Quarkonia, which are bound states of a heavy quark and antiquark, play a key role in probing the quark-gluon plasma (QGP). The dynamics of quarkonia in the QGP are encoded in their finite-temperature spectral functions. In this work, we estimate the quarkonium spectral functions in the pseudoscalar channel using ($2+1$)-flavor lattice QCD with a pion mass of 320 MeV, at temperatures of $220\mathrm{MeV}(1.2T_{pc})$, $251\mathrm{MeV}(1.4T_{pc})$, and $293\mathrm{MeV}(1.6T_{pc})$. Reconstructing the spectral function from the Euclidean lattice correlator is a well-known ill-posed problem, requiring additional physics-motivated input. We address this by smoothly matching contributions from different frequency regions of the spectral function, using appropriate physics valid for each region. The spectral function around $\omega \sim 2M_q$ is obtained using a nonperturbative complex potential, while for $\omega \gg 2M_q$ it is modeled using results from vacuum perturbation theory. Since the pseudoscalar channel does not receive a transport contribution near $\omega \sim 0$, we find that the combination of these two regions already provides a good description of the relativistic lattice pseudoscalar correlator. We observe a substantial thermal width in the ${\eta }_c(1S)$ state, indicating that pseudoscalar charmonium (${\eta }_c$) is nearing dissolution at the studied temperatures. In comparison, the ${\eta }_b$ ground state exhibits little change and remains well defined.

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• Finite temperature field theory
• Lattice QCD
• Quark-gluon plasma
• Quarkonia