Exotic Hadronic States

Jeff Wheeler May 1, 2018

Abstract Background: The current model of predicts all hadronic ​ in to exist in one of two families: or . However, the laws do not forbid larger collections of from existing. and ​ have long been postulated. Purpose: Advance the particle ​ ​ landscape into a regime including more complex systems of quarks. Studying these systems could help physicists gain greater insight into the nature of the strong force. Methods: Many different particle and detectors of varying ​ ​ energies and sensitivities were used to search for evidence of four- or five- states. Results: After a few false alarms, evidence for the existence of both ​ ​ tetraquark and pentaquark was obtained from multiple experiments. Conclusion: ​ Positive results from around the world have shown exotic hadronic states of matter to exist, and extended research will continue to test the leading theories of today and help further our understanding of the laws of physics.

I. Introduction

Since the discovery of atomic particles, scientists have attempted to determine their individual properties and produce a systematic method of grouping based on those properties. In the early days of , little was known besides the mere existence of and . With the advent of particle colliders and detectors, however, the collection of known particles grew rapidly. It wasn’t until 1961 that a successful classification system was produced independently by American physicist Murray Gell-Mann and Israeli physicist Yuval Ne’eman. This method was built upon the symmetric representation group SU(3). In this configuration, the spin-1/2 baryons were arranged in an octet (see fig. 1), which is what model. Gell-Mann and Russian-American inspired Gell-Mann to dub the system the physicist George Zweig postulated three new “”. With this system, other particles, called quarks, that would constitute categories of particles could be grouped the triplet. With the triplet in place, along with similarly; for example, spin-3/2 baryons and its conjugate, all of the other representations vector mesons were arranged in decuplets and could be constructed [1]. Gell-Mann and Zweig nonets, respectively, where “nonet” is the term had not only produced a theory of for the combined group of the singlet and octet. classification, but also a theory of the hadronic This method of grouping proved to be constituents: a theory of subatomic particles. very successful, and even led to Gell-Mann The divides hadrons into postulating the existence of a yet undiscovered two groups: baryons and mesons. Baryons - consist of three quarks (qqq) or antiquarks particle, which he named Ω .​ Only three years ​ later, the particle was discovered at (qqq) , and mesons are composed of a Brookhaven National Laboratory [1]! quark-antiquark pair (qq) . However, while all The success of the eightfold way paved of the particles detected prior to the turn of the the road for the next advancement in particle twenty-first century fit into one of these two physics. While Gell-Mann’s method showed categories, they are not exhaustive. In fact, promise categorizing hadrons into singlets, Gell-Mann himself postulated the existence of octets, and decuplets, it was missing an integral particles with a higher quark content [1]. part of the representation group: the triplet. Continued work in the field produced a This issue led to the formulation of the quark new theory of the strong , quantum

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chromodynamics (QCD), using the subatomic [5], but there are some theorists who believe the building blocks postulated by Gell-Mann and particles detected were more of a “ Zweig along with eight new vector ”. This configuration would consist of called . In addition to the configurations two traditional mesons that are loosely joined of quarks given by the quark model, QCD together [3] (see fig. 2); the attractive force calculations shows that particles containing four between the mesons could come from a or five quarks could also exist [2]. exchange [1]. Similarly, it would be possible for a pentaquark signature to be created from a II. Structure joined system of a and a meson, opposed to a true pentaquark. In QCD, a new quantum property called is introduced. There are three colors, each with a corresponding anticolor: red, green, blue, antired, antigreen, and antiblue. Each quark carries a single color charge, and all particles composed of quarks must be colorless in total. Particles can be colorless by containing all three colors in equal amounts or with equal amounts of color and its anticolor. The rule that all quark particles must be colorless is referred to as . With color confinement, we recover the two families of hadrons from the quark model with an added twist. In traditional baryons, each quark must have a different color charge in order to be colorless in total; similarly, mesons must be composed of a colored quark and a quark of the corresponding anticolor. However, baryons and mesons are not the only colorless configurations III. Experimental detection of quarks. Colorless four-quark systems can be composed of two colored quarks and their Since their postulation in the antiquarks (qqqq) , or five-quark systems can mid-1960’s, there have been several exist with four quarks and an antiquark experiments attempting to discover them. Here, (qqqqq) . I will focus on a few experiments detecting Despite evidence for tetraquark and tetraquark candidates and the LCHb experiment pentaquark particles discussed in a later section, detecting pentaquark candidates. there is still some debate on the true structure of the detected systems. For example, four-quark systems were observed at the

