{"title":"超重子光谱学 70 年:奇异Ξ重子、Ω重子以及粲重子和底重子的光谱回顾。","authors":"Volker Crede, John Yelton","doi":"10.1088/1361-6633/ad7610","DOIUrl":null,"url":null,"abstract":"<p><p>The first hyperon was discovered about 70 years ago, but the nature of these particles, particularly with regard to multistrange hyperons, and many of their properties can still be considered to be literally strange. A dedicated and successful global spectroscopy program in the 1960s and 1970s usingK-beams revealed many multistrange candidates, but the available evidence of their existence is statistically limited. For this reason, there is still much to learn about the systematics of the spectrum of excited hyperon states and what they have in common with their non-strange companions, or how they differ from the nucleon and Δ resonances. Results from photo- and electroproduction experiments off the proton and neutron using polarized beams and targets have provided intriguing evidence for new nucleon excitations and shed light on the structure of some of the known nucleon and Δ states. Recent years have also seen a great deal of progress in the field of charmed and bottom baryon spectroscopy. Unprecedented data from the Large Hadron Collider in particular indicate continued rapid progress in the field of bottom baryons. On the theoretical side, baryons with one heavy quark<i>Q</i>and a light<i>qq</i>system serve as an ideal laboratory for studying light<i>qq</i>(diquark) correlations and the dynamics of the light quarks in the colour environment of a heavy quark. In this review, we discuss the status of doubly and triply strange Ξ as well as Ω baryons, and the properties of all the known charmed and bottom states. The comparison of the two heavy sectors reveals many similarities as predicted by heavy-quark symmetries, together with differences in mass splittings easily understood by potential models. The multi-strange hyperons bridge the under-explored gap between the light- and the heavy-flavour baryons. How do the properties of a singly charmed<i>Q</i>-<i>qq</i>system change with decreasing mass of the heavy quark in the transition to a doubly strange<i>q</i>-<i>QQ</i>system with a heavier quark-quark system relative to one light quark? Significant progress towards understanding hyperon resonances is expected in coming years from the ongoing experiments at the high-energy collider facilities and planned experiments using<i>K</i>beams at Jefferson Laboratory and J-PARC.</p>","PeriodicalId":74666,"journal":{"name":"Reports on progress in physics. 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For this reason, there is still much to learn about the systematics of the spectrum of excited hyperon states and what they have in common with their non-strange companions, or how they differ from the nucleon and Δ resonances. Results from photo- and electroproduction experiments off the proton and neutron using polarized beams and targets have provided intriguing evidence for new nucleon excitations and shed light on the structure of some of the known nucleon and Δ states. Recent years have also seen a great deal of progress in the field of charmed and bottom baryon spectroscopy. Unprecedented data from the Large Hadron Collider in particular indicate continued rapid progress in the field of bottom baryons. On the theoretical side, baryons with one heavy quark<i>Q</i>and a light<i>qq</i>system serve as an ideal laboratory for studying light<i>qq</i>(diquark) correlations and the dynamics of the light quarks in the colour environment of a heavy quark. In this review, we discuss the status of doubly and triply strange Ξ as well as Ω baryons, and the properties of all the known charmed and bottom states. The comparison of the two heavy sectors reveals many similarities as predicted by heavy-quark symmetries, together with differences in mass splittings easily understood by potential models. The multi-strange hyperons bridge the under-explored gap between the light- and the heavy-flavour baryons. How do the properties of a singly charmed<i>Q</i>-<i>qq</i>system change with decreasing mass of the heavy quark in the transition to a doubly strange<i>q</i>-<i>QQ</i>system with a heavier quark-quark system relative to one light quark? Significant progress towards understanding hyperon resonances is expected in coming years from the ongoing experiments at the high-energy collider facilities and planned experiments using<i>K</i>beams at Jefferson Laboratory and J-PARC.