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Quarkonium propagation in the quark–gluon plasma

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Abstract

In relativistic heavy ion collisions at RHIC and the LHC, a quark–gluon plasma (QGP) is created for a short duration of about 10 fm/c. Quarkonia (bound states of \(c\bar{c}\) and \(b\bar{b}\)) are sensitive probes of this phase on length scales comparable to the size of the bound states which are less than 1 fm. Observations of quarkonia in these collisions provide us with a lot of information about how the presence of a QGP affects various quarkonium states. This has motivated the development of the theory of heavy quarks and their bound states in a thermal medium, and its application to the phenomenology of quarkonia in heavy ion collisions. We review some of these developments here.

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Notes

  1. Within the ambit of final state interactions there is another effect that can be included. The color octet state \(Q\bar{Q}\) undergoes energy loss before giving rise to the initial mesonic state. This effect was included in Ref. [61].

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Acknowledgements

We acknowledge collaborators on various projects related to heavy quark and quarkonium physics, Samuel Aronson, Evan Borras, Sourendu Gupta, Brian Odegard, Anurag Tiwari, Ivan Vitev, and Ben-Wei Zhang. We also thank Dibyendu Bala, Saumen Datta for several illuminating discussions. We also acknowledge discussions and exchanges with Yukiano Akamatsu, Jean-Paul Blaizot, Nora Brambilla, Alexander Rothkopf, and Peter Petreczky.

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    Rishi Sharma

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Sharma, R. Quarkonium propagation in the quark–gluon plasma. Eur. Phys. J. Spec. Top. 230, 697–718 (2021). https://doi.org/10.1140/epjs/s11734-021-00025-z

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