Abstract

In the article, we investigate the diquark-diquark-antiquark type fully-heavy pentaquark states with the spin-parity JP=12− via the QCD sum rules for the first time, and obtain the masses Mccccc¯=7.93±0.15 GeV and Mbbbbb¯=23.91±0.15 GeV. We can search for the fully-heavy pentaquark states in the J/ψΩccc and ϒΩbbb invariant mass spectrum in the future.

Highlights

  • IntroductionWe usually classify the hadrons into the traditional quark-antiquark type mesons, three-quark baryons, and exotic states, such as the tetraquark (molecular) states, pentaquark (molecular) states and hexaquark (molecular) states, etc

  • In the quark models, we usually classify the hadrons into the traditional quark-antiquark type mesons, three-quark baryons, and exotic states, such as the tetraquark states, pentaquark states and hexaquark states, etc

  • The exotic states provide us with a unique subject to investigate the strong interaction, which governs the dynamics of the quarks and gluons, and the confinement mechanism

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Summary

Introduction

We usually classify the hadrons into the traditional quark-antiquark type mesons, three-quark baryons, and exotic states, such as the tetraquark (molecular) states, pentaquark (molecular) states and hexaquark (molecular) states, etc. In 2020, the LHCb collaboration observed a narrow structure X(6900) and a broad structure just above the J/ψJ/ψ threshold in the J/ψJ/ψ invariant mass spectrum [5], such structures are the first fully-heavy exotic multiquark candidates claimed experimentally up to now. It is a very important step in investigations of the heavy hadrons, and provides very important experimental constraints on the theoretical models. P-wave and D-wave diquarks as the basic building blocks to investigate the doubly-heavy baryon states, tetraquark states and pentaquark states, we expect to obtain larger hadron masses considering the additional contributions from the P-waves and D-wave.

QCD sum rules for the fully-heavy pentaquark states
Numerical results and discussions
Central value ccccc
Conclusion
Full Text
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