Konstantin Ottnad, Simone Bacchio, Jacob Finkenrath, Bartosz Kostrzewa, Marcus Petschlies, Ferenc Pittler, Carsten Urbach, Urs Wenger
{"title":"在完全物理条件下晶格QCD的η, η '介子。","authors":"Konstantin Ottnad, Simone Bacchio, Jacob Finkenrath, Bartosz Kostrzewa, Marcus Petschlies, Ferenc Pittler, Carsten Urbach, Urs Wenger","doi":"10.1140/epja/s10050-025-01635-0","DOIUrl":null,"url":null,"abstract":"<p><p>We determine masses and mixing parameters of the <math><mi>η</mi></math> and <math><msup><mi>η</mi> <mo>'</mo></msup> </math> meson in lattice QCD. The calculations are carried out on a set of 13 ETMC gauge ensembles with <math> <mrow><msub><mi>N</mi> <mi>f</mi></msub> <mo>=</mo> <mn>2</mn> <mo>+</mo> <mn>1</mn> <mo>+</mo> <mn>1</mn></mrow> </math> (maximally) twisted-mass Clover-improved quarks. These ensemble cover four values of the lattice spacing <math><mrow><mi>a</mi> <mo>=</mo> <mn>0.057</mn> <mspace></mspace> <mtext>fm</mtext> <mo>,</mo> <mo>…</mo> <mo>,</mo> <mn>0.092</mn> <mspace></mspace> <mtext>fm</mtext></mrow> </math> and pion masses from 140 to <math><mrow><mn>360</mn> <mspace></mspace> <mtext>MeV</mtext></mrow> </math> , including three ensembles at physical quark masses and six ensembles with <math> <mrow><msub><mi>M</mi> <mi>π</mi></msub> <mo><</mo> <mn>200</mn> <mspace></mspace> <mtext>MeV</mtext></mrow> </math> . The strange-quark contribution is treated in a mixed-action approach using Osterwalder-Seiler fermions to avoid complications due to flavor mixing in the heavy quark sector and to enable the use of the one-end trick in the computation of strange quark-disconnected diagrams. With the strange-quark mass tuned to its physical value and several ensembles having close-to-physical light-quark mass, uncertainties related to the chiral extrapolations are reduced significantly compared to earlier studies. Physical results are computed with fully controlled systematics from a combined chiral, continuum and infinite-volume extrapolation, and a full error budget is obtained from model averages over of various fit ansätze and data cuts. Our results for the masses are given by <math> <mrow><msub><mi>M</mi> <mi>η</mi></msub> <mo>=</mo> <mn>551</mn> <mrow><mo>(</mo> <mn>16</mn> <mo>)</mo></mrow> <mspace></mspace> <mtext>MeV</mtext></mrow> </math> and <math> <mrow><msub><mi>M</mi> <msup><mi>η</mi> <mo>'</mo></msup> </msub> <mo>=</mo> <mn>972</mn> <mrow><mo>(</mo> <mn>20</mn> <mo>)</mo></mrow> <mspace></mspace> <mtext>MeV</mtext></mrow> </math> , respectively, where statistical and systematic errors have been added in quadrature. For the mixing angle and decay-constant parameters the Feldmann-Kroll-Stech scheme is employed to compute them from pseudoscalar matrix elements in the quark-flavor basis. For the mixing angle we obtain <math> <mrow><msup><mi>ϕ</mi> <mtext>phys</mtext></msup> <mo>=</mo> <mn>39.3</mn> <msup><mrow><mo>(</mo> <mn>2.0</mn> <mo>)</mo></mrow> <mo>∘</mo></msup> </mrow> </math> and our results for the decay-constant parameters are given by <math> <mrow><msubsup><mi>f</mi> <mi>l</mi> <mtext>phys</mtext></msubsup> <mo>=</mo> <mn>138.6</mn> <mrow><mo>(</mo> <mn>4.4</mn> <mo>)</mo></mrow> <mspace></mspace> <mtext>MeV</mtext></mrow> </math> and <math> <mrow><msubsup><mi>f</mi> <mi>s</mi> <mtext>phys</mtext></msubsup> <mo>=</mo> <mn>170.7</mn> <mrow><mo>(</mo> <mn>3.3</mn> <mo>)</mo></mrow> <mspace></mspace> <mtext>MeV</mtext></mrow> </math> .</p>","PeriodicalId":75005,"journal":{"name":"The European physical journal. A, Hadrons and nuclei","volume":"61 7","pages":"169"},"PeriodicalIF":0.0000,"publicationDate":"2025-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.ncbi.nlm.nih.gov/pmc/articles/PMC12283833/pdf/","citationCount":"0","resultStr":"{\"title\":\"<ArticleTitle xmlns:ns0=\\\"http://www.w3.org/1998/Math/MathML\\\"><ns0:math><ns0:mi>η</ns0:mi></ns0:math> , <ns0:math><ns0:msup><ns0:mi>η</ns0:mi> <ns0:mo>'</ns0:mo></ns0:msup> </ns0:math> mesons from lattice QCD in fully physical conditions.\",\"authors\":\"Konstantin Ottnad, Simone Bacchio, Jacob Finkenrath, Bartosz Kostrzewa, Marcus Petschlies, Ferenc Pittler, Carsten Urbach, Urs Wenger\",\"doi\":\"10.1140/epja/s10050-025-01635-0\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<p><p>We determine masses and mixing parameters of the <math><mi>η</mi></math> and <math><msup><mi>η</mi> <mo>'</mo></msup> </math> meson in lattice QCD. The calculations are carried out on a set of 13 ETMC gauge ensembles with <math> <mrow><msub><mi>N</mi> <mi>f</mi></msub> <mo>=</mo> <mn>2</mn> <mo>+</mo> <mn>1</mn> <mo>+</mo> <mn>1</mn></mrow> </math> (maximally) twisted-mass Clover-improved quarks. These ensemble cover four values of the lattice spacing <math><mrow><mi>a</mi> <mo>=</mo> <mn>0.057</mn> <mspace></mspace> <mtext>fm</mtext> <mo>,</mo> <mo>…</mo> <mo>,</mo> <mn>0.092</mn> <mspace></mspace> <mtext>fm</mtext></mrow> </math> and