Peter Boyle, Felix Erben, Vera Gülpers, Maxwell T. Hansen, Fabian Joswig, Michael Marshall, Nelson Pitanga Lachini, Antonin Portelli
{"title":"Light and Strange Vector Resonances from Lattice QCD at Physical Quark Masses","authors":"Peter Boyle, Felix Erben, Vera Gülpers, Maxwell T. Hansen, Fabian Joswig, Michael Marshall, Nelson Pitanga Lachini, Antonin Portelli","doi":"10.1103/physrevlett.134.111901","DOIUrl":null,"url":null,"abstract":"We present the first calculation at physical quark masses of scattering amplitudes describing the lightest pseudoscalar mesons interacting via the strong force in the vector channel. Using lattice quantum chromodynamics, we postdict the defining parameters for two short-lived resonances, the ρ</a:mi>(</a:mo>770</a:mn>)</a:mo></a:math> and <e:math xmlns:e=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><e:mrow><e:msup><e:mrow><e:mi>K</e:mi></e:mrow><e:mrow><e:mo>*</e:mo></e:mrow></e:msup><e:mo stretchy=\"false\">(</e:mo><e:mn>892</e:mn><e:mo stretchy=\"false\">)</e:mo></e:mrow></e:math>, which manifest as complex energy poles in <i:math xmlns:i=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><i:mi>π</i:mi><i:mi>π</i:mi></i:math> and <k:math xmlns:k=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><k:mi>K</k:mi><k:mi>π</k:mi></k:math> scattering amplitudes, respectively. The calculation proceeds by first computing the finite-volume energy spectrum of the two-hadron systems and then determining the amplitudes from the energies using the Lüscher formalism. The error budget includes a data-driven systematic error, obtained by scanning possible fit ranges and fit models to extract the spectrum from Euclidean correlators, as well as the scattering amplitudes from the latter. The final results, obtained by analytically continuing multiple parametrizations into the complex energy plane, are <m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><m:mrow><m:msub><m:mrow><m:mi>M</m:mi></m:mrow><m:mrow><m:mi>ρ</m:mi></m:mrow></m:msub><m:mo>=</m:mo><m:mn>796</m:mn><m:mo stretchy=\"false\">(</m:mo><m:mn>5</m:mn><m:mo stretchy=\"false\">)</m:mo><m:mo stretchy=\"false\">(</m:mo><m:mn>50</m:mn><m:mo stretchy=\"false\">)</m:mo><m:mtext> </m:mtext><m:mtext> </m:mtext><m:mi>MeV</m:mi></m:mrow></m:math>, <s:math xmlns:s=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><s:mrow><s:msub><s:mrow><s:mi mathvariant=\"normal\">Γ</s:mi></s:mrow><s:mrow><s:mi>ρ</s:mi></s:mrow></s:msub><s:mo>=</s:mo><s:mn>192</s:mn><s:mo stretchy=\"false\">(</s:mo><s:mn>10</s:mn><s:mo stretchy=\"false\">)</s:mo><s:mo stretchy=\"false\">(</s:mo><s:mn>31</s:mn><s:mo stretchy=\"false\">)</s:mo><s:mtext> </s:mtext><s:mtext> </s:mtext><s:mi>MeV</s:mi></s:mrow></s:math>, <z:math xmlns:z=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><z:mrow><z:msub><z:mrow><z:mi>M</z:mi></z:mrow><z:mrow><z:msup><z:mrow><z:mi>K</z:mi></z:mrow><z:mrow><z:mo>*</z:mo></z:mrow></z:msup></z:mrow></z:msub><z:mo>=</z:mo><z:mn>893</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>54</z:mn><z:mo stretchy=\"false\">)</z:mo><z:mtext> </z:mtext><z:mtext> </z:mtext><z:mi>MeV</z:mi></z:mrow></z:math>, and <fb:math xmlns:fb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><fb:mrow><fb:msub><fb:mrow><fb:mi mathvariant=\"normal\">Γ</fb:mi></fb:mrow><fb:mrow><fb:msup><fb:mrow><fb:mi>K</fb:mi></fb:mrow><fb:mrow><fb:mo>*</fb:mo></fb:mrow></fb:msup></fb:mrow></fb:msub><fb:mo>=</fb:mo><fb:mn>51</fb:mn><fb:mo stretchy=\"false\">(</fb:mo><fb:mn>2</fb:mn><fb:mo stretchy=\"false\">)</fb:mo><fb:mo stretchy=\"false\">(</fb:mo><fb:mn>11</fb:mn><fb:mo stretchy=\"false\">)</fb:mo><fb:mtext> </fb:mtext><fb:mtext> </fb:mtext><fb:mi>MeV</fb:mi></fb:mrow></fb:math>, where the subscript indicates the resonance and <mb:math xmlns:mb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mb:mi>M</mb:mi></mb:math> and <ob:math xmlns:ob=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><ob:mi mathvariant=\"normal\">Γ</ob:mi></ob:math> stand for the mass and width, respectively, and where the first bracket indicates the statistical and the second bracket the systematic uncertainty. <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":20069,"journal":{"name":"Physical review letters","volume":"37 1","pages":""},"PeriodicalIF":8.1000,"publicationDate":"2025-03-18","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Physical review letters","FirstCategoryId":"101","ListUrlMain":"https://doi.org/10.1103/physrevlett.134.111901","RegionNum":1,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"PHYSICS, MULTIDISCIPLINARY","Score":null,"Total":0}
引用次数: 0
Abstract
We present the first calculation at physical quark masses of scattering amplitudes describing the lightest pseudoscalar mesons interacting via the strong force in the vector channel. Using lattice quantum chromodynamics, we postdict the defining parameters for two short-lived resonances, the ρ(770) and K*(892), which manifest as complex energy poles in ππ and Kπ scattering amplitudes, respectively. The calculation proceeds by first computing the finite-volume energy spectrum of the two-hadron systems and then determining the amplitudes from the energies using the Lüscher formalism. The error budget includes a data-driven systematic error, obtained by scanning possible fit ranges and fit models to extract the spectrum from Euclidean correlators, as well as the scattering amplitudes from the latter. The final results, obtained by analytically continuing multiple parametrizations into the complex energy plane, are Mρ=796(5)(50)MeV, Γρ=192(10)(31)MeV, MK*=893(2)(54)MeV, and ΓK*=51(2)(11)MeV, where the subscript indicates the resonance and M and Γ stand for the mass and width, respectively, and where the first bracket indicates the statistical and the second bracket the systematic uncertainty. Published by the American Physical Society2025
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