Abstract

In the previous Quarks 2016 conference I have presented a concise review of description of quark-gluon plasma (QGP) formation in heavy-ion collisions (HIC) within the holographic approach. In particular, I have discussed how to get the total multiplicity and time formation of QGP in HIC that fit the recent experimental data. For this purpose we had to use an anisotropic holographic model. There are also experimental indications that QGP formed in HIC is anisotropic. In this talk I discuss static properties of anisotropic QGP, in particular, phase transition and diffusion coefficients.

Highlights

  • It is my pleasure to give a talk in the Quarks 2018 Conference

  • The subject of my talk is the same as in the previous Quarks 2016 Conference, it is about the holography description of quark-gluon plasma (QGP) formed in heavy-ion collisions (HIC) [1]

  • There are experimental indications that QGP formed in HIC is anisotropic [4]

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Summary

Introduction

It is my pleasure to give a talk in the Quarks 2018 Conference. I would like to thank the organizers for the invitation. The subject of my talk is the same as in the previous Quarks 2016 Conference, it is about the holography description of quark-gluon plasma (QGP) formed in heavy-ion collisions (HIC) [1]. There are experimental indications that QGP formed in HIC is anisotropic [4]. In this talk I mainly discuss static properties of anisotropic QGP formed in HIC. I just would like to mention that I’ll use the so-called the bottom-up holographic approach. In this approach we choose a 5-dim gravity to get phenomenologically acceptable theory on the 4-dimensional boundary

Holographic setup
Spatial Wilson loops and drag forces
Spatial WLxY
Spatial WLyY
Conclusion
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