Hard processes in multi-TeV ion collisions

IF 5.3 2区 物理与天体物理 Q1 Physics and Astronomy
Benjamin Fuks, Fotios Marougkas, Richard Ruiz, Alicja Sztandera
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We focus on the symmetric beam configurations Pb</a:mi></a:mrow>208</a:mn></a:mrow></a:mmultiscripts></a:mrow>−</a:mtext>Pb</a:mi></a:mrow>208</a:mn></a:mrow></a:mmultiscripts></a:mrow></a:mrow></a:math>, <c:math xmlns:c=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><c:mrow><c:mrow><c:mmultiscripts><c:mrow><c:mi>Xe</c:mi></c:mrow><c:mprescripts/><c:none/><c:mrow><c:mn>131</c:mn></c:mrow></c:mmultiscripts></c:mrow><c:mtext>−</c:mtext><c:mrow><c:mmultiscripts><c:mrow><c:mi>Xe</c:mi></c:mrow><c:mprescripts/><c:none/><c:mrow><c:mn>131</c:mn></c:mrow></c:mmultiscripts></c:mrow></c:mrow></c:math>, <e:math xmlns:e=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><e:mrow><e:mrow><e:mmultiscripts><e:mrow><e:mi mathvariant=\"normal\">C</e:mi></e:mrow><e:mprescripts/><e:none/><e:mrow><e:mn>12</e:mn></e:mrow></e:mmultiscripts></e:mrow><e:mtext>−</e:mtext><e:mrow><e:mmultiscripts><e:mrow><e:mi mathvariant=\"normal\">C</e:mi></e:mrow><e:mprescripts/><e:none/><e:mrow><e:mn>12</e:mn></e:mrow></e:mmultiscripts></e:mrow></e:mrow></e:math>, and <i:math xmlns:i=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><i:mi>p</i:mi><i:mi>p</i:mi></i:math>, and we catalog total and fiducial cross sections for dozens of processes, ranging from associated-Higgs and multiboson production to associated-top pair production, at next-to-leading order in QCD for nucleon-nucleon collision energies from <k:math xmlns:k=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><k:msqrt><k:msub><k:mi>s</k:mi><k:mrow><k:mi>N</k:mi><k:mi>N</k:mi></k:mrow></k:msub></k:msqrt><k:mo>=</k:mo><k:mn>1</k:mn></k:math> to 100 TeV. We report the residual scale uncertainties at this order as well as the uncertainties originating from fits of nuclear parton densities. We also discuss the propagation of nuclear dynamics (as encoded in nuclear parton densities) into parton luminosities and ultimately into predictions for cross sections. Finally, we report on the emergence of trends and the reliability of extrapolating cross sections across different nuclei. For Pb-Pb collisions at a hypothetical Future Circular Collider with <m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><m:mrow><m:msqrt><m:mrow><m:msub><m:mrow><m:mi>s</m:mi></m:mrow><m:mrow><m:mi>N</m:mi><m:mi>N</m:mi></m:mrow></m:msub></m:mrow></m:msqrt><m:mo>=</m:mo><m:mn>39</m:mn><m:mtext> </m:mtext><m:mtext> </m:mtext><m:mi>TeV</m:mi></m:mrow></m:math>, <o:math xmlns:o=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><o:mi mathvariant=\"script\">O</o:mi><o:mo stretchy=\"false\">(</o:mo><o:msup><o:mn>10</o:mn><o:mn>8</o:mn></o:msup><o:mo stretchy=\"false\">)</o:mo></o:math> weak bosons, <t:math xmlns:t=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><t:mi mathvariant=\"script\">O</t:mi><t:mo stretchy=\"false\">(</t:mo><t:msup><t:mn>10</t:mn><t:mn>5</t:mn></t:msup><t:mo stretchy=\"false\">)</t:mo></t:math> diboson pairs, <y:math xmlns:y=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><y:mi mathvariant=\"script\">O</y:mi><y:mo stretchy=\"false\">(</y:mo><y:msup><y:mn>10</y:mn><y:mn>4</y:mn></y:msup><y:mo stretchy=\"false\">)</y:mo></y:math> <db:math xmlns:db=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><db:mi>W</db:mi><db:mi>H</db:mi></db:math> and <fb:math xmlns:fb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><fb:mi>Z</fb:mi><fb:mi>H</fb:mi></fb:math> pairs, <hb:math xmlns:hb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><hb:mi mathvariant=\"script\">O</hb:mi><hb:mo stretchy=\"false\">(</hb:mo><hb:msup><hb:mn>10</hb:mn><hb:mn>3</hb:mn></hb:msup><hb:mo stretchy=\"false\">)</hb:mo></hb:math> triboson events, <mb:math xmlns:mb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mb:mi mathvariant=\"script\">O</mb:mi><mb:mo stretchy=\"false\">(</mb:mo><mb:msup><mb:mn>10</mb:mn><mb:mn>5</mb:mn></mb:msup><mb:mo stretchy=\"false\">)</mb:mo></mb:math> high-<rb:math xmlns:rb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><rb:msub><rb:mi>p</rb:mi><rb:mi>T</rb:mi></rb:msub></rb:math> photons events, and <tb:math xmlns:tb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><tb:mi mathvariant=\"script\">O</tb:mi><tb:mo stretchy=\"false\">(</tb:mo><tb:msup><tb:mn>10</tb:mn><tb:mn>7</tb:mn></tb:msup><tb:mo stretchy=\"false\">)</tb:mo></tb:math> <yb:math xmlns:yb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><yb:mi>t</yb:mi><yb:mover accent=\"true\"><yb:mi>t</yb:mi><yb:mo stretchy=\"false\">¯</yb:mo></yb:mover></yb:math> pairs can be produced with <cc:math xmlns:cc=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><cc:mrow><cc:mi mathvariant=\"script\">L</cc:mi><cc:mo>=</cc:mo><cc:mn>33</cc:mn><cc:mtext> </cc:mtext><cc:mtext> </cc:mtext><cc:msup><cc:mrow><cc:mi>nb</cc:mi></cc:mrow><cc:mrow><cc:mo>−</cc:mo><cc:mn>1</cc:mn></cc:mrow></cc:msup></cc:mrow></cc:math> of data. At <fc:math xmlns:fc=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><fc:mrow><fc:msqrt><fc:mrow><fc:msub><fc:mrow><fc:mi>s</fc:mi></fc:mrow><fc:mrow><fc:mi>N</fc:mi><fc:mi>N</fc:mi></fc:mrow></fc:msub></fc:mrow></fc:msqrt><fc:mo>=</fc:mo><fc:mn>5.52</fc:mn><fc:mtext> </fc:mtext><fc:mtext> </fc:mtext><fc:mi>TeV</fc:mi></fc:mrow></fc:math>, one can expect <hc:math xmlns:hc=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><hc:mrow><hc:mi mathvariant=\"script\">O</hc:mi><hc:mo stretchy=\"false\">(</hc:mo><hc:mn>10</hc:mn><hc:mi>–</hc:mi><hc:msup><hc:mrow><hc:mn>10</hc:mn></hc:mrow><hc:mrow><hc:mn>6</hc:mn></hc:mrow></hc:msup><hc:mo stretchy=\"false\">)</hc:mo></hc:mrow></hc:math> single, multiboson, and top events per <mc:math xmlns:mc=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mc:mn>1</mc:mn><mc:mtext> </mc:mtext><mc:mtext> </mc:mtext><mc:msup><mc:mi>nb</mc:mi><mc:mrow><mc:mo>−</mc:mo><mc:mn>1</mc:mn></mc:mrow></mc:msup></mc:math>. Decay rates and experimental selection/acceptance rates will impact final event yields and merit further study; as an illustrative example, we focus on select diboson and triboson channels in lead-lead collisions and discuss their observability at the high-luminosity phase of the Large Hadron Collider and the Future Circulate Collider. <jats:supplementary-material> <jats:copyright-statement>Published by the American Physical Society</jats:copyright-statement> <jats:copyright-year>2025</jats:copyright-year> </jats:permissions> </jats:supplementary-material>","PeriodicalId":20167,"journal":{"name":"Physical Review D","volume":"51 1","pages":""},"PeriodicalIF":5.3000,"publicationDate":"2025-01-23","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Physical Review D","FirstCategoryId":"101","ListUrlMain":"https://doi.org/10.1103/physrevd.111.014025","RegionNum":2,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"Physics and Astronomy","Score":null,"Total":0}
