Year: 2026
Type: conference-paper
Abstract: In this proceeding, we report the non-perturbative potential between a heavy quark–antiquark pair in a QCD plasma at finite temperature. We compute the spin-dependent component of the thermal potential using temporal Wilson line correlators with insertions of the color-magnetic field. The calculations are performed in quenched QCD at $1.5$ times the deconfinement temperature $T_d$, on a four-dimensional lattice with spatial extent $N_s = 68$, and temporal extents $N_\tau = 16$ and $20$. For the first time, we show that $V_{\text{ss}}(r)$ develops an imaginary part at finite temperature, a feature similar to that observed in the static potential. Finally, we discuss the physical implications of our results for understanding the dissociation of quarkonium bound states in the quark–gluon plasma.
DOI: 10.22323/1.518.0102
Language: English
Subfield: Nuclear and High Energy Physics
Field: Physics and Astronomy
Domain: Physical Sciences
Open Access status: hybrid
OpenAlex ID: W7154298170
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