Theoretical implications for a new measurement of KL→π0ℓℓ¯

IF 5 2区 物理与天体物理 Q1 Physics and Astronomy
G. D’Ambrosio, A. M. Iyer, F. Mahmoudi, S. Neshatpour
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Beginning with the golden channels, K</a:mi></a:mrow>+</a:mo></a:mrow></a:msup>→</a:mo>π</a:mi></a:mrow>+</a:mo></a:mrow></a:msup>ν</a:mi>ν</a:mi></a:mrow>¯</a:mo></a:mrow></a:mover></a:mrow></a:math> and <f:math xmlns:f=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><f:mrow><f:msub><f:mrow><f:mi>K</f:mi></f:mrow><f:mrow><f:mi>L</f:mi></f:mrow></f:msub><f:mo stretchy=\"false\">→</f:mo><f:msup><f:mrow><f:mi>π</f:mi></f:mrow><f:mrow><f:mn>0</f:mn></f:mrow></f:msup><f:mi>ν</f:mi><f:mover accent=\"true\"><f:mrow><f:mi>ν</f:mi></f:mrow><f:mrow><f:mo stretchy=\"false\">¯</f:mo></f:mrow></f:mover></f:mrow></f:math>, the paper will eventually cast the spotlight on the importance of a precise measurement of <k:math xmlns:k=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><k:mrow><k:mi>BR</k:mi><k:mo stretchy=\"false\">(</k:mo><k:msub><k:mrow><k:mi>K</k:mi></k:mrow><k:mrow><k:mi>L</k:mi></k:mrow></k:msub><k:mo stretchy=\"false\">→</k:mo><k:msup><k:mrow><k:mi>π</k:mi></k:mrow><k:mrow><k:mn>0</k:mn></k:mrow></k:msup><k:mo>ℓ</k:mo><k:mover accent=\"true\"><k:mrow><k:mo>ℓ</k:mo></k:mrow><k:mrow><k:mo stretchy=\"true\">¯</k:mo></k:mrow></k:mover><k:mo stretchy=\"false\">)</k:mo></k:mrow></k:math>. The phenomenological analyses involve sequentially adding kaon physics observables at the projected final precision of their respective measurements to the global fit. More specifically, we consider three different scenarios with different sets of observables assumed at their final precisions. Beginning with <r:math xmlns:r=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><r:mrow><r:mi>BR</r:mi><r:mo stretchy=\"false\">(</r:mo><r:msup><r:mrow><r:mi>K</r:mi></r:mrow><r:mrow><r:mo>+</r:mo></r:mrow></r:msup><r:mo stretchy=\"false\">→</r:mo><r:msup><r:mrow><r:mi>π</r:mi></r:mrow><r:mrow><r:mo>+</r:mo></r:mrow></r:msup><r:mi>ν</r:mi><r:mover accent=\"true\"><r:mrow><r:mi>ν</r:mi></r:mrow><r:mrow><r:mo stretchy=\"false\">¯</r:mo></r:mrow></r:mover><r:mo stretchy=\"false\">)</r:mo></r:mrow></r:math> and <y:math xmlns:y=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><y:mrow><y:mi>BR</y:mi><y:mo stretchy=\"false\">(</y:mo><y:msub><y:mrow><y:mi>K</y:mi></y:mrow><y:mrow><y:mi>L</y:mi></y:mrow></y:msub><y:mo stretchy=\"false\">→</y:mo><y:msup><y:mrow><y:mi>π</y:mi></y:mrow><y:mrow><y:mn>0</y:mn></y:mrow></y:msup><y:mi>ν</y:mi><y:mover accent=\"true\"><y:mrow><y:mi>ν</y:mi></y:mrow><y:mrow><y:mo stretchy=\"false\">¯</y:mo></y:mrow></y:mover><y:mo stretchy=\"false\">)</y:mo></y:mrow></y:math>, we sequentially add <fb:math xmlns:fb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><fb:mrow><fb:mi>BR</fb:mi><fb:mo stretchy=\"false\">(</fb:mo><fb:msub><fb:mrow><fb:mi>K</fb:mi></fb:mrow><fb:mrow><fb:mi>L</fb:mi></fb:mrow></fb:msub><fb:mo stretchy=\"false\">→</fb:mo><fb:msup><fb:mrow><fb:mi>π</fb:mi></fb:mrow><fb:mrow><fb:mn>0</fb:mn></fb:mrow></fb:msup><fb:mi>e</fb:mi><fb:mover accent=\"true\"><fb:mrow><fb:mi>e</fb:mi></fb:mrow><fb:mrow><fb:mo