{"title":"六边形晶格上的波传播","authors":"David Kapanadze, Ekaterina Pesetskaya","doi":"10.1515/gmj-2024-2035","DOIUrl":null,"url":null,"abstract":"We consider propagation of two-dimensional waves on the infinite hexagonal (honeycomb) lattice. Namely, we study the discrete Helmholtz equation in hexagonal lattices without and with a boundary. It is shown that for some configurations these problems can be equivalently reduced to similar problems for the triangular lattice. Based on this fact, new results are obtained for the existence and uniqueness of the solution in the case of the real wave number <jats:inline-formula> <jats:alternatives> <m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\"> <m:mrow> <m:mi>k</m:mi> <m:mo>∈</m:mo> <m:mrow> <m:mrow> <m:mo stretchy=\"false\">(</m:mo> <m:mn>0</m:mn> <m:mo>,</m:mo> <m:msqrt> <m:mn>6</m:mn> </m:msqrt> <m:mo stretchy=\"false\">)</m:mo> </m:mrow> <m:mo>∖</m:mo> <m:mrow> <m:mo stretchy=\"false\">{</m:mo> <m:msqrt> <m:mn>2</m:mn> </m:msqrt> <m:mo>,</m:mo> <m:msqrt> <m:mn>3</m:mn> </m:msqrt> <m:mo>,</m:mo> <m:mn>2</m:mn> <m:mo stretchy=\"false\">}</m:mo> </m:mrow> </m:mrow> </m:mrow> </m:math> <jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"graphic/j_gmj-2024-2035_eq_0179.png\"/> <jats:tex-math>{k\\in(0,\\sqrt{6})\\setminus\\{\\sqrt{2},\\sqrt{3},2\\}}</jats:tex-math> </jats:alternatives> </jats:inline-formula> for the non-homogeneous Helmholtz equation in hexagonal lattices with no boundaries and the real wave number <jats:inline-formula> <jats:alternatives> <m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\"> <m:mrow> <m:mi>k</m:mi> <m:mo>∈</m:mo> <m:mrow> <m:mrow> <m:mo stretchy=\"false\">(</m:mo> <m:mn>0</m:mn> <m:mo>,</m:mo> <m:msqrt> <m:mn>2</m:mn> </m:msqrt> <m:mo stretchy=\"false\">)</m:mo> </m:mrow> <m:mo>∪</m:mo> <m:mrow> <m:mo stretchy=\"false\">(</m:mo> <m:mn>2</m:mn> <m:mo>,</m:mo> <m:msqrt> <m:mn>6</m:mn> </m:msqrt> <m:mo stretchy=\"false\">)</m:mo> </m:mrow> </m:mrow> </m:mrow> </m:math> <jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"graphic/j_gmj-2024-2035_eq_0178.png\"/> <jats:tex-math>{k\\in(0,\\sqrt{2})\\cup(2,\\sqrt{6})}</jats:tex-math> </jats:alternatives> </jats:inline-formula> for the exterior Dirichlet problem.","PeriodicalId":55101,"journal":{"name":"Georgian Mathematical Journal","volume":null,"pages":null},"PeriodicalIF":0.8000,"publicationDate":"2024-06-25","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Wave propagation on hexagonal lattices\",\"authors\":\"David Kapanadze, Ekaterina Pesetskaya\",\"doi\":\"10.1515/gmj-2024-2035\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"We consider propagation of two-dimensional waves on the infinite hexagonal (honeycomb) lattice. Namely, we study the discrete Helmholtz equation in hexagonal lattices without and with a boundary. It is shown that for some configurations these problems can be equivalently reduced to similar problems for the triangular lattice. Based on this fact, new results are obtained for the existence and uniqueness of the solution in the case of the real wave number <jats:inline-formula> <jats:alternatives> <m:math xmlns:m=\\\"http://www.w3.org/1998/Math/MathML\\\"> <m:mrow> <m:mi>k</m:mi> <m:mo>∈</m:mo> <m:mrow> <m:mrow> <m:mo stretchy=\\\"false\\\">(</m:mo> <m:mn>0</m:mn> <m:mo>,</m:mo> <m:msqrt> <m:mn>6</m:mn> </m:msqrt> <m:mo