微扰QCD方法中的无粲准二体衰变:以实例为例

IF 1.5 4区 物理与天体物理 Q3 PHYSICS, PARTICLES & FIELDS Advances in High Energy Physics Pub Date : 2022-02-22 DOI:10.1155/2022/5287693
Wen-Feng Liu, Zhi-Tian Zou, Ying Li
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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":null,"pages":null},"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\":null,\"pages\":null},\"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}
引用次数: 0

摘要

三体衰变不仅大大拓宽了介子衰变机制的研究,而且提供了共振粒子的信息。由于动力学的复杂性,我们很难用一种特定的方法来研究整个相空间。本文以衰变为例,介绍了微扰QCD (PQCD)方法在准二体衰变中的应用。在准二体衰变中,两个粒子以大能量共线运动,其中一个粒子反冲。为了描述两个共线粒子的动力学,引入了具有不同波的卡子对的、、和-波函数。通过保持横向动量,PQCD方法可以计算出所有可能的图,包括硬旁观者图和湮灭图。大多数结果与目前BaBar, Belle和LHCb实验的测量结果一致。此外,在窄宽度近似下,我们可以提取涉及共振态的两体衰变的分支分数,并预测相应的准两体衰变的分支分数。所有的预测都将在正在进行的LHCb和Belle-II实验中得到验证。
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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.
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来源期刊
Advances in High Energy Physics
Advances in High Energy Physics PHYSICS, PARTICLES & FIELDS-
CiteScore
3.40
自引率
5.90%
发文量
55
审稿时长
6-12 weeks
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.
期刊最新文献
Statistical Issues on the Neutrino Mass Hierarchy with Determination of the Energy Eigenvalues of the Varshni-Hellmann Potential Hint for a Minimal Interaction Length in Annihilation in Total Cross Section of Center-of-Mass Energies 55-207 GeV Dissociation of and Using Dissociation Energy Criteria in -Dimensional Space Creation Field Cosmological Model with Variable Cosmological Term () in Bianchi Type III Space-Time
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