Jin Ma, Sheng-Quan Wang, Ting Sun, Jian-Ming Shen, Xing-Gang Wu
{"title":"在未来的 e + e - 对撞机上重新审视顶夸克对的产生* * 部分受国家自然科学基金(12175025、12147102、12265011)和贵州省厅项目(YQK[2023]016、ZK[2023]141、[2020]1Y027、GZMUZK[2022]PT01)资助","authors":"Jin Ma, Sheng-Quan Wang, Ting Sun, Jian-Ming Shen, Xing-Gang Wu","doi":"10.1088/1674-1137/ad243e","DOIUrl":null,"url":null,"abstract":"In this study, we reanalyze the top-quark pair production at next-to-next-to-leading order (NNLO) in quantum chromodynamics (QCD) at future <inline-formula>\n<tex-math><?CDATA $ e^+e^- $?></tex-math>\n<inline-graphic xlink:href=\"cpc_48_4_043105_M2.jpg\" xlink:type=\"simple\"></inline-graphic>\n</inline-formula> colliders using the Principle of Maximum Conformality (PMC) method. The PMC renormalization scales in <inline-formula>\n<tex-math><?CDATA $ \\alpha_s $?></tex-math>\n<inline-graphic xlink:href=\"cpc_48_4_043105_M3.jpg\" xlink:type=\"simple\"></inline-graphic>\n</inline-formula> are determined by absorbing the non-conformal <italic toggle=\"yes\">β</italic> terms by recursively using the Renormalization Group Equation (RGE). Unlike the conventional scale-setting method of fixing the scale at the center-of-mass energy <inline-formula>\n<tex-math><?CDATA $ \\mu_r=\\sqrt{s} $?></tex-math>\n<inline-graphic xlink:href=\"cpc_48_4_043105_M4.jpg\" xlink:type=\"simple\"></inline-graphic>\n</inline-formula>, the determined PMC scale <inline-formula>\n<tex-math><?CDATA $ Q_\\star $?></tex-math>\n<inline-graphic xlink:href=\"cpc_48_4_043105_M5.jpg\" xlink:type=\"simple\"></inline-graphic>\n</inline-formula> is far smaller than the <inline-formula>\n<tex-math><?CDATA $ \\sqrt{s} $?></tex-math>\n<inline-graphic xlink:href=\"cpc_48_4_043105_M6.jpg\" xlink:type=\"simple\"></inline-graphic>\n</inline-formula> and increases with the <inline-formula>\n<tex-math><?CDATA $ \\sqrt{s} $?></tex-math>\n<inline-graphic xlink:href=\"cpc_48_4_043105_M7.jpg\" xlink:type=\"simple\"></inline-graphic>\n</inline-formula>, yielding the correct physical behavior for the top-quark pair production process. Moreover, the convergence of the pQCD series for the top-quark pair production is greatly improved owing to the elimination of the renormalon divergence. For a typical collision energy of <inline-formula>\n<tex-math><?CDATA $ \\sqrt{s}=500 $?></tex-math>\n<inline-graphic xlink:href=\"cpc_48_4_043105_M8.jpg\" xlink:type=\"simple\"></inline-graphic>\n</inline-formula> GeV, the PMC scale is <inline-formula>\n<tex-math><?CDATA $ Q_\\star=107 $?></tex-math>\n<inline-graphic xlink:href=\"cpc_48_4_043105_M9.jpg\" xlink:type=\"simple\"></inline-graphic>\n</inline-formula> GeV; the QCD correction factor <italic toggle=\"yes\">K</italic> for conventional results is <inline-formula>\n<tex-math><?CDATA $ K\\sim1+0.1244^{+0.0102+0.0012}_{-0.0087-0.0011}+0.0184^{-0.0086+0.0002}_{+0.0061-0.0003} $?></tex-math>\n<inline-graphic xlink:href=\"cpc_48_4_043105_M10.jpg\" xlink:type=\"simple\"></inline-graphic>\n</inline-formula>, where the first error is caused by varying the scale <inline-formula>\n<tex-math><?CDATA $ \\mu_r\\in[\\sqrt{s}/2, 2\\sqrt{s}] $?></tex-math>\n<inline-graphic xlink:href=\"cpc_48_4_043105_M11.jpg\" xlink:type=\"simple\"></inline-graphic>\n</inline-formula> and the second error is from the top-quark mass <inline-formula>\n<tex-math><?CDATA $ \\Delta{m_t}=\\pm0.7 $?></tex-math>\n<inline-graphic xlink:href=\"cpc_48_4_043105_M12.jpg\" xlink:type=\"simple\"></inline-graphic>\n</inline-formula> GeV. After applying the PMC, the renormalization scale uncertainty is eliminated, and the QCD correction factor <italic toggle=\"yes\">K</italic> is improved to <inline-formula>\n<tex-math><?CDATA $ K\\sim 1+0.1507^{+0.0015}_{-0.0015}-0.0057^{+0.0001}_{-0.0000} $?