Charmoniumlike channels 1+ with isospin 1 from lattice and effective field theory

IF 5 2区 物理与天体物理 Q1 Physics and Astronomy
Mitja Sadl, Sara Collins, Zhi-Hui Guo, M. Padmanath, Sasa Prelovsek, Lin-Wan Yan
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We investigate <c:math xmlns:c=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><c:msup><c:mi>J</c:mi><c:mrow><c:mi>P</c:mi><c:mi>C</c:mi></c:mrow></c:msup><c:mo>=</c:mo><c:msup><c:mn>1</c:mn><c:mrow><c:mo>+</c:mo><c:mo>±</c:mo></c:mrow></c:msup></c:math> states with flavor <e:math xmlns:e=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><e:mover accent=\"true\"><e:mi>c</e:mi><e:mo stretchy=\"false\">¯</e:mo></e:mover><e:mi>c</e:mi><e:mover accent=\"true\"><e:mi>q</e:mi><e:mo stretchy=\"false\">¯</e:mo></e:mover><e:mi>q</e:mi></e:math> (<k:math xmlns:k=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><k:mrow><k:mi>q</k:mi><k:mo>=</k:mo><k:mi>u</k:mi></k:mrow></k:math>, <m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><m:mrow><m:mi>d</m:mi></m:mrow></m:math>) in isospin 1 using lattice QCD. This is the first study of these mesons employing more than one volume and involving frames with nonzero total momentum. We utilize two <o:math xmlns:o=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><o:msub><o:mi>N</o:mi><o:mi>f</o:mi></o:msub><o:mo>=</o:mo><o:mn>2</o:mn><o:mo>+</o:mo><o:mn>1</o:mn></o:math> CLS ensembles with <q:math xmlns:q=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><q:mrow><q:msub><q:mrow><q:mi>m</q:mi></q:mrow><q:mrow><q:mi>π</q:mi></q:mrow></q:msub><q:mo>≃</q:mo><q:mn>280</q:mn><q:mtext> </q:mtext><q:mtext> </q:mtext><q:mi>MeV</q:mi></q:mrow></q:math>. The simulations are performed with unphysical light quark masses at a single lattice spacing of <s:math xmlns:s=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><s:mrow><s:mi>a</s:mi><s:mo>≃</s:mo><s:mn>0.086</s:mn><s:mtext> </s:mtext><s:mtext> </s:mtext><s:mrow><s:mi>fm</s:mi></s:mrow></s:mrow></s:math> and omit <u:math xmlns:u=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><u:mi>ψ</u:mi><u:mo stretchy=\"false\">(</u:mo><u:mn>2</u:mn><u:mi>S</u:mi><u:mo stretchy=\"false\">)</u:mo><u:mi>π</u:mi></u:math>, <y:math xmlns:y=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><y:mi>ψ</y:mi><y:mo stretchy=\"false\">(</y:mo><y:mn>3770</y:mn><y:mo stretchy=\"false\">)</y:mo><y:mi>π</y:mi></y:math> and three-particle decay channels, so our results provide only qualitative insights. Resulting eigenenergies are compatible or just slightly shifted down with respect to noninteracting energies, where the most significant shifts occur for certain <cb:math xmlns:cb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><cb:mi>D</cb:mi><cb:msup><cb:mover accent=\"true\"><cb:mi>D</cb:mi><cb:mo stretchy=\"false\">¯</cb:mo></cb:mover><cb:mo>*</cb:mo></cb:msup></cb:math> states. Both channels <gb:math xmlns:gb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><gb:msup><gb:mn>1</gb:mn><gb:mrow><gb:mo>+</gb:mo><gb:mo>±</gb:mo></gb:mrow></gb:msup></gb:math> have a virtual pole slightly below the threshold if <ib:math xmlns:ib=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><ib:mi>D</ib:mi><ib:msup><ib:mover accent=\"true\"><ib:mi>D</ib:mi><ib:mo stretchy=\"false\">¯</ib:mo></ib:mover><ib:mo>*</ib:mo></ib:msup></ib:math> is assumed to be decoupled from other channels. In addition, we perform a coupled channel analysis of <mb:math xmlns:mb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mb:mi>J</mb:mi><mb:mo>/</mb:mo><mb:mi>ψ</mb:mi><mb:mi>π</mb:mi></mb:math> and <ob:math xmlns:ob=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><ob:mi>D</ob:mi><ob:msup><ob:mover accent=\"true\"><ob:mi>D</ob:mi><ob:mo stretchy=\"false\">¯</ob:mo></ob:mover><ob:mo>*</ob:mo></ob:msup></ob:math> scattering with <sb:math xmlns:sb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><sb:msup><sb:mi>J</sb:mi><sb:mrow><sb:mi>P</sb:mi><sb:mi>C</sb:mi></sb:mrow></sb:msup><sb:mo>=</sb:mo><sb:msup><sb:mn>1</sb:mn><sb:mrow><sb:mo>+</sb:mo><sb:mo>−</sb:mo></sb:mrow></sb:msup></sb:math> within an effective field theory framework. The <ub:math xmlns:ub=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><ub:mi>J</ub:mi><ub:mo>/</ub:mo><ub:mi>ψ</ub:mi><ub:mi>π</ub:mi></ub:math> and <wb:math xmlns:wb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><wb:mi>D</wb:mi><wb:msup><wb:mover