# Charmonium resonances with $J^{PC}=1^{--}$ and $3^{--}$ from $\bar DD$   scattering on the lattice

**Authors:** S. Piemonte, S. Collins, D. Mohler, M. Padmanath, S. Prelovsek

arXiv: 1905.03506 · 2019-10-30

## TL;DR

This lattice QCD study investigates charmonium resonances with specific quantum numbers near the open-charm threshold, extracting their masses and widths, and compares findings with experimental data, including recent discoveries.

## Contribution

First lattice QCD analysis of charmonium resonances with J^{PC}=1^{--} and 3^{--} considering strong D D̄ transitions, providing resonance parameters and exploring quark mass effects.

## Key findings

- Identified the ψ(3770) resonance with mass 3780 MeV
- Observed the ψ(2S) as a bound state at 3666 MeV
- Found the X(3842) consistent with a 3^{--} resonance

## Abstract

We present a lattice QCD study of charmonium resonances and bound states with $J^{PC}=1^{--}$ and $3^{--}$ near the open-charm threshold, taking into account their strong transitions to $\bar DD$. Vector charmonia are the most abundant in the experimentally established charmonium spectrum, while recently LHCb reported also the first discovery of a charmonium with likely spin three. The $\bar DD$ scattering amplitudes for partial waves $l=1$ and $l=3$ are extracted on the lattice by means of the L\"uscher formalism, using multiple volumes and inertial frames. Parameterizations of the scattering amplitudes provide masses and widths of the resonances, as well as the masses of bound states. CLS ensembles with 2+1 dynamical flavors of non-perturbatively $O(a)$ improved Wilson quarks are employed with $m_\pi\simeq 280$ MeV, a single lattice spacing of $a\simeq0.086$ fm and two lattice spatial extents of $L=24$ and $32$. Two values of the charm quark mass are considered to examine the influence of the position of the $\bar{D}D$ threshold on the hadron masses. For the lighter charm quark mass we find the vector resonance $\psi(3770)$ with mass $m=3780(7)$ MeV and coupling $g=16.0(^{+2.1}_{-0.2})$ (related to the width), both consistent with their experimental values. The vector $\psi(2S)$ appears as a bound state with $m=3666(10)$ MeV. The charmonium resonance with $J^{PC}=3^{--}$ is found at $m=3831(^{+10}_{-16})$ MeV, consistent with the $X(3842)$ recently discovered by LHCb. At our heavier charm-quark mass the $\psi(2S)$ as well as the $\psi(3770)$ are bound states and the $X(3842)$ remains a resonance. We stress that all quoted uncertainties are only statistical, while lattice spacing effects and the approach to the physical point still need to be explored. This study of conventional charmonia sets the stage for more challenging future studies of unconventional charmonium-like states.

## Full text

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## Figures

63 figures with captions in the complete paper: https://tomesphere.com/paper/1905.03506/full.md

## References

56 references — full list in the complete paper: https://tomesphere.com/paper/1905.03506/full.md

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Source: https://tomesphere.com/paper/1905.03506