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III.1 researchers claimed to have evidence of a 2 pentaquark of 1500 MeV/c .​ Additional ​ In the early 2010’s, two experiments data analyses from several other groups claimed published papers claiming discovery of to have reproduced the findings. These claims four-quark systems. One of these experiments did not hold, however, and after other repeated was the Belle collaboration. The Belle detector experiments of the same type failed to is located at the High Energy Accelerator reproduce the signature in the data, the Research Organization (KEK) in Tsukuba, pentaquark seemed to be ruled out of existence Japan. While analyzing - [2]. collisions, the detector recorded data consistent Over a decade later, the pentaquark with the decay of a four-quark system. These would make a resurgence. This time, the news systems were determined to consist of two came from researchers at the LHCb experiment charm quarks and two lighter quarks, denoted at the Large Hadron (LHC) at the by Zc(3900) [3]. European Organization for Nuclear Research ​ ​ The Zc(3900) particle was also (CERN) in Geneva, Switzerland. Unlike the ​ ​ independently discovered by the Beijing previous particle colliders mentioned, the LHC Spectrometer III (BESIII) housed at the Beijing studies -proton collisions and operates at Electron Positron Collider. much higher energies. This allows the creation As mentioned in the previous section, of higher-mass particles. In 2015, the LHCb there is still some debate regarding the actual announced new evidence for the elusive internal structure of the detected four-quark pentaquark [4]; and this time, they weren’t even systems. Those in favor of true tetraquark looking for it! detection point out that the meson molecule While studying the decay of unstable should split apart upon decay, but this type of particles, researchers found something strange behavior has not been recorded. However, the in their data, collected between 2009 and 2012. 0 uncertainties in the measurements are consistent The surprise came from analyzing Λb decay. with both the molecule and tetraquark structures This the main decay channel is expected to be 0 * [3]. Λb → J/ψΛ (fig. 3a) with the further decay of Λ* → K−p being detected. However, there III.2 could also be some exotic decay channels, such 0 + − as the one given by Λb → P c K (fig. 3b), Just as the search for tetraquarks had + where P c denotes the pentaquark with raised some skepticism, the history of the composition (uudcc) and referred to as pentaquark discoveries have not always been “charmonium” [2,4]. widely accepted. The first announcement of a While analyzing their data, researchers + pentaquark, named Θ , was put forth in 2002 noticed bump growing sticking out over their from data collected at the SPring-8 synchrotron expected curve (see fig. 4). Interestingly, due to in Harima, Japan. This experiment involved the infamous past of the pentaquark, the colliding high-energy and neutrons, and researchers originally ignored this anomalous 3

hump and continued their original research; The baryons and mesons of the quark model no however, they got to a point where they could longer encompassed all that was allowed in the no longer ignore their data. The bump was laws of particle physics, and since the very staring them right in the face, with an introduction of QCD, physicists have pondered astonishing significance of 9-sigma [2]! Not more exotic states of matter than those seen in only did the researchers find evidence for a new everyday life. Despite being postulated in the pentaquark particle, but the data showed mid-twentieth century, it wasn’t until the early evidence for two distinct short-lived objects twenty first that the first signs of tetra- and ​ 2 2 with of 4380 Mev/c 4450 Mev/c ,​ much pentaquarks were gathered. Results from 2011 ​ ​ higher masses than the Θ+ claimed to have been to 2015 showed significant evidence of exotic discovered previously [2]. quark states, and even though there is some debate on the data, the existence of some type of non-standard particle is hard to deny. Extended research into exotic quark states will further our knowledge of the most fundamental laws of physics and continue to put our best theories, namely QCD, to the test. Future work is needed to advance the exploration into the particle landscape. With higher energies and better detectors, researchers will be able to probe for more massive particles and delve deeper into the mysterious nature of the universe we inhabit.

IV. Conclusion

The landscape of particle physics has gone through some extreme changes over the last century. In the 1960’s, with the becoming overwhelmingly crowded, the introduction of the quark model brought some much needed order. The subsequent formulation of provided a radical new way of conceptualizing particles and their constituents along with a rigorous framework for doing calculations and making predictions.

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References

[1] Richard, Jean-Marc. “An introductions to the quark model.” arXiv:1205.4326v2 [hep-ph] (2012).

[2] Chalmers, Matthew. “Forsaken pentaquark particle spotten at CERN.” Nature 523, 267–268 ​ (16 July 2015). doi:10.1038/nature.2015.17968

[3] Powell, Devin. “Quark quartet opens fresh vista on matter.” Nature 498, 280–281 (20 June ​ 2013). doi:10.1038/498280a ​

[4] Aaij, R. et al. “Observation of J/ψp ​ ​ resonances consistent with pentaquark states in 0 − Λb → J/ψK p decays” Physical Review Letters, vol. 115, no. 7, 14 Aug. 2015, doi:https://doi.org/10.1103/PhysRevLett.115.07 2001.

[5] Adachi, I. et al. “Observation of two ​ ​ charged bottomonium-like resonances.” arXiv:1105.4583v3 [hep-ex] (2011).

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