Physical-mass calculation of ρ(770) and K*(892) resonance parameters via ππ and Kπ scattering amplitudes from lattice QCD

IF 5.3 2区 物理与天体物理 Q1 Physics and Astronomy Physical Review D Pub Date : 2025-03-18 DOI:10.1103/physrevd.111.054510
Peter Boyle, Felix Erben, Vera Gülpers, Maxwell T. Hansen, Fabian Joswig, Michael Marshall, Nelson Pitanga Lachini, Antonin Portelli
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Our final pole positions, <m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><m:mi>M</m:mi><m:mo>+</m:mo><m:mi>i</m:mi><m:mi mathvariant=\"normal\">Γ</m:mi><m:mo>/</m:mo><m:mn>2</m:mn></m:math>, with all statistical and systematic errors exposed, are <p:math xmlns:p=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><p:mrow><p:msub><p:mrow><p:mi>M</p:mi></p:mrow><p:mrow><p:msup><p:mrow><p:mi>K</p:mi></p:mrow><p:mrow><p:mo>*</p:mo></p:mrow></p:msup></p:mrow></p:msub><p:mo>=</p:mo><p:mn>893</p:mn><p:mo stretchy=\"false\">(</p:mo><p:mn>2</p:mn><p:mo stretchy=\"false\">)</p:mo><p:mo stretchy=\"false\">(</p:mo><p:mn>8</p:mn><p:mo stretchy=\"false\">)</p:mo><p:mo stretchy=\"false\">(</p:mo><p:mn>54</p:mn><p:mo stretchy=\"false\">)</p:mo><p:mo stretchy=\"false\">(</p:mo><p:mn>2</p:mn><p:mo stretchy=\"false\">)</p:mo><p:mtext> </p:mtext><p:mtext> </p:mtext><p:mi>MeV</p:mi></p:mrow></p:math> and <z:math xmlns:z=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><z:msub><z:mi mathvariant=\"normal\">Γ</z:mi><z:msup><z:mi>K</z:mi><z:mo>*</z:mo></z:msup></z:msub><z:mo>=</z:mo><z:mn>51</z:mn><z:mo stretchy=\"false\">(</z:mo><z:mn>2</z:mn><z:mo stretchy=\"false\">)</z:mo><z:mo stretchy=\"false\">(</z:mo><z:mn>11</z:mn><z:mo stretchy=\"false\">)</z:mo><z:mo stretchy=\"false\">(</z:mo><z:mn>3</z:mn><z:mo stretchy=\"false\">)</z:mo><z:mo stretchy=\"false\">(</z:mo><z:mn>0</z:mn><z:mo stretchy=\"false\">)</z:mo><z:mtext> </z:mtext><z:mtext> </z:mtext><z:mi>MeV</z:mi></z:math> for the <kb:math xmlns:kb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><kb:msup><kb:mi>K</kb:mi><kb:mo>*</kb:mo></kb:msup><kb:mo stretchy=\"false\">(</kb:mo><kb:mn>892</kb:mn><kb:mo stretchy=\"false\">)</kb:mo></kb:math> resonance and <ob:math xmlns:ob=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><ob:mrow><ob:msub><ob:mrow><ob:mi>M</ob:mi></ob:mrow><ob:mrow><ob:mi>ρ</ob:mi></ob:mrow></ob:msub><ob:mo>=</ob:mo><ob:mn>796</ob:mn><ob:mo stretchy=\"false\">(</ob:mo><ob:mn>5</ob:mn><ob:mo stretchy=\"false\">)</ob:mo><ob:mo stretchy=\"false\">(</ob:mo><ob:mn>15</ob:mn><ob:mo stretchy=\"false\">)</ob:mo><ob:mo stretchy=\"false\">(</ob:mo><ob:mn>48</ob:mn><ob:mo stretchy=\"false\">)</ob:mo><ob:mo stretchy=\"false\">(</ob:mo><ob:mn>2</ob:mn><ob:mo stretchy=\"false\">)</ob:mo><ob:mtext> </ob:mtext><ob:mtext> </ob:mtext><ob:mi>MeV</ob:mi></ob:mrow></ob:math> and <yb:math xmlns:yb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><yb:msub><yb:mi mathvariant=\"normal\">Γ</yb:mi><yb:mi>ρ</yb:mi></yb:msub><yb:mo>=</yb:mo><yb:mn>192</yb:mn><yb:mo stretchy=\"false\">(</yb:mo><yb:mn>10</yb:mn><yb:mo stretchy=\"false\">)</yb:mo><yb:mo stretchy=\"false\">(</yb:mo><yb:mn>28</yb:mn><yb:mo