{"title":"Hint for a Minimal Interaction Length in Annihilation in Total Cross Section of Center-of-Mass Energies 55-207 GeV","authors":"Yutao Chen, Minghui Liu, Jürgen Ulbricht","doi":"10.1155/2024/9755683","DOIUrl":null,"url":null,"abstract":"The measurements of the total cross section of the <span><svg height=\"14.2262pt\" style=\"vertical-align:-3.429501pt\" version=\"1.1\" viewbox=\"-0.0498162 -10.7967 44.732 14.2262\" width=\"44.732pt\" 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=\"#g113-102\"></use></g><g transform=\"matrix(.0091,0,0,-0.0091,5.382,-5.741)\"><use xlink:href=\"#g54-36\"></use></g><g transform=\"matrix(.013,0,0,-0.013,11.461,0)\"><use xlink:href=\"#g113-102\"></use></g><g transform=\"matrix(.0091,0,0,-0.0091,16.844,-5.741)\"><use xlink:href=\"#g54-33\"></use></g><g transform=\"matrix(.013,0,0,-0.013,26.554,0)\"><use xlink:href=\"#g117-149\"></use></g><g transform=\"matrix(.013,0,0,-0.013,32.33,0)\"><use xlink:href=\"#g117-148\"></use></g></svg><span></span><svg height=\"14.2262pt\" style=\"vertical-align:-3.429501pt\" version=\"1.1\" viewbox=\"48.3921838 -10.7967 28.781 14.2262\" width=\"28.781pt\" xmlns=\"http://www.w3.org/2000/svg\" xmlns:xlink=\"http://www.w3.org/1999/xlink\"><g transform=\"matrix(.013,0,0,-0.013,48.442,0)\"><use xlink:href=\"#g113-225\"></use></g><g transform=\"matrix(.013,0,0,-0.013,54.958,0)\"><use xlink:href=\"#g113-225\"></use></g><g transform=\"matrix(.013,0,0,-0.013,61.474,0)\"></path></g><g transform=\"matrix(.013,0,0,-0.013,65.972,0)\"><use xlink:href=\"#g113-225\"></use></g><g transform=\"matrix(.013,0,0,-0.013,72.488,0)\"></path></g></svg></span> reaction from the VENUS, TOPAS, OPAL, DELPHI, ALEPH, and L3 collaborations, collected between 1989 and 2003, are used to perform a <svg height=\"15.2296pt\" style=\"vertical-align:-3.6382pt\" version=\"1.1\" viewbox=\"-0.0498162 -11.5914 12.6404 15.2296\" width=\"12.6404pt\" 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><g transform=\"matrix(.0091,0,0,-0.0091,7.568,-5.741)\"></path></g></svg> test to validate the current quantum electrodynamics (QED) theory and search for possible deviations with the direct contact term annihilation. By observing a deviation from the QED predictions on the total cross section of the <span><svg height=\"14.2262pt\" style=\"vertical-align:-3.429501pt\" version=\"1.1\" viewbox=\"-0.0498162 -10.7967 44.732 14.2262\" width=\"44.732pt\" 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=\"#g113-102\"></use></g><g transform=\"matrix(.0091,0,0,-0.0091,5.382,-5.741)\"><use xlink:href=\"#g54-36\"></use></g><g transform=\"matrix(.013,0,0,-0.013,11.461,0)\"><use xlink:href=\"#g113-102\"></use></g><g transform=\"matrix(.0091,0,0,-0.0091,16.844,-5.741)\"><use xlink:href=\"#g54-33\"></use></g><g transform=\"matrix(.013,0,0,-0.013,26.554,0)\"><use xlink:href=\"#g117-149\"></use></g><g transform=\"matrix(.013,0,0,-0.013,32.33,0)\"><use xlink:href=\"#g117-148\"></use></g></svg><span></span><svg height=\"14.2262pt\" style=\"vertical-align:-3.429501pt\" version=\"1.1\" viewbox=\"48.3921838 -10.7967 28.781 14.2262\" width=\"28.781pt\" xmlns=\"http://www.w3.org/2000/svg\" xmlns:xlink=\"http://www.w3.org/1999/xlink\"><g transform=\"matrix(.013,0,0,-0.013,48.442,0)\"><use xlink:href=\"#g113-225\"></use></g><g