Heavy quark momentum diffusion coefficient from lattice QCD

Debasish Banerjee, Saumen Datta, Rajiv Gavai, and Pushan Majumdar
Phys. Rev. D 85, 014510 – Published 31 January 2012

Abstract

The momentum diffusion coefficient for heavy quarks is studied in a deconfined gluon plasma in the static approximation by investigating a correlation function of the color electric field using Monte Carlo techniques. The diffusion coefficient is extracted from the long-distance behavior of such a correlator. For temperatures Tc<T2Tc, our nonperturbative estimate of the diffusion coefficient is found to be very different from the leading-order perturbation theory and is in the right ballpark to explain the heavy quark flow seen by the PHENIX Collaboration at the RHIC experiment.

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  • Received 13 October 2011

DOI:https://doi.org/10.1103/PhysRevD.85.014510

© 2012 American Physical Society

Authors & Affiliations

Debasish Banerjee*, Saumen Datta, and Rajiv Gavai

  • Department of Theoretical Physics, Tata Institute of Fundamental Research, Homi Bhabha Road, Mumbai 400005, India

Pushan Majumdar§

  • Department of Theoretical Physics, Indian Association for the Cultivation of Science, Kolkata 700032, India

  • *debasish@theory.tifr.res.in
  • saumen@theory.tifr.res.in
  • gavai@tifr.res.in
  • §tppm@iacs.res.in

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Vol. 85, Iss. 1 — 1 January 2012

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