stretchy=\"false\">)</yb:mo><yb:mo stretchy=\"false\">(</yb:mo><yb:mn>12</yb:mn><yb:mo stretchy=\"false\">)</yb:mo><yb:mo stretchy=\"false\">(</yb:mo><yb:mn>0</yb:mn><yb:mo stretchy=\"false\">)</yb:mo><yb:mtext> </yb:mtext><yb:mtext> </yb:mtext><yb:mi>MeV</yb:mi></yb:math> for the <jc:math xmlns:jc=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><jc:mi>ρ</jc:mi><jc:mo stretchy=\"false\">(</jc:mo><jc:mn>770</jc:mn><jc:mo stretchy=\"false\">)</jc:mo></jc:math> resonance. The four differently grouped sources of uncertainties are, in the order of occurrence: statistical, data-driven systematic, an estimation of systematic effects beyond our computation (dominated by the fact that we employ a single lattice spacing), and the error from the scale-setting uncertainty on our ensemble. <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":"44 1","pages":""},"PeriodicalIF":5.3000,"publicationDate":"2025-03-18","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.111.054510","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}
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Abstract

We present our study of the ρ(770) and K*(892) resonances from lattice quantum chromodynamics (QCD) employing domain-wall fermions at physical quark masses. We determine the finite-volume energy spectrum in various momentum frames and obtain phase-shift parametrizations via the Lüscher formalism and as a final step the complex resonance poles of the ππ and Kπ elastic scattering amplitudes via an analytical continuation of the models. By sampling a large number of representative sets of underlying energy-level fits, we also assign a systematic uncertainty to our final results. This is a significant extension to data-driven analysis methods that have been used in lattice QCD to date, due to the two-step nature of the formalism. Our final pole positions, M+iΓ/2, with all statistical and systematic errors exposed, are MK*=893(2)(8)(54)(2) MeV and ΓK*=51(2)(11)(3)(0) MeV for the K*(892) resonance and Mρ=796(5)(15)(48)(2) MeV and Γρ=192(10)(28)(12)(0) MeV for the ρ(770) resonance. The four differently grouped sources of uncertainties are, in the order of occurrence: statistical, data-driven systematic, an estimation of systematic effects beyond our computation (dominated by the fact that we employ a single lattice spacing), and the error from the scale-setting uncertainty on our ensemble. Published by the American Physical Society 2025
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利用晶格QCD的ππ和Kπ散射振幅计算ρ(770)和K*(892)共振参数的物理质量
本文利用域壁费米子在物理夸克质量下对晶格量子色动力学(QCD)中的ρ(770)和K*(892)共振进行了研究。我们确定了不同动量系下的有限体积能谱,并通过l舍尔公式得到相移参数化,最后通过模型的解析延演得到ππ和Kπ弹性散射振幅的复共振极点。通过对大量具有代表性的潜在能级拟合集进行抽样,我们还为最终结果分配了系统的不确定性。由于形式化的两步性质,这是迄今为止在晶格QCD中使用的数据驱动分析方法的重要扩展。我们的最终极点M+iΓ/2,暴露了所有统计和系统误差,K*(892)共振的MK*=893(2)(8)(54)(2) MeV和ΓK*=51(2)(11)(3)(0) MeV, ρ(770)共振的ρ=796(5)(15)(48)(2) MeV和Γρ=192(10)(28)(12)(0) MeV。根据发生的顺序,四种不同分组的不确定性来源是:统计的,数据驱动的系统的,超出我们计算的系统效应的估计(由我们使用单个晶格间距的事实主导),以及来自我们集合的尺度设置不确定性的误差。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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