Analysis of the ${\frac{1}{2}}^{\pm}$ pentaquark states in the diquark-diquark-antiquark model with QCD sum rules

TL;DR

This paper systematically studies the masses and properties of hidden-charm pentaquark states with different strangeness using QCD sum rules, constructing specific interpolating currents and considering vacuum condensates up to dimension-10.

Contribution

It introduces a comprehensive QCD sum rule analysis for ${rac{1}{2}}^{ ext{±}}$ pentaquark states with detailed current constructions and scale-setting methods, including SU(3) breaking effects.

Findings

Predicted masses for various strangeness states.

Method for determining energy scales of spectral densities.

Analysis of vacuum condensate contributions up to dimension-10.

Abstract

In this article, we construct both the axialvector-diquark-axialvector-diquark-antiquark type and axialvector-diquark-scalar-diquark-antiquark type interpolating currents, then calculate the contributions of the vacuum condensates up to dimension-10 in the operator product expansion, and study the masses and pole residues of the $J^P={\frac{1}{2}}^\pm$ hidden-charm pentaquark states with the QCD sum rules in a systematic way. In calculations, we use the formula $\mu=\sqrt{M^2_{P}-(2{\mathbb{M}}_c)^2}$ to determine the energy scales of the QCD spectral densities. We take into account the $SU(3)$ breaking effects of the light quarks, and obtain the masses of the hidden charm pentaquark states with the strangeness $S=0,\,-1,\,-2,\,-3$, which can be confronted with the experimental data in the future.