Charged current neutrino and antineutrino induced associated particle production from nucleons

IF 5.3 2区 物理与天体物理 Q1 Physics and Astronomy
A. Fatima, M. Sajjad Athar, S. K. Singh
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For the resonant contributions, we consider the low-lying spin-<g:math xmlns:g=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><g:mfrac><g:mn>1</g:mn><g:mn>2</g:mn></g:mfrac></g:math> resonances, such as <i:math xmlns:i=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><i:msub><i:mi>S</i:mi><i:mn>11</i:mn></i:msub><i:mo stretchy=\"false\">(</i:mo><i:mn>1650</i:mn><i:mo stretchy=\"false\">)</i:mo></i:math>, <m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><m:msub><m:mi>P</m:mi><m:mn>11</m:mn></m:msub><m:mo stretchy=\"false\">(</m:mo><m:mn>1710</m:mn><m:mo stretchy=\"false\">)</m:mo></m:math>, <q:math xmlns:q=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><q:msub><q:mi>P</q:mi><q:mn>11</q:mn></q:msub><q:mo stretchy=\"false\">(</q:mo><q:mn>1880</q:mn><q:mo stretchy=\"false\">)</q:mo></q:math>, and <u:math xmlns:u=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><u:msub><u:mi>S</u:mi><u:mn>11</u:mn></u:msub><u:mo stretchy=\"false\">(</u:mo><u:mn>1895</u:mn><u:mo stretchy=\"false\">)</u:mo></u:math>, and spin-<y:math xmlns:y=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><y:mfrac><y:mn>3</y:mn><y:mn>2</y:mn></y:mfrac></y:math> resonances, such as P</ab:mi>13</ab:mn></ab:msub>(</ab:mo>1720</ab:mn>)</ab:mo></ab:math> and <eb:math xmlns:eb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><eb:msub><eb:mi>P</eb:mi><eb:mn>13</eb:mn></eb:msub><eb:mo stretchy=\"false\">(</eb:mo><eb:mn>1900</eb:mn><eb:mo stretchy=\"false\">)</eb:mo></eb:math>, which have finite branching ratios to the <ib:math xmlns:ib=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><ib:mi>K</ib:mi><ib:mi mathvariant=\"normal\">Λ</ib:mi></ib:math> channel. 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The model is then applied to study the weak production of <rb:math xmlns:rb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><rb:mi>K</rb:mi><rb:mi mathvariant=\"normal\">Λ</rb:mi></rb:math> induced by the neutrinos and antineutrinos and predicts the numerical values for the <ub:math xmlns:ub=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><ub:msup><ub:mi>Q</ub:mi><ub:mn>2</ub:mn></ub:msup></ub:math> distribution <wb:math xmlns:wb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><wb:mo stretchy=\"false\">(</wb:mo><wb:mfrac><wb:mrow><wb:mi>d</wb:mi><wb:mi>σ</wb:mi></wb:mrow><wb:mrow><wb:mi>d</wb:mi><wb:msup><wb:mi>Q</wb:mi><wb:mn>2</wb:mn></wb:msup></wb:mrow></wb:mfrac><wb:mo stretchy=\"false\">)</wb:mo></wb:math>, the kinetic energy distribution for the outgoing kaon (</ac:mo>d</ac:mi>σ</ac:mi></ac:mrow>d</ac:mi>p</ac:mi>K</ac:mi></ac:msub></ac:mrow></ac:mfrac>)</ac:mo></ac:math>, and the total scattering cross sections (<ec:math xmlns:ec=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><ec:mi>σ</ec:mi></ec:math>) with and without a cut on the center of mass energy <gc:math xmlns:gc=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><gc:mi>W</gc:mi></gc:math>. The results presented in this work are relevant for the present and future accelerator experiments like MicroBooNE, T2K, NOvA, MINERvA, SBND, ICARUS, T2-HyperK, and DUNE as well as for the atmospheric neutrino experiments.","PeriodicalId":20167,"journal":{"name":"Physical Review D","volume":"45 1","pages":""},"PeriodicalIF":5.3000,"publicationDate":"2025-10-17","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/10.1103/6c5c-sl4t","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

In this work, we study the charged-current (anti)neutrino induced associated particle (KΛ) production (ΔS=0) from free nucleons in the energy region of a few GeV, relevant to the (anti)neutrino oscillation experiments with accelerator and atmospheric neutrinos. We employ a model based on effective Lagrangians to evaluate the contributions from the nonresonant and the resonant diagrams. The nonresonant background terms are calculated using a microscopic model derived from the SU(3) chiral Lagrangians. For the resonant contributions, we consider the low-lying spin-12 resonances, such as S11(1650), P11(1710), P11(1880), and S11(1895), and spin-32 resonances, such as P13(1720) and P13(1900), which have finite branching ratios to the KΛ channel. These resonant contributions are modeled using an effective phenomenological Lagrangian approach, with strong couplings determined from the experimental branching ratios and the decay widths to the KΛ channel. To fix the parameters of the vector current interaction, the model is first used to reproduce satisfactorily the MAMI@Mainz experimental data on the real photon induced scattering off the nucleon resulting an eta meson in the final state and with the CLAS@JLab data for the KΛ production in the final state. The partial conservation of the axial vector current hypothesis and the generalized Goldberger-Treiman relation are used to fix the parameters of the axial vector interaction. The model is then applied to study the weak production of KΛ induced by the neutrinos and antineutrinos and predicts the numerical values for the Q2 distribution (dσdQ2), the kinetic energy distribution for the outgoing kaon (dσdpK), and the total scattering cross sections (σ) with and without a cut on the center of mass energy W. The results presented in this work are relevant for the present and future accelerator experiments like MicroBooNE, T2K, NOvA, MINERvA, SBND, ICARUS, T2-HyperK, and DUNE as well as for the atmospheric neutrino experiments.
带电电流中微子和反中微子诱导核子产生相关粒子
在这项工作中,我们研究了带电电流(反)中微子诱导的伴生粒子(KΛ)产生(ΔS=0),这与加速器和大气中微子的(反)中微子振荡实验有关。我们采用一个基于有效拉格朗日量的模型来评价非共振图和共振图的贡献。非共振背景项的计算采用了由SU(3)手性拉格朗日量导出的微观模型。对于共振的贡献,我们考虑了低位置的自旋-12共振,如S11(1650), P11(1710), P11(1880)和S11(1895),以及自旋-32共振,如P13(1720)和P13(1900),它们与KΛ通道的分支比有限。这些共振贡献使用有效的现象学拉格朗日方法进行建模,从实验分支比和KΛ通道的衰减宽度确定强耦合。为了确定矢量电流相互作用的参数,首先用该模型令人满意地再现了真实光子散射导致最终状态的中子产生eta介子的MAMI@Mainz实验数据和最终状态产生KΛ的CLAS@JLab数据。利用轴向电流假设的部分守恒和广义Goldberger-Treiman关系确定了轴向相互作用的参数。应用该模型研究了中微子和反中微子诱导的KΛ弱产生,并预测了Q2分布(dσdQ2)、出射kaon的动能分布(dσdpK)和总散射截面(σ)在质能中心w上有切割和没有切割的数值。所得结果对MicroBooNE、T2K、NOvA、MINERvA、SBND、ICARUS、T2-HyperK等加速器实验具有一定的指导意义。DUNE以及大气中微子实验。
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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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