{"title":"理论","authors":"Michael Kellmann, S. Kölling)","doi":"10.4324/9780429423857-2","DOIUrl":null,"url":null,"abstract":". This paper gives an introduction to the theory of oscillatory integrals of the first kind. Due to the complexity and multiplicity of critical points in higher dimensions, the decay of | I ( λ ) | in R d with d > 1 is far from clear-cut. However, using the method of stationary phase, one can establish an explicit decay property of the oscillatory integral in certain cases. We will first prove decay of | I ( λ ) | in the more straightforward case in which the phase function does not have a critical point. Next, we will analyze the case of a nondegenerate critical point and demonstrate some applications of oscillatory integrals in the study of partial differential equations.","PeriodicalId":418981,"journal":{"name":"Recovery and Stress in Sport","volume":"45 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2019-03-19","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Theory\",\"authors\":\"Michael Kellmann, S. Kölling)\",\"doi\":\"10.4324/9780429423857-2\",\"DOIUrl\":null,\"url\":null,\"abstract\":\". This paper gives an introduction to the theory of oscillatory integrals of the first kind. Due to the complexity and multiplicity of critical points in higher dimensions, the decay of | I ( λ ) | in R d with d > 1 is far from clear-cut. However, using the method of stationary phase, one can establish an explicit decay property of the oscillatory integral in certain cases. We will first prove decay of | I ( λ ) | in the more straightforward case in which the phase function does not have a critical point. Next, we will analyze the case of a nondegenerate critical point and demonstrate some applications of oscillatory integrals in the study of partial differential equations.\",\"PeriodicalId\":418981,\"journal\":{\"name\":\"Recovery and Stress in Sport\",\"volume\":\"45 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2019-03-19\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Recovery and Stress in Sport\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.4324/9780429423857-2\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Recovery and Stress in Sport","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.4324/9780429423857-2","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
. This paper gives an introduction to the theory of oscillatory integrals of the first kind. Due to the complexity and multiplicity of critical points in higher dimensions, the decay of | I ( λ ) | in R d with d > 1 is far from clear-cut. However, using the method of stationary phase, one can establish an explicit decay property of the oscillatory integral in certain cases. We will first prove decay of | I ( λ ) | in the more straightforward case in which the phase function does not have a critical point. Next, we will analyze the case of a nondegenerate critical point and demonstrate some applications of oscillatory integrals in the study of partial differential equations.