></tex-math>\n<inline-graphic xlink:href=\"cpc_48_4_043105_M13.jpg\" xlink:type=\"simple\"></inline-graphic>\n</inline-formula>, where the error is from the top-quark mass <inline-formula>\n<tex-math><?CDATA $ \\Delta{m_t}=\\pm0.7 $?></tex-math>\n<inline-graphic xlink:href=\"cpc_48_4_043105_M14.jpg\" xlink:type=\"simple\"></inline-graphic>\n</inline-formula> GeV. The PMC improved predictions for the top-quark pair production are helpful for detailed studies of the properties of the top-quark at future <inline-formula>\n<tex-math><?CDATA $ e^+e^- $?></tex-math>\n<inline-graphic xlink:href=\"cpc_48_4_043105_M15.jpg\" xlink:type=\"simple\"></inline-graphic>\n</inline-formula> colliders.","PeriodicalId":10250,"journal":{"name":"中国物理C","volume":"40 1","pages":""},"PeriodicalIF":3.6000,"publicationDate":"2024-04-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Revisiting the top-quark pair production at future e + e − colliders* * Supported in part by the Natural Science Foundation of China (12175025, 12147102, 12265011), by the Projects of Guizhou Provincial Department (YQK[2023]016, ZK[2023]141, [2020]1Y027, GZMUZK[2022]PT01)\",\"authors\":\"Jin Ma, Sheng-Quan Wang, Ting Sun, Jian-Ming Shen, Xing-Gang Wu\",\"doi\":\"10.1088/1674-1137/ad243e\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"In this study, we reanalyze the top-quark pair production at next-to-next-to-leading order (NNLO) in quantum chromodynamics (QCD) at future <inline-formula>\\n<tex-math><?CDATA $ e^+e^- $?></tex-math>\\n<inline-graphic xlink:href=\\\"cpc_48_4_043105_M2.jpg\\\" xlink:type=\\\"simple\\\"></inline-graphic>\\n</inline-formula> colliders using the Principle of Maximum Conformality (PMC) method. The PMC renormalization scales in <inline-formula>\\n<tex-math><?CDATA $ \\\\alpha_s $?></tex-math>\\n<inline-graphic xlink:href=\\\"cpc_48_4_043105_M3.jpg\\\" xlink:type=\\\"simple\\\"></inline-graphic>\\n</inline-formula> are determined by absorbing the non-conformal <italic toggle=\\\"yes\\\">β</italic> terms by recursively using the Renormalization Group Equation (RGE). Unlike the conventional scale-setting method of fixing the scale at the center-of-mass energy <inline-formula>\\n<tex-math><?CDATA $ \\\\mu_r=\\\\sqrt{s} $?></tex-math>\\n<inline-graphic xlink:href=\\\"cpc_48_4_043105_M4.jpg\\\" xlink:type=\\\"simple\\\"></inline-graphic>\\n</inline-formula>, the determined PMC scale <inline-formula>\\n<tex-math><?CDATA $ Q_\\\\star $?></tex-math>\\n<inline-graphic xlink:href=\\\"cpc_48_4_043105_M5.jpg\\\" xlink:type=\\\"simple\\\"></inline-graphic>\\n</inline-formula> is far smaller than the <inline-formula>\\n<tex-math><?CDATA $ \\\\sqrt{s} $?></tex-math>\\n<inline-graphic xlink:href=\\\"cpc_48_4_043105_M6.jpg\\\" xlink:type=\\\"simple\\\"></inline-graphic>\\n</inline-formula> and increases with the <inline-formula>\\n<tex-math><?CDATA $ \\\\sqrt{s} $?></tex-math>\\n<inline-graphic xlink:href=\\\"cpc_48_4_043105_M7.jpg\\\" xlink:type=\\\"simple\\\"></inline-graphic>\\n</inline-formula>, yielding the correct physical behavior for the top-quark pair production process. 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For a typical collision energy of <inline-formula>\\n<tex-math><?CDATA $ \\\\sqrt{s}=500 $?></tex-math>\\n<inline-graphic xlink:href=\\\"cpc_48_4_043105_M8.jpg\\\" xlink:type=\\\"simple\\\"></inline-graphic>\\n</inline-formula> GeV, the PMC scale is <inline-formula>\\n<tex-math><?CDATA $ Q_\\\\star=107 $?></tex-math>\\n<inline-graphic xlink:href=\\\"cpc_48_4_043105_M9.jpg\\\" xlink:type=\\\"simple\\\"></inline-graphic>\\n</inline-formula> GeV; the QCD correction factor <italic toggle=\\\"yes\\\">K</italic> for conventional results is <inline-formula>\\n<tex-math><?CDATA $ K\\\\sim1+0.1244^{+0.0102+0.0012}_{-0.0087-0.0011}+0.0184^{-0.0086+0.0002}_{+0.0061-0.0003} $?