transform=\"matrix(.013,0,0,-0.013,54.958,0)\"><use xlink:href=\"#g113-225\"></use></g><g transform=\"matrix(.013,0,0,-0.013,61.474,0)\"><use xlink:href=\"#g113-41\"></use></g><g transform=\"matrix(.013,0,0,-0.013,65.972,0)\"><use xlink:href=\"#g113-225\"></use></g><g transform=\"matrix(.013,0,0,-0.013,72.488,0)\"><use xlink:href=\"#g113-42\"></use></g></svg></span> reaction above <span><svg height=\"13.1484pt\" style=\"vertical-align:-2.636801pt\" version=\"1.1\" viewbox=\"-0.0498162 -10.5116 26.125 13.1484\" width=\"26.125pt\" xmlns=\"http://www.w3.org/2000/svg\" xmlns:xlink=\"http://www.w3.org/1999/xlink\"><g transform=\"matrix(.013,0,0,-0.013,0,-.271)\"></path></g><rect height=\"0.65243\" width=\"4.89327\" x=\"9.96925\" y=\"-9.80939\"></rect><g transform=\"matrix(.013,0,0,-0.013,9.969,0)\"></path></g><g transform=\"matrix(.013,0,0,-0.013,18.494,0)\"></path></g></svg><span></span><svg height=\"13.1484pt\" style=\"vertical-align:-2.636801pt\" version=\"1.1\" viewbox=\"29.707183800000003 -10.5116 28.157 13.1484\" width=\"28.157pt\" xmlns=\"http://www.w3.org/2000/svg\" xmlns:xlink=\"http://www.w3.org/1999/xlink\"><g transform=\"matrix(.013,0,0,-0.013,29.757,0)\"></path></g><g transform=\"matrix(.013,0,0,-0.013,35.997,0)\"></path></g><g transform=\"matrix(.013,0,0,-0.013,42.237,0)\"></path></g><g transform=\"matrix(.013,0,0,-0.013,48.477,0)\"></path></g><g transform=\"matrix(.013,0,0,-0.013,51.441,0)\"><use xlink:href=\"#g113-49\"></use></g></svg></span> GeV, a non-QED direct contact term is introduced following the dimension 6 effective theory to explain the deviation. In the non-QED direct contact term, a threshold energy scale <svg height=\"8.68572pt\" style=\"vertical-align:-0.0498209pt\" version=\"1.1\" viewbox=\"-0.0498162 -8.6359 9.05107 8.68572\" width=\"9.05107pt\" 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> is included and explained to the finite interaction length in direct contact term and in consequence the size of the electron involved in the annihilation area. The experimental data of the total cross section is compared to the QED cross section by a <svg height=\"15.2296pt\" style=\"vertical-align:-3.6382pt\" version=\"1.1\" viewbox=\"-0.0498162 -11.5914 12.6404 15.2296\" width=\"12.6404pt\" 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=\"#g113-244\"></use></g><g transform=\"matrix(.0091,0,0,-0.0091,7.568,-5.741)\"><use xlink:href=\"#g50-51\"></use></g></svg> test, which gives a best fit of the <svg height=\"8.68572pt\" style=\"vertical-align:-0.0498209pt\" version=\"1.1\" viewbox=\"-0.0498162 -8.6359 9.05107 8.68572\" width=\"9.05107pt\" 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=\"#g113-140\"></use></g></svg> to be <span><svg height=\"8.69875pt\" style=\"vertical-align:-0.3499298pt\" version=\"1.1\" viewbox=\"-0.0498162 -8.34882 35.499 8.69875\" width=\"35.499pt\" 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=\"#g113-50\"></use></g><g transform=\"matrix(.013,0,0,-0.013,6.24,0)\"></path></g><g transform=\"matrix(.013,0,0,-0.013,12.48,0)\"></path></g><g transform=\"matrix(.013,0,0,-0.013,18.722,0)\"></path></g><g transform=\"matrix(.013,0,0,-0.013,27.868,0)\"></path></g></svg><span></span><svg height=\"8.69875pt\" style=\"vertical-align:-0.3499298pt\" version=\"1.1\" viewbox=\"38.3551838 -8.34882 19.009 8.69875\" width=\"19.009pt\" xmlns=\"http://www.w3.org/2000/svg\" xmlns:xlink=\"http://www.w3.org/1999/xlink\"><g transform=\"matrix(.013,0,0,-0.013,38.405,0)\"></path></g><g transform=\"matrix(.013,0,0,-0.013,44.645,0)\"><use xlink:href=\"#g113-49\"></use></g><g transform=\"matrix(.013,0,0,-0.013,50.885,0)\"><use xlink:href=\"#g113-51\"></use></g></svg></span> GeV, corresponding to a finite interaction length of <span><svg height=\"14.8825pt\" style=\"vertical-align:-3.2911pt\" version=\"1.1\" viewbox=\"-0.0498162 -11.5914 20.517 14.8825\" width=\"20.517pt\" 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><g transform=\"matrix(.0091,0,0,-0.0091,4.901,3.132)\"></path></g><g transform=\"matrix(.013,0,0,-0.013,12.886,0)\"><use xlink:href=\"#g117-34\"></use></g></svg><span></span><svg height=\"14.8825pt\" style=\"vertical-align:-3.2911pt\" version=\"1.1\" viewbox=\"24.0981838 -11.5914 36.719 14.8825\" width=\"36.719pt\" xmlns=\"http://www.w3.org/2000/svg\" xmlns:xlink=\"http://www.w3.org/1999/xlink\"><g transform=\"matrix(.013,0,0,-0.013,24.148,0)\"><use xlink:href=\"#g113-41\"></use></g><g transform=\"matrix(.013,0,0,-0.013,28.646,0)\"><use xlink:href=\"#g113-50\"></use></g><g transform=\"matrix(.013,0,0,-0.013,34.886,0)\"><use xlink:href=\"#g113-47\"></use></g><g transform=\"matrix(.013,0,0,-0.013,37.85,0)\"><use xlink:href=\"#g113-51\"></use></g><g transform=\"matrix(.013,0,0,-0.013,44.09,0)\"><use xlink:href=\"#g113-54\"></use></g><g transform=\"matrix(.013,0,0,-0.013,53.236,0)\"><use xlink:href=\"#g117-37\"></use></g></svg><span></span><svg height=\"14.8825pt\" style=\"vertical-align:-3.2911pt\" version=\"1.1\" viewbox=\"63.7231838 -11.5914 36.718 14.8825\" width=\"36.718pt\" xmlns=\"http://www.w3.org/2000/svg\" xmlns:xlink=\"http://www.w3.org/1999/xlink\"><g transform=\"matrix(.013,0,0,-0.013,63.773,0)\"><use xlink:href=\"#g113-49\"></use></g><g transform=\"matrix(.013,0,0,-0.013,70.013,0)\"><use xlink:href=\"#g113-47\"></use></g><g transform=\"matrix(.013,0,0,-0.013,72.977,0)\"><use xlink:href=\"#g113-50\"></use></g><g transform=\"matrix(.013,0,0,-0.013,79.217,0)\"><use xlink:href=\"#g113-55\"></use></g><g transform=\"matrix(.013,0,0,-0.013,85.457,0)\"><use xlink:href=\"#g113-42\"></use></g><g transform=\"matrix(.013,0,0,-0.013,92.86,0)\"></path></g></svg><span></span><svg height=\"14.8825pt\" style=\"vertical-align:-3.2911pt\" version=\"1.1\" viewbox=\"103.34718380000001 -11.5914 27.902 14.8825\" width=\"27.902pt\" xmlns=\"http://www.w3.org/2000/svg\" xmlns:xlink=\"http://www.w3.org/1999/xlink\"><g transform=\"matrix(.013,0,0,-0.013,103.397,0)\"><use xlink:href=\"#g113-50\"></use></g><g transform=\"matrix(.013,0,0,-0.013,109.637,0)\"><use xlink:href=\"#g113-49\"></use></g><g transform=\"matrix(.0091,0,0,-0.0091,115.877,-5.741)\"><use xlink:href=\"#g54-33\"></use></g><g transform=\"matrix(.0091,0,0,-0.0091,121.437,-5.741)\"></path></g><g transform=\"matrix(.0091,0,0,-0.0091,125.869,-5.741)\"></path></g></svg></span> (cm). In the direct contact term annihilation, this interaction length is a measure of the size of an electron <span><svg height=\"9.25202pt\" style=\"vertical-align:-3.29111pt\" version=\"1.1\" viewbox=\"-0.0498162 -5.96091 9.37172 9.25202\" width=\"9.37172pt\" 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=\"#g113-115\"></use></g><g transform=\"matrix(.0091,0,0,-0.0091,4.901,3.132)\"><use xlink:href=\"#g50-102\"></use></g></svg>.