stretchy=\"false\">¯</fb:mo></fb:mrow></fb:mover><fb:mo stretchy=\"false\">)</fb:mo></fb:mrow></fb:math> and <mb:math xmlns:mb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mb:mrow><mb:mi>BR</mb:mi><mb:mo stretchy=\"false\">(</mb:mo><mb:msub><mb:mrow><mb:mi>K</mb:mi></mb:mrow><mb:mrow><mb:mi>L</mb:mi></mb:mrow></mb:msub><mb:mo stretchy=\"false\">→</mb:mo><mb:msup><mb:mrow><mb:mi>π</mb:mi></mb:mrow><mb:mrow><mb:mn>0</mb:mn></mb:mrow></mb:msup><mb:mi>μ</mb:mi><mb:mover accent=\"true\"><mb:mrow><mb:mi>μ</mb:mi></mb:mrow><mb:mrow><mb:mo stretchy=\"false\">¯</mb:mo></mb:mrow></mb:mover><mb:mo stretchy=\"false\">)</mb:mo></mb:mrow></mb:math> to the global fit. The evolution of the result from one scenario to the next makes a strong case for the consideration of future measurement of <tb:math xmlns:tb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><tb:mrow><tb:mi>BR</tb:mi><tb:mo stretchy=\"false\">(</tb:mo><tb:msub><tb:mrow><tb:mi>K</tb:mi></tb:mrow><tb:mrow><tb:mi>L</tb:mi></tb:mrow></tb:msub><tb:mo stretchy=\"false\">→</tb:mo><tb:msup><tb:mrow><tb:mi>π</tb:mi></tb:mrow><tb:mrow><tb:mn>0</tb:mn></tb:mrow></tb:msup><tb:mo>ℓ</tb:mo><tb:mover accent=\"true\"><tb:mrow><tb:mo>ℓ</tb:mo></tb:mrow><tb:mrow><tb:mo stretchy=\"true\">¯</tb:mo></tb:mrow></tb:mover><tb:mo stretchy=\"false\">)</tb:mo></tb:mrow></tb:math>. <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":"2 1","pages":""},"PeriodicalIF":5.0000,"publicationDate":"2025-01-10","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.l011701","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

Kaon physics is at an important experimental juncture with respect to the ongoing measurements of several observables. This work will build on the existing status by formulating different phenomenological analyses corresponding to different paths that may lie ahead. Beginning with the golden channels, K+→π+νν¯ and KLπ0νν¯, the paper will eventually cast the spotlight on the importance of a precise measurement of BR(KLπ0¯). The phenomenological analyses involve sequentially adding kaon physics observables at the projected final precision of their respective measurements to the global fit. More specifically, we consider three different scenarios with different sets of observables assumed at their final precisions. Beginning with BR(K+π+νν¯) and BR(KLπ0νν¯), we sequentially add BR(KLπ0ee¯) and BR(KLπ0μμ¯) to the global fit. The evolution of the result from one scenario to the next makes a strong case for the consideration of future measurement of BR(KLπ0¯). Published by the American Physical Society 2025
KL→π0 l_l_¯新测量方法的理论意义
Kaon物理学正处于一个重要的实验节点上,相对于几个可观测的正在进行的测量。这项工作将建立在现有的状态,通过制定不同的现象学分析对应于不同的路径,可能会摆在前面。本文将从K+→π+νν¯和KL→π0νν¯这两个黄金通道开始,最终将重点放在精确测量BR(KL→π0∑ν¯)的重要性上。现象学分析包括按顺序将各自测量的最终预测精度的kaon物理观测值添加到全局拟合中。更具体地说,我们考虑了三种不同的场景,假设在它们的最终精度下有不同的可观测集。从BR(K+→π+νν¯)和BR(KL→π0νν¯)开始,依次将BR(KL→π0ee¯)和BR(KL→π0μμ¯)加入到全局拟合中。结果从一种情况到另一种情况的演变,为考虑未来测量BR(KL→π0 r¯)提供了强有力的理由。2025年由美国物理学会出版
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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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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