{"title":"微扰QCD方法中的无粲准二体衰变:以实例为例","authors":"Wen-Feng Liu, Zhi-Tian Zou, Ying Li","doi":"10.1155/2022/5287693","DOIUrl":null,"url":null,"abstract":"Three-body <svg height=\"8.68572pt\" style=\"vertical-align:-0.0498209pt\" version=\"1.1\" viewbox=\"-0.0498162 -8.6359 7.94191 8.68572\" width=\"7.94191pt\" xmlns=\"http://www.w3.org/2000/svg\" xmlns:xlink=\"http://www.w3.org/1999/xlink\"><g transform=\"matrix(.013,0,0,-0.013,0,0)\"><use xlink:href=\"#g113-67\"></use></g></svg> decays not only significantly broaden the study of <svg height=\"8.68572pt\" style=\"vertical-align:-0.0498209pt\" version=\"1.1\" viewbox=\"-0.0498162 -8.6359 7.94191 8.68572\" width=\"7.94191pt\" xmlns=\"http://www.w3.org/2000/svg\" xmlns:xlink=\"http://www.w3.org/1999/xlink\"><g transform=\"matrix(.013,0,0,-0.013,0,0)\"><use xlink:href=\"#g113-67\"></use></g></svg> meson decay mechanisms but also provide information of resonant particles. Because of complicate dynamics, it is very hard for us to study the whole phase space in a specific approach. In this review, we take <span><svg height=\"13.0648pt\" style=\"vertical-align:-2.268101pt\" version=\"1.1\" viewbox=\"-0.0498162 -10.7967 29.623 13.0648\" width=\"29.623pt\" xmlns=\"http://www.w3.org/2000/svg\" xmlns:xlink=\"http://www.w3.org/1999/xlink\"><g transform=\"matrix(.013,0,0,-0.013,0,0)\"><use xlink:href=\"#g113-67\"></use></g><g transform=\"matrix(.013,0,0,-0.013,11.445,0)\"><use xlink:href=\"#g117-149\"></use></g><g transform=\"matrix(.013,0,0,-0.013,17.221,0)\"><use xlink:href=\"#g117-148\"></use></g></svg><span></span><svg height=\"13.0648pt\" style=\"vertical-align:-2.268101pt\" version=\"1.1\" viewbox=\"33.2821838 -10.7967 48.397 13.0648\" width=\"48.397pt\" xmlns=\"http://www.w3.org/2000/svg\" xmlns:xlink=\"http://www.w3.org/1999/xlink\"><g transform=\"matrix(.013,0,0,-0.013,33.332,0)\"><use xlink:href=\"#g113-76\"></use></g><g transform=\"matrix(.013,0,0,-0.013,43.149,0)\"><use xlink:href=\"#g113-41\"></use></g><g transform=\"matrix(.013,0,0,-0.013,47.647,0)\"><use xlink:href=\"#g198-19\"></use></g><g transform=\"matrix(.013,0,0,-0.013,63.551,0)\"><use xlink:href=\"#g117-149\"></use></g><g transform=\"matrix(.013,0,0,-0.013,69.327,0)\"><use xlink:href=\"#g117-148\"></use></g></svg><span></span><svg height=\"13.0648pt\" style=\"vertical-align:-2.268101pt\" version=\"1.1\" viewbox=\"81.7561838 -10.7967 36.603 13.0648\" width=\"36.603pt\" xmlns=\"http://www.w3.org/2000/svg\" xmlns:xlink=\"http://www.w3.org/1999/xlink\"><g transform=\"matrix(.013,0,0,-0.013,81.806,0)\"><use xlink:href=\"#g113-42\"></use></g><g transform=\"matrix(.013,0,0,-0.013,86.304,0)\"><use xlink:href=\"#g113-76\"></use></g><g transform=\"matrix(.0091,0,0,-0.0091,96.122,-5.741)\"><use xlink:href=\"#g54-36\"></use></g><g transform=\"matrix(.013,0,0,-0.013,102.201,0)\"><use xlink:href=\"#g113-76\"></use></g><g transform=\"matrix(.0091,0,0,-0.0091,112.018,-5.741)\"><use xlink:href=\"#g54-33\"></use></g></svg></span> decays as examples and show the application of the perturbative QCD (PQCD) approach in studying the quasi-two-body <svg height=\"8.68572pt\" style=\"vertical-align:-0.0498209pt\" version=\"1.1\" viewbox=\"-0.0498162 -8.6359 7.94191 8.68572\" width=\"7.94191pt\" xmlns=\"http://www.w3.org/2000/svg\" xmlns:xlink=\"http://www.w3.org/1999/xlink\"><g transform=\"matrix(.013,0,0,-0.013,0,0)\"><use xlink:href=\"#g113-67\"></use></g></svg> decays, where two particles move collinearly