Abstract:When studying tetraquark states using the method of QCD sum rules, we find some tetraquark currents, such as ūLγµdL dLγ µ uL and ūLγµdL dRγ µ uR, etc. We calculate their correlation functions using the method of operator product expansion, and find that non-perturbative QCD effects do not contribute much to them. This indicates the possible existence of tetraquark states composed of bare quarks with abnormally small masses. We study the possible assignment of the X17 as such a state. We argue that the Atomki e… Show more
“…Interested readers may consult Refs. [106,107,108,109,110,111,112,113,114,115,116,117,118,119] for a systematical study on chiral properties of the light baryon and tetraquark fields.…”
The past decades witnessed the golden era of hadron physics. Many excited open heavy flavor mesons and baryons have been observed since 2017. We shall provide an updated review of the recent experimental and theoretical progresses in this active field. Besides the conventional heavy hadrons, we shall also review the recently observed open heavy flavor tetraquark states X(2900) and T + cc (3875) as well as the hidden heavy flavor multiquark states X(6900), P cs (4459) 0 , Z cs (3985) − , Z cs (4000) + , and Z cs (4220) + . We will also cover the recent progresses on the glueballs and light hybrid mesons, which are the direct manifestations of the non-Abelian SU (3) gauge interaction of the Quantum Chromodynamics in the low-energy region.
“…Interested readers may consult Refs. [106,107,108,109,110,111,112,113,114,115,116,117,118,119] for a systematical study on chiral properties of the light baryon and tetraquark fields.…”
The past decades witnessed the golden era of hadron physics. Many excited open heavy flavor mesons and baryons have been observed since 2017. We shall provide an updated review of the recent experimental and theoretical progresses in this active field. Besides the conventional heavy hadrons, we shall also review the recently observed open heavy flavor tetraquark states X(2900) and T + cc (3875) as well as the hidden heavy flavor multiquark states X(6900), P cs (4459) 0 , Z cs (3985) − , Z cs (4000) + , and Z cs (4220) + . We will also cover the recent progresses on the glueballs and light hybrid mesons, which are the direct manifestations of the non-Abelian SU (3) gauge interaction of the Quantum Chromodynamics in the low-energy region.
“…This mechanism also makes the QCD vacuum possess nontrivial structures, such as the nonzero quark condensates. Interested readers may consult [108][109][110][111][112][113][114][115][116][117][118][119][120][121][122] for a systematical study on chiral properties of the light baryon and tetraquark fields.…”
The past decades witnessed the golden era of hadron physics. Many excited open heavy flavor mesons and baryons have been observed since 2017. We shall provide an updated review of the recent experimental and theoretical progresses in this active field. Besides the conventional heavy hadrons, we shall also review the recently observed open heavy flavor tetraquark states X(2900) and Tcc(3875) as well as the hidden heavy flavor multiquark states X(6900), Pcs(4459), Zcs(3985), Zcs(4000), and Zcs(4220). We will also cover the recent progresses on the glueballs and light hybrid mesons, which are the direct manifestations of the non-Abelian SU(3) gauge interaction of the Quantum Chromodynamics in the low-energy region.
“…For what concerns possible SM explanations, various Authors have proposed that the X17 resonance may be a new exotic QCD bound state. In [29] it has been proposed that the X17 resonance might be identified with a tetraquark, i.e. a four quarks QCD bound state, made up by first generation quarks.…”
Section: Summary Of the Experimental Status Of X17 Searchesmentioning
The workshop “Shedding light on X17” brings together scientists looking for the existence of a possible new light particle, often referred to as X17. This hypothetical particle can explain the resonant structure observed at $$\sim $$
∼
17 MeV in the invariant mass of electron-positron pairs, produced after excitation of nuclei such as $$^8\hbox {Be}$$
8
Be
and $$^4\hbox {He}$$
4
He
by means of proton beams at the Atomki Laboratory in Debrecen. The purpose of the workshop is to discuss implications of this anomaly, in particular theoretical interpretations as well as present and future experiments aiming at confirming the result and/or at providing experimental evidence for its interpretation.
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