{"title":"Current-Component Independent Transition Form Factors for Semileptonic and Rare \n D\n ⟶\n π\n \n \n K\n \n \n Decays in the Light-Front Quark Model","authors":"H. Choi","doi":"10.1155/2021/4277321","DOIUrl":null,"url":null,"abstract":"<jats:p>We investigate the exclusive semileptonic and rare <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M2\">\n <mi>D</mi>\n <mo>⟶</mo>\n <mi>π</mi>\n <mfenced open=\"(\" close=\")\">\n <mrow>\n <mi>K</mi>\n </mrow>\n </mfenced>\n </math>\n </jats:inline-formula> decays within the standard model together with the light-front quark model (LFQM) constrained by the variational principle for the QCD-motivated effective Hamiltonian. The form factors are obtained in the <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M3\">\n <msup>\n <mrow>\n <mi>q</mi>\n </mrow>\n <mrow>\n <mo>+</mo>\n </mrow>\n </msup>\n <mo>=</mo>\n <mn>0</mn>\n </math>\n </jats:inline-formula> frame and then analytically continue to the physical timelike region. Together with our recent analysis of the current-component independent form factors <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M4\">\n <msub>\n <mrow>\n <mi>f</mi>\n </mrow>\n <mrow>\n <mo>±</mo>\n </mrow>\n </msub>\n <mfenced open=\"(\" close=\")\">\n <mrow>\n <msup>\n <mrow>\n <mi>q</mi>\n </mrow>\n <mrow>\n <mn>2</mn>\n </mrow>\n </msup>\n </mrow>\n </mfenced>\n </math>\n </jats:inline-formula> for the semileptonic decays, we present the current-component independent tensor form factor <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M5\">\n <msub>\n <mrow>\n <mi>f</mi>\n </mrow>\n <mrow>\n <mi>T</mi>\n </mrow>\n </msub>\n <mfenced open=\"(\" close=\")\">\n <mrow>\n <msup>\n <mrow>\n <mi>q</mi>\n </mrow>\n <mrow>\n <mn>2</mn>\n </mrow>\n </msup>\n </mrow>\n </mfenced>\n </math>\n </jats:inline-formula> for the rare decays to make the complete set of hadronic matrix elements regulating the semileptonic and rare <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M6\">\n <mi>D</mi>\n <mo>⟶</mo>\n <mi>π</mi>\n <mfenced open=\"(\" close=\")\">\n <mrow>\n <mi>K</mi>\n </mrow>\n </mfenced>\n </math>\n </jats:inline-formula> decays in our LFQM. The tensor form factor <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M7\">\n <msub>\n <mrow>\n <mi>f</mi>\n </mrow>\n <mrow>\n <mi>T</mi>\n </mrow>\n </msub>\n <mfenced open=\"(\" close=\")\">\n <mrow>\n <msup>\n <mrow>\n <mi>q</mi>\n </mrow>\n <mrow>\n <mn>2</mn>\n </mrow>\n </msup>\n </mrow>\n </mfenced>\n </math>\n </jats:inline-formula> are obtained from two independent sets <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M8\">\n <mfenced open=\"(\" close=\")\">\n <mrow>\n <msubsup>\n <mrow>\n <mi>J</mi>\n </mrow>\n <mrow>\n <mi>T</mi>\n </mrow>\n <mrow>\n <mo>+</mo>\n <mrow>\n <mo>⊥</mo>\n </mrow>\n </mrow>\n </msubsup>\n <mrow>\n <mo>,</mo>\n </mrow>\n <msubsup>\n <mrow>\n <mi>J</mi>\n </mrow>\n <mrow>\n <mi>T</mi>\n </mrow>\n <mrow>\n <mo>+</mo>\n <mrow>\n <mo>−</mo>\n </mrow>\n </mrow>\n </msubsup>\n </mrow>\n </mfenced>\n </math>\n </jats:inline-formula> of the tensor current <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M9\">\n <msubsup>\n <mrow>\n <mi>J</mi>\n </mrow>\n <mrow>\n <mi>T</mi>\n </mrow>\n <mrow>\n <mi>u</mi>\n <mi>v</mi>\n </mrow>\n </msubsup>\n </math>\n </jats:inline-formula> . As in our recent analysis of <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M10\">\n <msub>\n <mrow>\n <mi>f</mi>\n </mrow>\n <mrow>\n <mo>−</mo>\n </mrow>\n </msub>\n <mfenced open=\"(\" close=\")\">\n <mrow>\n <msup>\n <mrow>\n <mi>q</mi>\n </mrow>\n <mrow>\n <mn>2</mn>\n </mrow>\n </msup>\n </mrow>\n </mfenced>\n </math>\n </jats:inline-formula>, we show that <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M11\">\n <msub>\n <mrow>\n <mi>f</mi>\n </mrow>\n <mrow>\n <mi>T</mi>\n </mrow>\n </msub>\n <mfenced open=\"(\" close=\")\">\n <mrow>\n <msup>\n <mrow>\n <mi>q</mi>\n </mrow>\n <mrow>\n <mn>2</mn>\n </mrow>\n </msup>\n </mrow>\n </mfenced>\n </math>\n </jats:inline-formula> obtained from the two different sets of the current components gives the identical result in the valence region of the <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M12\">\n <msup>\n <mrow>\n <mi>q</mi>\n </mrow>\n <mrow>\n <mo>+</mo>\n </mrow>\n </msup>\n <mo>=</mo>\n <mn>0</mn>\n </math>\n </jats:inline-formula> frame without involving the explicit zero modes and the instantaneous contributions. The implications of the zero modes and the instantaneou","PeriodicalId":7498,"journal":{"name":"Advances in High Energy Physics","volume":" ","pages":""},"PeriodicalIF":1.5000,"publicationDate":"2021-08-24","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"5","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Advances in High Energy Physics","FirstCategoryId":"101","ListUrlMain":"https://doi.org/10.1155/2021/4277321","RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q3","JCRName":"PHYSICS, PARTICLES & FIELDS","Score":null,"Total":0}
引用次数: 5
Abstract
We investigate the exclusive semileptonic and rare decays within the standard model together with the light-front quark model (LFQM) constrained by the variational principle for the QCD-motivated effective Hamiltonian. The form factors are obtained in the frame and then analytically continue to the physical timelike region. Together with our recent analysis of the current-component independent form factors for the semileptonic decays, we present the current-component independent tensor form factor for the rare decays to make the complete set of hadronic matrix elements regulating the semileptonic and rare decays in our LFQM. The tensor form factor are obtained from two independent sets of the tensor current . As in our recent analysis of , we show that obtained from the two different sets of the current components gives the identical result in the valence region of the frame without involving the explicit zero modes and the instantaneous contributions. The implications of the zero modes and the instantaneou
期刊介绍:
Advances in High Energy Physics publishes the results of theoretical and experimental research on the nature of, and interaction between, energy and matter. Considering both original research and focussed review articles, the journal welcomes submissions from small research groups and large consortia alike.