with large energy and the bachelor one recoils back. To describe the dynamics of two collinear particles, the <span><svg height=\"8.8423pt\" style=\"vertical-align:-0.2064009pt\" version=\"1.1\" viewbox=\"-0.0498162 -8.6359 6.25863 8.8423\" width=\"6.25863pt\" xmlns=\"http://www.w3.org/2000/svg\" xmlns:xlink=\"http://www.w3.org/1999/xlink\"><g transform=\"matrix(.013,0,0,-0.013,0,0)\"></path></g></svg>,</span> <span><svg height=\"8.68572pt\" style=\"vertical-align:-0.0498209pt\" version=\"1.1\" viewbox=\"-0.0498162 -8.6359 8.15071 8.68572\" width=\"8.15071pt\" xmlns=\"http://www.w3.org/2000/svg\" xmlns:xlink=\"http://www.w3.org/1999/xlink\"><g transform=\"matrix(.013,0,0,-0.013,0,0)\"></path></g></svg>,</span> and <span><svg height=\"8.68572pt\" style=\"vertical-align:-0.0498209pt\" version=\"1.1\" viewbox=\"-0.0498162 -8.6359 10.095 8.68572\" width=\"10.095pt\" xmlns=\"http://www.w3.org/2000/svg\" xmlns:xlink=\"http://www.w3.org/1999/xlink\"><g transform=\"matrix(.013,0,0,-0.013,0,0)\"></path></g></svg>-</span>wave functions of kaon-pair with different waves are introduced. By keeping the transverse momenta, all possible diagrams including the hard spectator diagrams and annihilation ones can be calculated in PQCD approach. Most results are well consistent with the current measurements from BaBar, Belle, and LHCb experiments. Moreover, under the narrow-width approximation, we can extract the branching fractions of the two-body decays involving the resonant states and also predict the branching fractions of the corresponding quasi-two-body decays <span><svg height=\"13.0648pt\" style=\"vertical-align:-2.268101pt\" version=\"1.1\" viewbox=\"-0.0498162 -10.7967 29.623 13.0648\" width=\"29.623pt\" xmlns=\"http://www.w3.org/2000/svg\" xmlns:xlink=\"http://www.w3.org/1999/xlink\"><g transform=\"matrix(.013,0,0,-0.013,0,0)\"><use xlink:href=\"#g113-67\"></use></g><g transform=\"matrix(.013,0,0,-0.013,11.445,0)\"><use xlink:href=\"#g117-149\"></use></g><g transform=\"matrix(.013,0,0,-0.013,17.221,0)\"><use xlink:href=\"#g117-148\"></use></g></svg><span></span><svg height=\"13.0648pt\" style=\"vertical-align:-2.268101pt\" version=\"1.1\" viewbox=\"33.2821838 -10.7967 48.397 13.0648\" width=\"48.397pt\" xmlns=\"http://www.w3.org/2000/svg\" xmlns:xlink=\"http://www.w3.org/1999/xlink\"><g transform=\"matrix(.013,0,0,-0.013,33.332,0)\"><use xlink:href=\"#g113-76\"></use></g><g transform=\"matrix(.013,0,0,-0.013,43.149,0)\"><use xlink:href=\"#g113-41\"></use></g><g transform=\"matrix(.013,0,0,-0.013,47.647,0)\"><use xlink:href=\"#g198-19\"></use></g><g transform=\"matrix(.013,0,0,-0.013,63.551,0)\"><use xlink:href=\"#g117-149\"></use></g><g transform=\"matrix(.013,0,0,-0.013,69.327,0)\"><use xlink:href=\"#g117-148\"></use></g></svg><span></span><span><svg height=\"13.0648pt\" style=\"vertical-align:-2.268101pt\" version=\"1.1\" viewbox=\"81.7561838 -10.7967 32.323 13.0648\" width=\"32.323pt\" xmlns=\"http://www.w3.org/2000/svg\" xmlns:xlink=\"http://www.w3.org/1999/xlink\"><g transform=\"matrix(.013,0,0,-0.013,81.806,0)\"><use xlink:href=\"#g113-42\"></use></g><g transform=\"matrix(.013,0,0,-0.013,86.304,0)\"></path></g><g transform=\"matrix(.0091,0,0,-0.0091,93.989,-5.741)\"><use xlink:href=\"#g54-36\"></use></g><g transform=\"matrix(.013,0,0,-0.013,100.068,0)\"><use xlink:href=\"#g113-238\"></use></g><g transform=\"matrix(.0091,0,0,-0.0091,107.752,-5.741)\"><use xlink:href=\"#g54-33\"></use></g></svg>.