accent=\"true\"><wb:mi>D</wb:mi><wb:mo stretchy=\"false\">¯</wb:mo></wb:mover><wb:mo>*</wb:mo></wb:msup></wb:math> invariant-mass distributions from BESIII and finite-volume energies from several lattice QCD simulations, including this work, are fitted simultaneously. All fits yield two poles relatively close to the D</ac:mi>D</ac:mi>¯</ac:mo></ac:mover>*</ac:mo></ac:msup></ac:math> threshold and reasonably reproduce the experimental <ec:math xmlns:ec=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><ec:msub><ec:mi>Z</ec:mi><ec:mi>c</ec:mi></ec:msub></ec:math> peaks. They also reproduce lattice energies up to slightly above the <gc:math xmlns:gc=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><gc:mi>D</gc:mi><gc:msup><gc:mover accent=\"true\"><gc:mi>D</gc:mi><gc:mo stretchy=\"false\">¯</gc:mo></gc:mover><gc:mo>*</gc:mo></gc:msup></gc:math> threshold, while reproduction at even higher energies is better for fits that put more weight on the lattice data. Our findings suggest that the employed effective field theory can reasonably reconcile the peaks in the experimental line shapes and the lattice energies, although those lie close to noninteracting energies. We also study <kc:math xmlns:kc=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><kc:mi>J</kc:mi><kc:mo>/</kc:mo><kc:mi>ψ</kc:mi><kc:mi>π</kc:mi></kc:math> scattering in s wave and place upper bounds on the phase shift. <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":"25 1","pages":""},"PeriodicalIF":5.0000,"publicationDate":"2025-04-08","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.111.054513","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

Many exotic charmoniumlike mesons have already been discovered experimentally, of which the Zc mesons with isospin 1 are prominent examples. We investigate JPC=1+± states with flavor c¯cq¯q (q=u, d) in isospin 1 using lattice QCD. This is the first study of these mesons employing more than one volume and involving frames with nonzero total momentum. We utilize two Nf=2+1 CLS ensembles with mπ280 MeV. The simulations are performed with unphysical light quark masses at a single lattice spacing of a0.086 fm and omit ψ(2S)π, ψ(3770)π and three-particle decay channels, so our results provide only qualitative insights. Resulting eigenenergies are compatible or just slightly shifted down with respect to noninteracting energies, where the most significant shifts occur for certain DD¯* states. Both channels 1+± have a virtual pole slightly below the threshold if DD¯* is assumed to be decoupled from other channels. In addition, we perform a coupled channel analysis of J/ψπ and DD¯* scattering with JPC=1+ within an effective field theory framework. The J/ψπ and DD¯* invariant-mass distributions from BESIII and finite-volume energies from several lattice QCD simulations, including this work, are fitted simultaneously. All fits yield two poles relatively close to the DD¯* threshold and reasonably reproduce the experimental Zc peaks. They also reproduce lattice energies up to slightly above the DD¯* threshold, while reproduction at even higher energies is better for fits that put more weight on the lattice data. Our findings suggest that the employed effective field theory can reasonably reconcile the peaks in the experimental line shapes and the lattice energies, although those lie close to noninteracting energies. We also study J/ψπ scattering in s wave and place upper bounds on the phase shift. Published by the American Physical Society 2025
实验中已经发现了许多奇异的类粲介子,其中具有等空间素 1 的 Zc 介子就是突出的例子。我们利用格子 QCD 研究了等空间素 1 中具有 c¯cq¯q (q=u, d)味道的 JPC=1+± 态。这是对这些介子的首次研究,采用了一个以上的体积,并涉及具有非零总动量的框架。我们使用了两个 mπ≃280 MeV 的 Nf=2+1 CLS 集合。模拟是在单一晶格间距为 a≃0.086 fm 的非物理轻夸克质量下进行的,省略了ψ(2S)π、ψ(3770)π 和三粒子衰变通道,因此我们的结果只能提供定性的见解。得出的特征能与非相互作用能相容或只是略微下移,其中最显著的下移发生在某些 DD¯* 态上。如果假定 DD¯* 与其他通道脱钩,通道 1+± 都有一个略低于阈值的虚极。此外,我们还在有效场论框架内对JPC=1+-的J/ψπ和DD¯*散射进行了耦合通道分析。同时拟合了来自 BESIII 的 J/ψπ 和 DD¯* 不变质量分布,以及包括本研究在内的若干格子 QCD 模拟的有限体积能量。所有拟合都产生了相对接近 DD¯* 门限的两个极点,并合理地再现了实验 Zc 峰。它们还再现了略高于 DD¯* 阈值的晶格能量,而对于更重视晶格数据的拟合,在更高能量下的再现效果更好。我们的研究结果表明,采用的有效场理论可以合理地协调实验线形中的峰值和晶格能量,尽管这些峰值接近非相互作用能量。我们还研究了 s 波中的 J/ψπ 散射,并给出了相移的上限。 美国物理学会出版 2025
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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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