version/id/urn:cambridge.org:id:binary:20240110161445970-0774:S0308210523001300:S0308210523001300_inline6.png\\\"/></span></span> is an integer multiple of <span><span><span data-mathjax-type=\\\"texmath\\\"><span>$p$</span></span><img data-mimesubtype=\\\"png\\\" data-type=\\\"\\\" src=\\\"https://static.cambridge.org/binary/version/id/urn:cambridge.org:id:binary:20240110161445970-0774:S0308210523001300:S0308210523001300_inline7.png\\\"/></span></span>, based on the singular theorem.</p>\",\"PeriodicalId\":54560,\"journal\":{\"name\":\"Proceedings of the Royal Society of Edinburgh Section A-Mathematics\",\"volume\":\"51 1\",\"pages\":\"\"},\"PeriodicalIF\":1.3000,\"publicationDate\":\"2024-01-11\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Proceedings of the Royal Society of Edinburgh Section A-Mathematics\",\"FirstCategoryId\":\"100\",\"ListUrlMain\":\"https://doi.org/10.1017/prm.2023.130\",\"RegionNum\":3,\"RegionCategory\":\"数学\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q1\",\"JCRName\":\"MATHEMATICS\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Proceedings of the Royal Society of Edinburgh Section A-Mathematics","FirstCategoryId":"100","ListUrlMain":"https://doi.org/10.1017/prm.2023.130","RegionNum":3,"RegionCategory":"数学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"MATHEMATICS","Score":null,"Total":0}
Branching patterns of wave trains in mass-in-mass lattices
We investigate the existence and branching patterns of wave trains in the mass-in-mass (MiM) lattice, which is a variant of the Fermi–Pasta–Ulam (FPU) lattice. In contrast to FPU lattice, we have to solve coupled advance-delay differential equations, which are reduced to a finite-dimensional bifurcation equation with an inherited Hamiltonian structure by applying a Lyapunov–Schmidt reduction and invariant theory. We establish a link between the MiM lattice and the monatomic FPU lattice. That is, the monochromatic and bichromatic wave trains persist near $\mu =0$ in the nonresonance case and in the resonance case $p:q$ where $q$ is not an integer multiple of $p$. Furthermore, we obtain the multiplicity of bichromatic wave trains in $p:q$ resonance where $q$ is an integer multiple of $p$, based on the singular theorem.
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