</span></span> All predictions are expected to be tested in the ongoing LHCb and Belle-II experiments.","PeriodicalId":7498,"journal":{"name":"Advances in High Energy Physics","volume":"15 1","pages":""},"PeriodicalIF":1.5000,"publicationDate":"2022-02-22","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Charmless Quasi-Two-Body Decays in Perturbative QCD Approach: Taking as Examples\",\"authors\":\"Wen-Feng Liu, Zhi-Tian Zou, Ying Li\",\"doi\":\"10.1155/2022/5287693\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Three-body <svg height=\\\"8.68572pt\\\" style=\\\"vertical-align:-0.0498209pt\\\" version=\\\"1.1\\\" viewbox=\\\"-0.0498162 -8.6359 7.94191 8.68572\\\" width=\\\"7.94191pt\\\" xmlns=\\\"http://www.w3.org/2000/svg\\\" xmlns:xlink=\\\"http://www.w3.org/1999/xlink\\\"><g transform=\\\"matrix(.013,0,0,-0.013,0,0)\\\"><use xlink:href=\\\"#g113-67\\\"></use></g></svg> decays not only significantly broaden the study of <svg height=\\\"8.68572pt\\\" style=\\\"vertical-align:-0.0498209pt\\\" version=\\\"1.1\\\" viewbox=\\\"-0.0498162 -8.6359 7.94191 8.68572\\\" width=\\\"7.94191pt\\\" xmlns=\\\"http://www.w3.org/2000/svg\\\" xmlns:xlink=\\\"http://www.w3.org/1999/xlink\\\"><g transform=\\\"matrix(.013,0,0,-0.013,0,0)\\\"><use xlink:href=\\\"#g113-67\\\"></use></g></svg> meson decay mechanisms but also provide information of resonant particles. Because of complicate dynamics, it is very hard for us to study the whole phase space in a specific approach. In this review, we take <span><svg height=\\\"13.0648pt\\\" style=\\\"vertical-align:-2.268101pt\\\" version=\\\"1.1\\\" viewbox=\\\"-0.0498162 -10.7967 29.623 13.0648\\\" width=\\\"29.623pt\\\" xmlns=\\\"http://www.w3.org/2000/svg\\\" xmlns:xlink=\\\"http://www.w3.org/1999/xlink\\\"><g transform=\\\"matrix(.013,0,0,-0.013,0,0)\\\"><use xlink:href=\\\"#g113-67\\\"></use></g><g transform=\\\"matrix(.013,0,0,-0.013,11.445,0)\\\"><use xlink:href=\\\"#g117-149\\\"></use></g><g transform=\\\"matrix(.013,0,0,-0.013,17.221,0)\\\"><use xlink:href=\\\"#g117-148\\\"></use></g></svg><span></span><svg height=\\\"13.0648pt\\\" style=\\\"vertical-align:-2.268101pt\\\" version=\\\"1.1\\\" viewbox=\\\"33.2821838 -10.7967 48.397 13.0648\\\" width=\\\"48.397pt\\\" xmlns=\\\"http://www.w3.org/2000/svg\\\" xmlns:xlink=\\\"http://www.w3.org/1999/xlink\\\"><g transform=\\\"matrix(.013,0,0,-0.013,33.332,0)\\\"><use xlink:href=\\\"#g113-76\\\"></use></g><g transform=\\\"matrix(.013,0,0,-0.013,43.149,0)\\\"><use xlink:href=\\\"#g113-41\\\"></use></g><g transform=\\\"matrix(.013,0,0,-0.013,47.647,0)\\\"><use xlink:href=\\\"#g198-19\\\"></use></g><g transform=\\\"matrix(.013,0,0,-0.013,63.551,0)\\\"><use xlink:href=\\\"#g117-149\\\"></use></g><g transform=\\\"matrix(.013,0,0,-0.013,69.327,0)\\\"><use xlink:href=\\\"#g117-148\\\"></use></g></svg><span></span><svg height=\\\"13.0648pt\\\" style=\\\"vertical-align:-2.268101pt\\\" version=\\\"1.1\\\" viewbox=\\\"81.7561838 -10.7967 36.603 13.0648\\\" width=\\\"36.603pt\\\" xmlns=\\\"http://www.w3.org/2000/svg\\\" xmlns:xlink=\\\"http://www.w3.org/1999/xlink\\\"><g transform=\\\"matrix(.013,0,0,-0.013,81.806,0)\\\"><use xlink:href=\\\"#g113-42\\\"></use></g><g transform=\\\"matrix(.013,0,0,-0.013,86.304,0)\\\"><use xlink:href=\\\"#g113-76\\\"></use></g><g transform=\\\"matrix(.0091,0,0,-0.0091,96.122,-5.741)\\\"><use xlink:href=\\\"#g54-36\\\"></use></g><g transform=\\\"matrix(.013,0,0,-0.013,102.201,0)\\\"><use