{"title":"有限代数量子场论","authors":"A. D. Alhaidari","doi":"arxiv-2407.14524","DOIUrl":null,"url":null,"abstract":"Based on a recently proposed quantum field theory (QFT) for particles with or\nwithout structure, called \"Structural Algebraic QFT (SAQFT)\", we introduce a\nfinite QFT. That is, a QFT for structureless elementary particles that does not\nrequire renormalization where loop integrals in the Feynman diagrams are\nfinite. It is an algebraic theory utilizing orthogonal polynomials and based on\nthe structureless sector of SAQFT.","PeriodicalId":501190,"journal":{"name":"arXiv - PHYS - General Physics","volume":"9 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-07-07","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Finite Algebraic Quantum Field Theory\",\"authors\":\"A. D. Alhaidari\",\"doi\":\"arxiv-2407.14524\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Based on a recently proposed quantum field theory (QFT) for particles with or\\nwithout structure, called \\\"Structural Algebraic QFT (SAQFT)\\\", we introduce a\\nfinite QFT. That is, a QFT for structureless elementary particles that does not\\nrequire renormalization where loop integrals in the Feynman diagrams are\\nfinite. It is an algebraic theory utilizing orthogonal polynomials and based on\\nthe structureless sector of SAQFT.\",\"PeriodicalId\":501190,\"journal\":{\"name\":\"arXiv - PHYS - General Physics\",\"volume\":\"9 1\",\"pages\":\"\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2024-07-07\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"arXiv - PHYS - General Physics\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/arxiv-2407.14524\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"arXiv - PHYS - General Physics","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/arxiv-2407.14524","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Based on a recently proposed quantum field theory (QFT) for particles with or
without structure, called "Structural Algebraic QFT (SAQFT)", we introduce a
finite QFT. That is, a QFT for structureless elementary particles that does not
require renormalization where loop integrals in the Feynman diagrams are
finite. It is an algebraic theory utilizing orthogonal polynomials and based on
the structureless sector of SAQFT.