></tex-math>\\n<inline-graphic xlink:href=\\\"cpc_48_4_043105_M10.jpg\\\" xlink:type=\\\"simple\\\"></inline-graphic>\\n</inline-formula>, where the first error is caused by varying the scale <inline-formula>\\n<tex-math><?CDATA $ \\\\mu_r\\\\in[\\\\sqrt{s}/2, 2\\\\sqrt{s}] $?></tex-math>\\n<inline-graphic xlink:href=\\\"cpc_48_4_043105_M11.jpg\\\" xlink:type=\\\"simple\\\"></inline-graphic>\\n</inline-formula> and the second error is from the top-quark mass <inline-formula>\\n<tex-math><?CDATA $ \\\\Delta{m_t}=\\\\pm0.7 $?></tex-math>\\n<inline-graphic xlink:href=\\\"cpc_48_4_043105_M12.jpg\\\" xlink:type=\\\"simple\\\"></inline-graphic>\\n</inline-formula> GeV. 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引用次数: 0
摘要
在本研究中,我们利用最大共形原理(PMC)方法,在未来对撞机上重新分析了量子色动力学(QCD)中次前阶(NNLO)的顶夸克对产生。PMC中的重正化尺度是通过递归使用重正化群方程(Renormalization Group Equation,RGE)吸收非共形β项来确定的。与将尺度固定在质量中心能量上的传统尺度设定方法不同,所确定的 PMC 尺度远远小于 ,并随着 ,的增大而增大,从而产生了正确的顶夸克对产生过程的物理行为。此外,由于消除了重正子发散,pQCD 序列对顶夸克对产生的收敛性大大提高。对于 GeV 的典型对撞能量,PMC 尺度为 GeV;传统结果的 QCD 修正系数 K 为 ,其中第一个误差由尺度变化引起,第二个误差来自顶夸克质量 GeV。应用 PMC 后,消除了重正化尺度的不确定性,QCD 修正系数 K 提高到 ,其中误差来自顶夸克质量 GeV。PMC对顶夸克对产生的改进预测有助于在未来对撞机上详细研究顶夸克的性质。
Revisiting the top-quark pair production at future e + e − colliders* * Supported in part by the Natural Science Foundation of China (12175025, 12147102, 12265011), by the Projects of Guizhou Provincial Department (YQK[2023]016, ZK[2023]141, [2020]1Y027, GZMUZK[2022]PT01)
In this study, we reanalyze the top-quark pair production at next-to-next-to-leading order (NNLO) in quantum chromodynamics (QCD) at future colliders using the Principle of Maximum Conformality (PMC) method. The PMC renormalization scales in are determined by absorbing the non-conformal β terms by recursively using the Renormalization Group Equation (RGE). Unlike the conventional scale-setting method of fixing the scale at the center-of-mass energy , the determined PMC scale is far smaller than the and increases with the , yielding the correct physical behavior for the top-quark pair production process. Moreover, the convergence of the pQCD series for the top-quark pair production is greatly improved owing to the elimination of the renormalon divergence. For a typical collision energy of GeV, the PMC scale is GeV; the QCD correction factor K for conventional results is , where the first error is caused by varying the scale and the second error is from the top-quark mass GeV. After applying the PMC, the renormalization scale uncertainty is eliminated, and the QCD correction factor K is improved to , where the error is from the top-quark mass GeV. The PMC improved predictions for the top-quark pair production are helpful for detailed studies of the properties of the top-quark at future colliders.
期刊介绍:
Chinese Physics C covers the latest developments and achievements in the theory, experiment and applications of:
Particle physics;
Nuclear physics;
Particle and nuclear astrophysics;
Cosmology;
Accelerator physics.
The journal publishes original research papers, letters and reviews. The Letters section covers short reports on the latest important scientific results, published as quickly as possible. Such breakthrough research articles are a high priority for publication.
The Editorial Board is composed of about fifty distinguished physicists, who are responsible for the review of submitted papers and who ensure the scientific quality of the journal.
The journal has been awarded the Chinese Academy of Sciences ‘Excellent Journal’ award multiple times, and is recognized as one of China''s top one hundred key scientific periodicals by the General Administration of News and Publications.