xlink:href=\\\"#g113-76\\\"></use></g><g transform=\\\"matrix(.0091,0,0,-0.0091,112.018,-5.741)\\\"><use xlink:href=\\\"#g54-33\\\"></use></g></svg></span> decays as examples and show the application of the perturbative QCD (PQCD) approach in studying the quasi-two-body <svg height=\\\"8.68572pt\\\" style=\\\"vertical-align:-0.0498209pt\\\" version=\\\"1.1\\\" viewbox=\\\"-0.0498162 -8.6359 7.94191 8.68572\\\" width=\\\"7.94191pt\\\" xmlns=\\\"http://www.w3.org/2000/svg\\\" xmlns:xlink=\\\"http://www.w3.org/1999/xlink\\\"><g transform=\\\"matrix(.013,0,0,-0.013,0,0)\\\"><use xlink:href=\\\"#g113-67\\\"></use></g></svg> decays, where two particles move collinearly with large energy and the bachelor one recoils back. To describe the dynamics of two collinear particles, the <span><svg height=\\\"8.8423pt\\\" style=\\\"vertical-align:-0.2064009pt\\\" version=\\\"1.1\\\" viewbox=\\\"-0.0498162 -8.6359 6.25863 8.8423\\\" width=\\\"6.25863pt\\\" xmlns=\\\"http://www.w3.org/2000/svg\\\" xmlns:xlink=\\\"http://www.w3.org/1999/xlink\\\"><g transform=\\\"matrix(.013,0,0,-0.013,0,0)\\\"></path></g></svg>,</span> <span><svg height=\\\"8.68572pt\\\" style=\\\"vertical-align:-0.0498209pt\\\" version=\\\"1.1\\\" viewbox=\\\"-0.0498162 -8.6359 8.15071 8.68572\\\" width=\\\"8.15071pt\\\" xmlns=\\\"http://www.w3.org/2000/svg\\\" xmlns:xlink=\\\"http://www.w3.org/1999/xlink\\\"><g transform=\\\"matrix(.013,0,0,-0.013,0,0)\\\"></path></g></svg>,</span> and <span><svg height=\\\"8.68572pt\\\" style=\\\"vertical-align:-0.0498209pt\\\" version=\\\"1.1\\\" viewbox=\\\"-0.0498162 -8.6359 10.095 8.68572\\\" width=\\\"10.095pt\\\" xmlns=\\\"http://www.w3.org/2000/svg\\\" xmlns:xlink=\\\"http://www.w3.org/1999/xlink\\\"><g transform=\\\"matrix(.013,0,0,-0.013,0,0)\\\"></path></g></svg>-</span>wave functions of kaon-pair with different waves are introduced. By keeping the transverse momenta, all possible diagrams including the hard spectator diagrams and annihilation ones can be calculated in PQCD approach. Most results are well consistent with the current measurements from BaBar, Belle, and LHCb experiments. Moreover, under the narrow-width approximation, we can extract the branching fractions of the two-body decays involving the resonant states and also predict the branching fractions of the corresponding quasi-two-body decays <span><svg height=\\\"13.0648pt\\\" style=\\\"vertical-align:-2.268101pt\\\" version=\\\"1.1\\\" viewbox=\\\"-0.0498162 -10.7967 29.623 13.0648\\\" width=\\\"29.623pt\\\" xmlns=\\\"http://www.w3.org/2000/svg\\\" xmlns:xlink=\\\"http://www.w3.org/1999/xlink\\\"><g transform=\\\"matrix(.013,0,0,-0.013,0,0)\\\"><use xlink:href=\\\"#g113-67\\\"></use></g><g transform=\\\"matrix(.013,0,0,-0.013,11.445,0)\\\"><use xlink:href=\\\"#g117-149\\\"></use></g><g transform=\\\"matrix(.013,0,0,-0.013,17.221,0)\\\"><use xlink:href=\\\"#g117-148\\\"></use></g></svg><span></span><svg height=\\\"13.0648pt\\\" style=\\\"vertical-align:-2.268101pt\\\" version=\\\"1.1\\\" viewbox=\\\"33.2821838 -10.7967 48.397 13.0648\\\" width=\\\"48.397pt\\\" xmlns=\\\"http://www.w3.org/2000/svg\\\" xmlns:xlink=\\\"http://www.w3.org/1999/xlink\\\"><g transform=\\\"matrix(.013,0,0,-0.013,33.332,0)\\\"><use xlink:href=\\\"#g113-76\\\"></use></g><g transform=\\\"matrix(.013,0,0,-0.013,43.149,0)\\\"><use xlink:href=\\\"#g113-41\\\"></use></g><g transform=\\\"matrix(.013,0,0,-0.013,47.647,0)\\\"><use