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质子弱电荷的精确测量。

Precision measurement of the weak charge of the proton.

出版信息

Nature. 2018 May;557(7704):207-211. doi: 10.1038/s41586-018-0096-0. Epub 2018 May 9.

DOI:10.1038/s41586-018-0096-0
PMID:29743692
Abstract

Large experimental programmes in the fields of nuclear and particle physics search for evidence of physics beyond that explained by current theories. The observation of the Higgs boson completed the set of particles predicted by the standard model, which currently provides the best description of fundamental particles and forces. However, this theory's limitations include a failure to predict fundamental parameters, such as the mass of the Higgs boson, and the inability to account for dark matter and energy, gravity, and the matter-antimatter asymmetry in the Universe, among other phenomena. These limitations have inspired searches for physics beyond the standard model in the post-Higgs era through the direct production of additional particles at high-energy accelerators, which have so far been unsuccessful. Examples include searches for supersymmetric particles, which connect bosons (integer-spin particles) with fermions (half-integer-spin particles), and for leptoquarks, which mix the fundamental quarks with leptons. Alternatively, indirect searches using precise measurements of well predicted standard-model observables allow highly targeted alternative tests for physics beyond the standard model because they can reach mass and energy scales beyond those directly accessible by today's high-energy accelerators. Such an indirect search aims to determine the weak charge of the proton, which defines the strength of the proton's interaction with other particles via the well known neutral electroweak force. Because parity symmetry (invariance under the spatial inversion (x, y, z) → (-x, -y, -z)) is violated only in the weak interaction, it provides a tool with which to isolate the weak interaction and thus to measure the proton's weak charge . Here we report the value 0.0719 ± 0.0045, where the uncertainty is one standard deviation, derived from our measured parity-violating asymmetry in the scattering of polarized electrons on protons, which is -226.5 ± 9.3 parts per billion (the uncertainty is one standard deviation). Our value for the proton's weak charge is in excellent agreement with the standard model and sets multi-teraelectronvolt-scale constraints on any semi-leptonic parity-violating physics not described within the standard model. Our results show that precision parity-violating measurements enable searches for physics beyond the standard model that can compete with direct searches at high-energy accelerators and, together with astronomical observations, can provide fertile approaches to probing higher mass scales.

摘要

大型实验计划在核物理和粒子物理领域寻找超出当前理论解释的物理证据。希格斯玻色子的观测完成了标准模型预测的粒子集合,该模型目前为基本粒子和力提供了最佳描述。然而,该理论的局限性包括无法预测基本参数,例如希格斯玻色子的质量,以及无法解释暗物质和能量、引力以及宇宙中的物质-反物质不对称性等现象。这些局限性激发了在后希格斯时代通过高能加速器中额外粒子的直接产生来寻找超越标准模型的物理,迄今为止这些搜索尚未成功。例如,对超对称粒子的搜索,将玻色子(整数自旋粒子)与费米子(半整数自旋粒子)联系起来,以及对轻夸克的搜索,将基本夸克与轻子混合。或者,使用对标准模型预测良好的可观测量的精确测量进行间接搜索,可以为超越标准模型的物理提供高度针对性的替代测试,因为它们可以达到当今高能加速器无法直接达到的质量和能量尺度。这种间接搜索旨在确定质子的弱电荷,该电荷定义了质子通过众所周知的弱电相互作用与其他粒子相互作用的强度。由于宇称对称性(在空间反转(x,y,z)→(-x,-y,-z)下不变)仅在弱相互作用中被破坏,因此它提供了一种工具,可以分离弱相互作用,从而测量质子的弱电荷。在这里,我们报告的数值为 0.0719±0.0045,其中不确定性为一个标准差,来自我们对极化电子在质子上散射的宇称破坏不对称性的测量,其值为-226.5±9.3 十亿分之一(不确定性为一个标准差)。我们对质子弱电荷的测量值与标准模型非常吻合,并对任何超出标准模型描述的半轻宇称破坏物理设定了万亿电子伏特量级的约束。我们的结果表明,精确的宇称破坏测量可以进行超越标准模型的搜索,这些搜索可以与高能加速器中的直接搜索相媲美,并且与天文观测一起,可以为探测更高质量尺度提供富有成效的方法。

相似文献

1
Precision measurement of the weak charge of the proton.质子弱电荷的精确测量。
Nature. 2018 May;557(7704):207-211. doi: 10.1038/s41586-018-0096-0. Epub 2018 May 9.
2
A detailed map of Higgs boson interactions by the ATLAS experiment ten years after the discovery.十年后 ATLAS 实验对希格斯玻色子相互作用的详细地图。
Nature. 2022 Jul;607(7917):52-59. doi: 10.1038/s41586-022-04893-w. Epub 2022 Jul 4.
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Measurement of parity violation in electron-quark scattering.测量电子-夸克散射中的宇称破坏。
Nature. 2014 Feb 6;506(7486):67-70. doi: 10.1038/nature12964.
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A new boson with a mass of 125 GeV observed with the CMS experiment at the Large Hadron Collider.CMS 实验在大型强子对撞机上观测到质量为 125GeV 的新玻色子。
Science. 2012 Dec 21;338(6114):1569-75. doi: 10.1126/science.1230816.
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A parts-per-billion measurement of the antiproton magnetic moment.反质子磁矩的十亿分之一测量值。
Nature. 2017 Oct 18;550(7676):371-374. doi: 10.1038/nature24048.
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New physics searches at the BESIII experiment.北京谱仪III实验中的新物理搜索。
Natl Sci Rev. 2021 Oct 20;8(11):nwab189. doi: 10.1093/nsr/nwab189. eCollection 2021 Nov.
7
Precision determination of electroweak coupling from atomic parity violation and implications for particle physics.基于原子宇称不守恒对电弱耦合的精确测定及其对粒子物理学的影响。
Phys Rev Lett. 2009 May 8;102(18):181601. doi: 10.1103/PhysRevLett.102.181601. Epub 2009 May 5.
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Constraints on models of the Higgs boson with exotic spin and parity using decays to bottom-antibottom quarks in the full CDF data set.利用完整CDF数据集中希格斯玻色子衰变为底夸克对的过程,对具有奇异自旋和宇称的希格斯玻色子模型的限制。
Phys Rev Lett. 2015 Apr 10;114(14):141802. doi: 10.1103/PhysRevLett.114.141802.
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Beyond the standard Higgs after the 125 GeV Higgs discovery.在发现 125GeV 希格斯玻色子之后的标准希格斯玻色子之外。
Philos Trans A Math Phys Eng Sci. 2015 Jan 13;373(2032):1-7.
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A 16-parts-per-trillion measurement of the antiproton-to-proton charge-mass ratio.反质子与质子电荷质量比的测量值为万亿分之十六。
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