pion masses from 140 to <math><mrow><mn>360</mn> <mspace></mspace> <mtext>MeV</mtext></mrow> </math> , including three ensembles at physical quark masses and six ensembles with <math> <mrow><msub><mi>M</mi> <mi>π</mi></msub> <mo><</mo> <mn>200</mn> <mspace></mspace> <mtext>MeV</mtext></mrow> </math> . The strange-quark contribution is treated in a mixed-action approach using Osterwalder-Seiler fermions to avoid complications due to flavor mixing in the heavy quark sector and to enable the use of the one-end trick in the computation of strange quark-disconnected diagrams. With the strange-quark mass tuned to its physical value and several ensembles having close-to-physical light-quark mass, uncertainties related to the chiral extrapolations are reduced significantly compared to earlier studies. Physical results are computed with fully controlled systematics from a combined chiral, continuum and infinite-volume extrapolation, and a full error budget is obtained from model averages over of various fit ansätze and data cuts. Our results for the masses are given by <math> <mrow><msub><mi>M</mi> <mi>η</mi></msub> <mo>=</mo> <mn>551</mn> <mrow><mo>(</mo> <mn>16</mn> <mo>)</mo></mrow> <mspace></mspace> <mtext>MeV</mtext></mrow> </math> and <math> <mrow><msub><mi>M</mi> <msup><mi>η</mi> <mo>'</mo></msup> </msub> <mo>=</mo> <mn>972</mn> <mrow><mo>(</mo> <mn>20</mn> <mo>)</mo></mrow> <mspace></mspace> <mtext>MeV</mtext></mrow> </math> , respectively, where statistical and systematic errors have been added in quadrature. For the mixing angle and decay-constant parameters the Feldmann-Kroll-Stech scheme is employed to compute them from pseudoscalar matrix elements in the quark-flavor basis. For the mixing angle we obtain <math> <mrow><msup><mi>ϕ</mi> <mtext>phys</mtext></msup> <mo>=</mo> <mn>39.3</mn> <msup><mrow><mo>(</mo> <mn>2.0</mn> <mo>)</mo></mrow> <mo>∘</mo></msup> </mrow> </math> and our results for the decay-constant parameters are given by <math> <mrow><msubsup><mi>f</mi> <mi>l</mi> <mtext>phys</mtext></msubsup> <mo>=</mo> <mn>138.6</mn> <mrow><mo>(</mo> <mn>4.4</mn> <mo>)</mo></mrow> <mspace></mspace> <mtext>MeV</mtext></mrow> </math> and <math> <mrow><msubsup><mi>f</mi> <mi>s</mi> <mtext>phys</mtext></msubsup> <mo>=</mo> <mn>170.7</mn> <mrow><mo>(</mo> <mn>3.3</mn> <mo>)</mo></mrow> <mspace></mspace> <mtext>MeV</mtext></mrow> </math> .</p>\",\"PeriodicalId\":75005,\"journal\":{\"name\":\"The European physical journal. A, Hadrons and nuclei\",\"volume\":\"61 7\",\"pages\":\"169\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2025-01-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"https://www.ncbi.nlm.nih.gov/pmc/articles/PMC12283833/pdf/\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"The European physical journal. A, Hadrons and nuclei\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1140/epja/s10050-025-01635-0\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"2025/7/22 0:00:00\",\"PubModel\":\"Epub\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"The European physical journal. A, Hadrons and nuclei","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1140/epja/s10050-025-01635-0","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"2025/7/22 0:00:00","PubModel":"Epub","JCR":"","JCRName":"","Score":null,"Total":0}
η , η' mesons from lattice QCD in fully physical conditions.
We determine masses and mixing parameters of the and meson in lattice QCD. The calculations are carried out on a set of 13 ETMC gauge ensembles with (maximally) twisted-mass Clover-improved quarks. These ensemble cover four values of the lattice spacing and pion masses from 140 to , including three ensembles at physical quark masses and six ensembles with . The strange-quark contribution is treated in a mixed-action approach using Osterwalder-Seiler fermions to avoid complications due to flavor mixing in the heavy quark sector and to enable the use of the one-end trick in the computation of strange quark-disconnected diagrams. With the strange-quark mass tuned to its physical value and several ensembles having close-to-physical light-quark mass, uncertainties related to the chiral extrapolations are reduced significantly compared to earlier studies. Physical results are computed with fully controlled systematics from a combined chiral, continuum and infinite-volume extrapolation, and a full error budget is obtained from model averages over of various fit ansätze and data cuts. Our results for the masses are given by and , respectively, where statistical and systematic errors have been added in quadrature. For the mixing angle and decay-constant parameters the Feldmann-Kroll-Stech scheme is employed to compute them from pseudoscalar matrix elements in the quark-flavor basis. For the mixing angle we obtain and our results for the decay-constant parameters are given by and .