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Tetraquark

physical science Maturity 11-13 Next article →

A tetraquark is an exotic meson made of four valence quarks. In particle physics, quarks are the fundamental building blocks of matter. Most particles follow a conventional quark model. For example, many common particles contain only two or three quarks. A tetraquark is different because it lies outside these standard classifications. It belongs to a larger group of particles called hadrons. Scientists have long suspected that these four-quark states are possible. Their existence is supported by quantum chromodynamics. This is the modern theory of strong interactions.

TQ EB ape hyp r1 8 r2 14 Act 3D Sim
TQ EB ape hyp r1 8 r2 14 Act 3D Sim

To understand how a tetraquark works, we must look at quantum chromodynamics. This theory explains the strong interaction between quarks. This force is governed by color charges. In these particles, confinement occurs due to these charges. Confinement means quarks cannot exist alone. Instead, they are connected by color flux tubes. These flux tubes are produced by the four static quark and antiquark charges. They act like attractive, string-like potentials. This pull keeps the four quarks bound together in a single state.

TQ EB ape hyp r1 8 r2 14 Act 3D Sim
TQ EB ape hyp r1 8 r2 14 Act 3D Sim

There are many different types of tetraquark states. Most observed tetraquarks have a specific quark content. They often consist of a light quark and a heavy quark. The light quarks include the up, down, or strange varieties. The heavy quarks include charm or bottom quarks. In scientific notation, these are often written as qQ. Here, q represents the light quark and Q represents the heavy quark. Antiquarks are also part of these structures. They are denoted with an overline symbol. Theoretical physicists also discuss states made of two light quarks or two heavy quarks. However, these specific types have not been reported by experiments yet.

Discovery of these particles has happened in stages during the 21st century. The search began with several candidates. In 2003, the Belle experiment in Japan proposed X(3872). The number 3872 represents its mass in MeV. The name X is temporary because scientists are still testing its properties. In 2004, the SELEX experiment at Fermilab suggested the DsJ(2632) state was a candidate. In 2007, Belle announced the Z(4430) state. Belle also found indications for the Y(4660) state that same year. In 2009, Fermilab announced the Y(4140) particle. These discoveries slowly built a map of exotic matter.

Major milestones have confirmed these particles are real. In 2010, researchers from DESY and Quaid-i-Azam University re-analyzed data. They found a well-defined tetraquark resonance linked to the (5S) meson. A significant breakthrough occurred in June 2013. The BES III experiment in China and the Belle experiment in Japan independently reported the Zc(3900). This was the first confirmed four-quark state. Later, in 2014, the LHCb experiment confirmed the Z(4430) state. This confirmation had a significance of over 13.9 sigma. This high number shows the discovery was very certain.

Recent years have brought even more specific findings. In 2016, the LHCb experiment announced three more candidates. These were named X(4274), X(4500), and X(4700). In 2020, LHCb discovered the X(6900) tetraquark. The ATLAS experiment also observed X(6900) in 2022. By 2023, the CMS experiment reported three states: X(6600), X(6900), and X(7300). There was also some debate regarding the X(5568). The DØ experiment reported evidence for it in 2016 and 2017. However, other experiments like LHCb, CMS, CDF, and ATLAS did not observe it.

These discoveries connect to the broader study of nuclear physics. By studying tetraquarks, scientists learn about the strong force. They also learn about color confinement. Every new state, like the cu or cd states found by LHCb, provides data. These particles help us understand how matter is held together at the smallest scales. The study of exotic hadrons continues to expand our knowledge of the universe.

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