</span> By combining all the data results from the mentioned collaborations, we have at least 2 to 3 times more statistics than every single experiment at high <svg height=\"13.1484pt\" style=\"vertical-align:-2.636801pt\" version=\"1.1\" viewbox=\"-0.0498162 -10.5116 14.9622 13.1484\" width=\"14.9622pt\" xmlns=\"http://www.w3.org/2000/svg\" xmlns:xlink=\"http://www.w3.org/1999/xlink\"><g transform=\"matrix(.013,0,0,-0.013,0,-.271)\"><use xlink:href=\"#g119-37\"></use></g><rect height=\"0.65243\" width=\"4.89327\" x=\"9.96925\" y=\"-9.80939\"></rect><g transform=\"matrix(.013,0,0,-0.013,9.969,0)\"><use xlink:href=\"#g113-116\"></use></g></svg> region. This induces the best precision on <svg height=\"9.25202pt\" style=\"vertical-align:-3.29111pt\" version=\"1.1\" viewbox=\"-0.0498162 -5.96091 9.37172 9.25202\" width=\"9.37172pt\" 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=\"#g113-115\"></use></g><g transform=\"matrix(.0091,0,0,-0.0091,4.901,3.132)\"><use xlink:href=\"#g50-102\"></use></g></svg> compared to the previous measurements.","PeriodicalId":7498,"journal":{"name":"Advances in High Energy Physics","volume":null,"pages":null},"PeriodicalIF":1.5000,"publicationDate":"2024-04-10","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/10.1155/2024/9755683","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
Abstract
The measurements of the total cross section of the reaction from the VENUS, TOPAS, OPAL, DELPHI, ALEPH, and L3 collaborations, collected between 1989 and 2003, are used to perform a test to validate the current quantum electrodynamics (QED) theory and search for possible deviations with the direct contact term annihilation. By observing a deviation from the QED predictions on the total cross section of the reaction above GeV, a non-QED direct contact term is introduced following the dimension 6 effective theory to explain the deviation. In the non-QED direct contact term, a threshold energy scale is included and explained to the finite interaction length in direct contact term and in consequence the size of the electron involved in the annihilation area. The experimental data of the total cross section is compared to the QED cross section by a test, which gives a best fit of the to be GeV, corresponding to a finite interaction length of (cm). In the direct contact term annihilation, this interaction length is a measure of the size of an electron . By combining all the data results from the mentioned collaborations, we have at least 2 to 3 times more statistics than every single experiment at high region. This induces the best precision on compared to the previous measurements.
1989年至2003年间,VENUS、TOPAS、OPAL、DELPHI、ALEPH和L3合作小组对反应总截面的测量结果被用来验证当前的量子电动力学(QED)理论,并寻找直接接触项湮灭的可能偏差。通过观察 GeV 以上反应总截面与 QED 预测的偏差,按照维度 6 有效理论引入了非 QED 直接接触项来解释这种偏差。在非 QED 直接接触项中,包含了一个阈值能量尺度,并解释了直接接触项中的有限相互作用长度,以及湮灭区域中电子的大小。总截面的实验数据通过测试与 QED 截面进行比较,得出最佳拟合值为 GeV,对应于(厘米)的有限相互作用长度。在直接接触项湮灭中,这个相互作用长度是电子大小的量度。通过综合上述合作的所有数据结果,我们在高区域的统计数据至少是每个实验的 2 到 3 倍。因此,与之前的测量相比,我们的测量精度是最高的。
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.