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Long-Range $N-J/ψ$ Interaction from an Operator Product Expansion Perspective

Seokwoo Yeo, In Woo Park, Su Houng Lee

TL;DR

The paper addresses the long-range part of the $N$-$J/\\psi$ interaction in nuclear matter, motivated by lattice results showing attraction driven by two-pion exchange. It employs QCD sum rules with an operator-product expansion up to dimension-6, isolating the pion-coupled four-quark condensates via a Fierz transformation and incorporating density dependence through a parameter $\\kappa$. The results yield a small but meaningful in-medium mass decrease for the $J/\\psi$ that qualitatively agrees with lattice findings, with the magnitude and sign depending on $\\kappa$ and $\\alpha_{s,\\mathrm{IR}}$, and vanish or reverse if the pion-coupled component is not isolated. This work links chiral-symmetry restoration effects to heavy-quark systems and underscores the importance of properly accounting for long-distance hadronic contributions in QCD sum-rule analyses of in-medium hadrons.

Abstract

A recent lattice QCD study has shown that the $N-J/ψ$ potential is attractive at all distances, and its long-range tail is well described by two-pion exchange. Here, we study to what extent the long-range part of the attraction can be reproduced from the perspective of the operator product expansion (OPE). This is accomplished by extracting the leading-order four-quark operator that couples to two pions and calculating its contribution to the $J/ψ$ mass in nuclear matter, to linear order in density, within the QCD sum rule framework. Using previous estimates of the four-quark operators for the chiral symmetric and breaking parts, we obtain a mass decrease that is smaller in magnitude but qualitatively consistent with the attraction obtained in the lattice QCD calculation. By expressing the interaction in terms of four-quark operators, we can analyze the effects of chiral symmetry restoration in dense matter on the masses of the $J/ψ$ and other mesons composed of heavy quarks.

Long-Range $N-J/ψ$ Interaction from an Operator Product Expansion Perspective

TL;DR

The paper addresses the long-range part of the - interaction in nuclear matter, motivated by lattice results showing attraction driven by two-pion exchange. It employs QCD sum rules with an operator-product expansion up to dimension-6, isolating the pion-coupled four-quark condensates via a Fierz transformation and incorporating density dependence through a parameter . The results yield a small but meaningful in-medium mass decrease for the that qualitatively agrees with lattice findings, with the magnitude and sign depending on and , and vanish or reverse if the pion-coupled component is not isolated. This work links chiral-symmetry restoration effects to heavy-quark systems and underscores the importance of properly accounting for long-distance hadronic contributions in QCD sum-rule analyses of in-medium hadrons.

Abstract

A recent lattice QCD study has shown that the potential is attractive at all distances, and its long-range tail is well described by two-pion exchange. Here, we study to what extent the long-range part of the attraction can be reproduced from the perspective of the operator product expansion (OPE). This is accomplished by extracting the leading-order four-quark operator that couples to two pions and calculating its contribution to the mass in nuclear matter, to linear order in density, within the QCD sum rule framework. Using previous estimates of the four-quark operators for the chiral symmetric and breaking parts, we obtain a mass decrease that is smaller in magnitude but qualitatively consistent with the attraction obtained in the lattice QCD calculation. By expressing the interaction in terms of four-quark operators, we can analyze the effects of chiral symmetry restoration in dense matter on the masses of the and other mesons composed of heavy quarks.

Paper Structure

This paper contains 9 sections, 23 equations, 1 figure, 1 table.

Figures (1)

  • Figure 1: The mass shifts of $J/\psi$ as a function of $\kappa$. We present results for larger infrared strong coupling constants, $\alpha_{s,\text{IR}}$.