Computing Jet Transport Coefficients On The Lattice

TL;DR

This paper presents the first continuum-extrapolated lattice QCD calculation of the jet transport coefficient , revealing a temperature dependence different from weak-coupling predictions, with implications for understanding jet quenching in heavy-ion collisions.

Contribution

It introduces a novel lattice QCD formalism to compute jet transport coefficients , including continuum extrapolation and non-perturbative results for pure SU(3) and preliminary unquenched estimates.

Findings

 shows a non-weak-coupling temperature dependence.

Results obtained for a wide temperature range from 200MeV to 1GeV.

Preliminary unquenched results are consistent with quenched calculations.

Abstract

The leading jet transport coefficients $\hat{q}$ or $\hat{e}_{2}$ encode transverse or longitudinal momentum broadening of a hard parton traversing a hot medium. Understanding their temperature dependence is key to appreciating the observed suppression of high-transverse momentum probes at RHIC or LHC collision energies. We present a first continuum extrapolated result of $\hat{q}$ computed on pure SU(3) lattices with non-trivial temperature dependence different from the weak-coupling expectation. We discuss our formalism and its challenges and status in view of obtaining $\hat{e}_{2}$ or of unquenching the calculation. We consider a hard quark subject to a single scattering on the plasma. The transport coefficients are factorized in terms of matrix elements given as integrals of non-local gauge-covariant gluon field-strength field-strength correlators. After the analytic continuation to the deep-Euclidean region, the hard scale permits to recast these as a series of local, gauge-invariant operators. The renormalized leading-twist term in this expansion is closely related to static quantities, and is computed on pure SU(3) lattices ($N_{\tau}=4,~6,~8,$ and $10$) for a wide range of temperatures, ranging from 200MeV < T < 1GeV. Our estimate for the unquenched result in $2+1$-flavor QCD has very similar features.