xlink:href=\\\"#g198-19\\\"></use></g><g transform=\\\"matrix(.013,0,0,-0.013,63.551,0)\\\"><use xlink:href=\\\"#g117-149\\\"></use></g><g transform=\\\"matrix(.013,0,0,-0.013,69.327,0)\\\"><use xlink:href=\\\"#g117-148\\\"></use></g></svg><span></span><span><svg height=\\\"13.0648pt\\\" style=\\\"vertical-align:-2.268101pt\\\" version=\\\"1.1\\\" viewbox=\\\"81.7561838 -10.7967 32.323 13.0648\\\" width=\\\"32.323pt\\\" xmlns=\\\"http://www.w3.org/2000/svg\\\" xmlns:xlink=\\\"http://www.w3.org/1999/xlink\\\"><g transform=\\\"matrix(.013,0,0,-0.013,81.806,0)\\\"><use xlink:href=\\\"#g113-42\\\"></use></g><g transform=\\\"matrix(.013,0,0,-0.013,86.304,0)\\\"></path></g><g transform=\\\"matrix(.0091,0,0,-0.0091,93.989,-5.741)\\\"><use xlink:href=\\\"#g54-36\\\"></use></g><g transform=\\\"matrix(.013,0,0,-0.013,100.068,0)\\\"><use xlink:href=\\\"#g113-238\\\"></use></g><g transform=\\\"matrix(.0091,0,0,-0.0091,107.752,-5.741)\\\"><use xlink:href=\\\"#g54-33\\\"></use></g></svg>.</span></span> All predictions are expected to be tested in the ongoing LHCb and Belle-II experiments.\",\"PeriodicalId\":7498,\"journal\":{\"name\":\"Advances in High Energy Physics\",\"volume\":\"15 1\",\"pages\":\"\"},\"PeriodicalIF\":1.5000,\"publicationDate\":\"2022-02-22\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Advances in High Energy Physics\",\"FirstCategoryId\":\"101\",\"ListUrlMain\":\"https://doi.org/10.1155/2022/5287693\",\"RegionNum\":4,\"RegionCategory\":\"物理与天体物理\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q3\",\"JCRName\":\"PHYSICS, PARTICLES & FIELDS\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Advances in High Energy Physics","FirstCategoryId":"101","ListUrlMain":"https://doi.org/10.1155/2022/5287693","RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q3","JCRName":"PHYSICS, PARTICLES & FIELDS","Score":null,"Total":0}
Charmless Quasi-Two-Body Decays in Perturbative QCD Approach: Taking as Examples
Three-body decays not only significantly broaden the study of meson decay mechanisms but also provide information of resonant particles. Because of complicate dynamics, it is very hard for us to study the whole phase space in a specific approach. In this review, we take decays as examples and show the application of the perturbative QCD (PQCD) approach in studying the quasi-two-body decays, where two particles move collinearly with large energy and the bachelor one recoils back. To describe the dynamics of two collinear particles, the ,, and -wave functions of kaon-pair with different waves are introduced. By keeping the transverse momenta, all possible diagrams including the hard spectator diagrams and annihilation ones can be calculated in PQCD approach. Most results are well consistent with the current measurements from BaBar, Belle, and LHCb experiments. Moreover, under the narrow-width approximation, we can extract the branching fractions of the two-body decays involving the resonant states and also predict the branching fractions of the corresponding quasi-two-body decays . All predictions are expected to be tested in the ongoing LHCb and Belle-II experiments.
期刊介绍:
Advances in High Energy Physics publishes the results of theoretical and experimental research on the nature of, and interaction between, energy and matter. Considering both original research and focussed review articles, the journal welcomes submissions from small research groups and large consortia alike.