引用次数: 0

Abstract

Motivated by the ion-collision program at the Large Hadron Collider, plans for its high-luminosity upgrade, and ongoing discussions for multi-TeV future hadron colliders, we systematically investigate hard-scattering, Standard Model processes in many-TeV ion-ion collisions. We focus on the symmetric beam configurations Pb208−Pb208, Xe131Xe131, C12C12, and pp, and we catalog total and fiducial cross sections for dozens of processes, ranging from associated-Higgs and multiboson production to associated-top pair production, at next-to-leading order in QCD for nucleon-nucleon collision energies from sNN=1 to 100 TeV. We report the residual scale uncertainties at this order as well as the uncertainties originating from fits of nuclear parton densities. We also discuss the propagation of nuclear dynamics (as encoded in nuclear parton densities) into parton luminosities and ultimately into predictions for cross sections. Finally, we report on the emergence of trends and the reliability of extrapolating cross sections across different nuclei. For Pb-Pb collisions at a hypothetical Future Circular Collider with sNN=39 TeV, O(108) weak bosons, O(105) diboson pairs, O(104) WH and ZH pairs, O(103) triboson events, O(105) high-pT photons events, and O(107) tt¯ pairs can be produced with L=33 nb1 of data. At sNN=5.52 TeV, one can expect O(10106) single, multiboson, and top events per 1 nb1. Decay rates and experimental selection/acceptance rates will impact final event yields and merit further study; as an illustrative example, we focus on select diboson and triboson channels in lead-lead collisions and discuss their observability at the high-luminosity phase of the Large Hadron Collider and the Future Circulate Collider. Published by the American Physical Society 2025
多tev离子碰撞中的硬过程
在大型强子对撞机的离子碰撞项目、高亮度升级计划以及对未来多tev强子对撞机的持续讨论的推动下,我们系统地研究了多tev离子碰撞中的硬散射、标准模型过程。我们重点研究了Pb208−Pb208、Xe131−Xe131、C12−C12和pp的对称束流构型,并对数十个过程的总截面和基准截面进行了编目,范围从关联希格斯和多玻色子的产生到关联顶对的产生,在QCD中,核子-核子碰撞能量从sNN=1到100 TeV的数量级。我们报告了这一阶的剩余尺度不确定度以及由核部分子密度拟合引起的不确定度。我们还讨论了核动力学(以核部分子密度编码)在部分子光度中的传播,并最终预测了截面。最后,我们报告了趋势的出现和跨不同核的外推截面的可靠性。在假设的sNN=39 TeV的未来圆形对撞机上,用L=33 nb−1的数据可以产生O(108)个弱玻色子、O(105)对二玻色子、O(104)对WH和ZH、O(103)个摩擦玻色子事件、O(105)个高pt光子事件和O(107) tt¯对的Pb-Pb碰撞。在sNN=5.52 TeV时,每1 nb−1可以产生O(10-106)个单、多玻色子和顶级事件。衰减率和实验选择/接受率将影响最终事件产量,值得进一步研究;作为一个说明性的例子,我们重点讨论了铅-铅碰撞中选择的diboson和triboson通道,并讨论了它们在大型强子对撞机和未来循环对撞机的高亮度阶段的可观测性。2025年由美国物理学会出版
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来源期刊
Physical Review D
Physical Review D 物理-天文与天体物理
CiteScore
9.20
自引率
36.00%
发文量
0
审稿时长
2 months
期刊介绍: Physical Review D (PRD) is a leading journal in elementary particle physics, field theory, gravitation, and cosmology and is one of the top-cited journals in high-energy physics. PRD covers experimental and theoretical results in all aspects of particle physics, field theory, gravitation and cosmology, including: Particle physics experiments, Electroweak interactions, Strong interactions, Lattice field theories, lattice QCD, Beyond the standard model physics, Phenomenological aspects of field theory, general methods, Gravity, cosmology, cosmic rays, Astrophysics and astroparticle physics, General relativity, Formal aspects of field theory, field theory in curved space, String theory, quantum gravity, gauge/gravity duality.
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