stretchy=\\\"false\\\">)</m:mo> </m:mrow> <m:mo>∖</m:mo> <m:mrow> <m:mo stretchy=\\\"false\\\">{</m:mo> <m:msqrt> <m:mn>2</m:mn> </m:msqrt> <m:mo>,</m:mo> <m:msqrt> <m:mn>3</m:mn> </m:msqrt> <m:mo>,</m:mo> <m:mn>2</m:mn> <m:mo stretchy=\\\"false\\\">}</m:mo> </m:mrow> </m:mrow> </m:mrow> </m:math> <jats:inline-graphic xmlns:xlink=\\\"http://www.w3.org/1999/xlink\\\" xlink:href=\\\"graphic/j_gmj-2024-2035_eq_0179.png\\\"/> <jats:tex-math>{k\\\\in(0,\\\\sqrt{6})\\\\setminus\\\\{\\\\sqrt{2},\\\\sqrt{3},2\\\\}}</jats:tex-math> </jats:alternatives> </jats:inline-formula> for the non-homogeneous Helmholtz equation in hexagonal lattices with no boundaries and the real wave number <jats:inline-formula> <jats:alternatives> <m:math xmlns:m=\\\"http://www.w3.org/1998/Math/MathML\\\"> <m:mrow> <m:mi>k</m:mi> <m:mo>∈</m:mo> <m:mrow> <m:mrow> <m:mo stretchy=\\\"false\\\">(</m:mo> <m:mn>0</m:mn> <m:mo>,</m:mo> <m:msqrt> <m:mn>2</m:mn> </m:msqrt> <m:mo stretchy=\\\"false\\\">)</m:mo> </m:mrow> <m:mo>∪</m:mo> <m:mrow> <m:mo stretchy=\\\"false\\\">(</m:mo> <m:mn>2</m:mn> <m:mo>,</m:mo> <m:msqrt> <m:mn>6</m:mn> </m:msqrt> <m:mo stretchy=\\\"false\\\">)</m:mo> </m:mrow> </m:mrow> </m:mrow> </m:math> <jats:inline-graphic xmlns:xlink=\\\"http://www.w3.org/1999/xlink\\\" xlink:href=\\\"graphic/j_gmj-2024-2035_eq_0178.png\\\"/> <jats:tex-math>{k\\\\in(0,\\\\sqrt{2})\\\\cup(2,\\\\sqrt{6})}</jats:tex-math> </jats:alternatives> </jats:inline-formula> for the exterior Dirichlet problem.\",\"PeriodicalId\":55101,\"journal\":{\"name\":\"Georgian Mathematical Journal\",\"volume\":null,\"pages\":null},\"PeriodicalIF\":0.8000,\"publicationDate\":\"2024-06-25\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Georgian Mathematical Journal\",\"FirstCategoryId\":\"100\",\"ListUrlMain\":\"https://doi.org/10.1515/gmj-2024-2035\",\"RegionNum\":4,\"RegionCategory\":\"数学\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q2\",\"JCRName\":\"MATHEMATICS\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Georgian Mathematical Journal","FirstCategoryId":"100","ListUrlMain":"https://doi.org/10.1515/gmj-2024-2035","RegionNum":4,"RegionCategory":"数学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"MATHEMATICS","Score":null,"Total":0}
We consider propagation of two-dimensional waves on the infinite hexagonal (honeycomb) lattice. Namely, we study the discrete Helmholtz equation in hexagonal lattices without and with a boundary. It is shown that for some configurations these problems can be equivalently reduced to similar problems for the triangular lattice. Based on this fact, new results are obtained for the existence and uniqueness of the solution in the case of the real wave number k∈(0,6)∖{2,3,2}{k\in(0,\sqrt{6})\setminus\{\sqrt{2},\sqrt{3},2\}} for the non-homogeneous Helmholtz equation in hexagonal lattices with no boundaries and the real wave number k∈(0,2)∪(2,6){k\in(0,\sqrt{2})\cup(2,\sqrt{6})} for the exterior Dirichlet problem.
期刊介绍:
The Georgian Mathematical Journal was founded by the Georgian National Academy of Sciences and A. Razmadze Mathematical Institute, and is jointly produced with De Gruyter. The concern of this international journal is the publication of research articles of best scientific standard in pure and applied mathematics. Special emphasis is put on the presentation of results obtained by Georgian mathematicians.