The ${ϕNN,J/ψNN,η_c NN}$ systems based on HAL QCD interactions

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Hauptverfasser: Wen, Liang-Zhen, Ma, Yao, Meng, Lu, Zhu, Shi-Lin
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Veröffentlicht: 2025
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author Wen, Liang-Zhen
Ma, Yao
Meng, Lu
Zhu, Shi-Lin
author_facet Wen, Liang-Zhen
Ma, Yao
Meng, Lu
Zhu, Shi-Lin
contents We investigate the existence of bound states and resonances in the ${ϕNN, J/ψNN, η_c NN}$ systems using HAL QCD interactions for ${ϕN, J/ψN}$, and ${η_c N}$. We employ the Gaussian expansion method to solve the complex-scaled Schrödinger equation and find no resonances or bound states in the ${J/ψNN}$ and ${η_c NN}$ systems. We estimate the interaction between charmonium and nuclei, concluding that the $J/ψ$ or $η_c$ is likely to bind with ${}^3\mathrm{H}$, ${}^3\mathrm{He}$, ${}^4\mathrm{He}$, and heavier nuclei. For the $ϕNN$ system, the lattice QCD $ϕN\left({ }^2 S_{1 / 2}\right)$ interaction is absent. We combine the $ϕp$ correlation function analysis and HAL QCD results in Model A. We assume the spin-spin interactions for $J/ψN$ and $ϕN$ systems are inversely proportional to their masses in Model B. Model A predicts a stronger $ϕN({}^2 S_{1/2})$ interaction and permits a two-body bound state, whereas Model B suggests the interaction is attractive but too weak to form a bound state. Both models predict bound states for the $I(J^P) = 0(0^-)$ and $0(1^-)$ $ϕNN$ systems. In Model A, these states are deeply bound with binding energies exceeding 15 MeV and remain existent when considering parameter uncertainties. In contrast, these states are very loosely bound in Model B, with binding energies below 1 MeV and an existent probability of about 60\% when parameter uncertainties are considered. In both models, there exist very loosely bound $I(J^P) = 0(2^-)$ three-body states which resemble a $ϕ$-d atom with the $ϕ$ meson surrounding the deuteron, but their existences are sensitive to parameter uncertainties. No bound states or resonances are found in the isovector $I(J^P) = 1(1^-)$ $ϕNN$ system.
format Preprint
id arxiv_https___arxiv_org_abs_2503_11938
institution arXiv
publishDate 2025
record_format arxiv
spellingShingle The ${ϕNN,J/ψNN,η_c NN}$ systems based on HAL QCD interactions
Wen, Liang-Zhen
Ma, Yao
Meng, Lu
Zhu, Shi-Lin
High Energy Physics - Phenomenology
High Energy Physics - Experiment
High Energy Physics - Lattice
Nuclear Experiment
Nuclear Theory
We investigate the existence of bound states and resonances in the ${ϕNN, J/ψNN, η_c NN}$ systems using HAL QCD interactions for ${ϕN, J/ψN}$, and ${η_c N}$. We employ the Gaussian expansion method to solve the complex-scaled Schrödinger equation and find no resonances or bound states in the ${J/ψNN}$ and ${η_c NN}$ systems. We estimate the interaction between charmonium and nuclei, concluding that the $J/ψ$ or $η_c$ is likely to bind with ${}^3\mathrm{H}$, ${}^3\mathrm{He}$, ${}^4\mathrm{He}$, and heavier nuclei. For the $ϕNN$ system, the lattice QCD $ϕN\left({ }^2 S_{1 / 2}\right)$ interaction is absent. We combine the $ϕp$ correlation function analysis and HAL QCD results in Model A. We assume the spin-spin interactions for $J/ψN$ and $ϕN$ systems are inversely proportional to their masses in Model B. Model A predicts a stronger $ϕN({}^2 S_{1/2})$ interaction and permits a two-body bound state, whereas Model B suggests the interaction is attractive but too weak to form a bound state. Both models predict bound states for the $I(J^P) = 0(0^-)$ and $0(1^-)$ $ϕNN$ systems. In Model A, these states are deeply bound with binding energies exceeding 15 MeV and remain existent when considering parameter uncertainties. In contrast, these states are very loosely bound in Model B, with binding energies below 1 MeV and an existent probability of about 60\% when parameter uncertainties are considered. In both models, there exist very loosely bound $I(J^P) = 0(2^-)$ three-body states which resemble a $ϕ$-d atom with the $ϕ$ meson surrounding the deuteron, but their existences are sensitive to parameter uncertainties. No bound states or resonances are found in the isovector $I(J^P) = 1(1^-)$ $ϕNN$ system.
title The ${ϕNN,J/ψNN,η_c NN}$ systems based on HAL QCD interactions
topic High Energy Physics - Phenomenology
High Energy Physics - Experiment
High Energy Physics - Lattice
Nuclear Experiment
Nuclear Theory
url https://arxiv.org/abs/2503.11938