</p>\",\"PeriodicalId\":74666,\"journal\":{\"name\":\"Reports on progress in physics. Physical Society (Great Britain)\",\"volume\":\" \",\"pages\":\"\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2024-09-30\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Reports on progress in physics. 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引用次数: 0
摘要
第一个超子是在大约 70 年前被发现的,但这些粒子的性质,特别是多量程超子,以及它们的许多特性仍然可以被认为是非常奇怪的。20 世纪 60 年代和 70 年代,利用 K 光束开展的一项专门的全球光谱计划取得了成功,发现了许多多量程候选粒子,但从统计学角度来看,证明它们存在的现有证据非常有限。因此,关于激发超子态光谱的系统性,它们与非超子态的共同点,或者它们与核子和Δ共振的区别,还有很多东西需要了解。利用偏振光束和靶子对质子和中子进行的光子和电子产生实验的结果为新的核子激发态提供了引人入胜的证据,并揭示了一些已知核子和Δ态的结构。近年来,粲重子和底重子光谱学领域也取得了巨大进展。特别是来自大型强子对撞机的前所未有的数据表明,底重子领域继续取得快速进展。在理论方面,具有一个重夸克 Q 和一个轻 qq 系统的重子是研究轻 qq(二夸克)相关性和轻夸克在重夸克颜色环境中的动力学的理想实验室。在这篇综述中,我们讨论了双奇异Ξ和三奇异Ξ以及Ω重子的现状,以及所有已知粲态和底态的性质。通过对这两个重部门的比较,我们发现了重夸克对称性所预言的许多相似之处,以及潜在模型容易理解的质量分裂差异。多量程超子弥补了轻重子之间探索不足的差距。在过渡到双奇异q-QQ系统(相对于一个轻夸克,夸克-夸克系统更重)的过程中,单粲Q-qq系统的性质如何随着重夸克质量的降低而变化?高能对撞机设施正在进行的实验以及计划在杰斐逊实验室和 J-PARC 使用 K 波束进行的实验预计将在未来几年里为了解超子共振取得重大进展。
70 years of hyperon spectroscopy: a review of strange Ξ, Ω baryons, and the spectrum of charmed and bottom baryons.
The first hyperon was discovered about 70 years ago, but the nature of these particles, particularly with regard to multistrange hyperons, and many of their properties can still be considered to be literally strange. A dedicated and successful global spectroscopy program in the 1960s and 1970s usingK-beams revealed many multistrange candidates, but the available evidence of their existence is statistically limited. For this reason, there is still much to learn about the systematics of the spectrum of excited hyperon states and what they have in common with their non-strange companions, or how they differ from the nucleon and Δ resonances. Results from photo- and electroproduction experiments off the proton and neutron using polarized beams and targets have provided intriguing evidence for new nucleon excitations and shed light on the structure of some of the known nucleon and Δ states. Recent years have also seen a great deal of progress in the field of charmed and bottom baryon spectroscopy. Unprecedented data from the Large Hadron Collider in particular indicate continued rapid progress in the field of bottom baryons. On the theoretical side, baryons with one heavy quarkQand a lightqqsystem serve as an ideal laboratory for studying lightqq(diquark) correlations and the dynamics of the light quarks in the colour environment of a heavy quark. In this review, we discuss the status of doubly and triply strange Ξ as well as Ω baryons, and the properties of all the known charmed and bottom states. The comparison of the two heavy sectors reveals many similarities as predicted by heavy-quark symmetries, together with differences in mass splittings easily understood by potential models. The multi-strange hyperons bridge the under-explored gap between the light- and the heavy-flavour baryons. How do the properties of a singly charmedQ-qqsystem change with decreasing mass of the heavy quark in the transition to a doubly strangeq-QQsystem with a heavier quark-quark system relative to one light quark? Significant progress towards understanding hyperon resonances is expected in coming years from the ongoing experiments at the high-energy collider facilities and planned experiments usingKbeams at Jefferson Laboratory and J-PARC.