# Renato Critelli - Sao Paulo University

## Contact Details

NameRenato Critelli |
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AffiliationSao Paulo University |
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CityGuarulhos |
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CountryBrazil |
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## Pubs By Year |
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## Pub CategoriesNuclear Theory (7) High Energy Physics - Theory (7) High Energy Physics - Phenomenology (6) High Energy Physics - Lattice (2) Nuclear Experiment (1) General Relativity and Quantum Cosmology (1) |

## Publications Authored By Renato Critelli

**Authors:**Romulo Rougemont

^{1}, Renato Critelli

^{2}, Jacquelyn Noronha-Hostler

^{3}, Jorge Noronha

^{4}, Claudia Ratti

^{5}

**Affiliations:**

^{1}IIP, Brazil,

^{2}Sao Paulo U.,

^{3}Houston U.,

^{4}Sao Paulo U.,

^{5}Houston U.

We employ an Einstein-Maxwell-Dilaton (EMD) holographic model, which is known to be in good agreement with lattice results for the QCD equation of state with $(2+1)$ flavors and physical quark masses, to investigate the temperature and baryon chemical potential dependence of the susceptibilities, conductivities, and diffusion coefficients associated with baryon, electric, and strangeness conserved charges. We also determine how the bulk and shear viscosities of the plasma vary with increasing baryon density. The diffusion of conserved charges and the hydrodynamic viscosities in a baryon rich quark-gluon plasma are found to be suppressed with respect to the zero net baryon case. Read More

This manuscript reviews recent theoretical progress on the understanding of the quark gluon plasma in a magnetic field that I presented on the conference Hot Quarks 2016, held at South Padre Island, Texas, USA, 12-17 September 2016. It is shown that, using a holographic bottom-up Einstein-Maxwell-Dilaton model, one can have a good quantitative agreement with Lattice data for QCD equation of state and Polyakov loop with nonzero magnetic field. I also present results for the anisotropic shear viscosity ratio $\eta_{\parallel}/\eta_{\perp}$, with the conclusion that $\eta_{\parallel}<\eta_{\perp}$ for $B>0$. Read More

**Authors:**Stefano I. Finazzo

^{1}, Romulo Rougemont

^{2}, Maicon Zaniboni

^{3}, Renato Critelli

^{4}, Jorge Noronha

^{5}

**Affiliations:**

^{1}Sao Paulo, IFT,

^{2}Sao Paulo U.,

^{3}Sao Paulo U.,

^{4}Sao Paulo U.,

^{5}Sao Paulo U.

We study the behavior of quasinormal modes in a top-down holographic dual corresponding to a strongly coupled $\mathcal{N} = 4$ super Yang-Mills plasma charged under a $U(1)$ subgroup of the global $SU(4)$ R-symmetry. In particular, we analyze the spectra of quasinormal modes in the external scalar and vector diffusion channels near the critical point and obtain the behavior of the characteristic equilibration times of the plasma as the system evolves towards the critical point of its phase diagram. Except close to the critical point, we observe that by increasing the chemical potential one generally increases the damping rate of the quasinormal modes, which leads to a reduction of the characteristic equilibration times in the dual strongly coupled plasma. Read More

In this dissertation we use the gauge/gravity duality approach to study the dynamics of strongly coupled non-Abelian plasmas. Ultimately, we want to understand the properties of the quark-gluon plasma (QGP), whose scientifc interest by the scientific community escalated exponentially after its discovery in the 2000's through the collision of ultrarelativistic heavy ions. One can enrich the dynamics of the QGP by adding an external field, such as the baryon chemical potential (needed to study the QCD phase diagram), or a magnetic field. Read More

**Affiliations:**

^{1}Sao Paulo U.,

^{2}Sao Paulo U.,

^{3}Sao Paulo, IFT,

^{4}Sao Paulo U.

We investigate the temperature and magnetic field dependence of the Polyakov loop and heavy quark entropy in a bottom-up Einstein-Maxwell-dilaton (EMD) holographic model for the strongly coupled quark-gluon plasma (QGP) that quantitatively matches lattice data for the $(2+1)$-flavor QCD equation of state at finite magnetic field and physical quark masses. We compare the holographic EMD model results for the Polyakov loop at zero and nonzero magnetic fields and the heavy quark entropy at vanishing magnetic field with the latest lattice data available for these observables and find good agreement for temperatures $T\gtrsim 150$ MeV and magnetic fields $eB\lesssim 1$ GeV$^2$. Predictions for the behavior of the heavy quark entropy at nonzero magnetic fields are made that could be readily tested on the lattice. Read More

**Affiliations:**

^{1}Sao Paulo, IFT,

^{2}Sao Paulo U.,

^{3}Sao Paulo U.,

^{4}Sao Paulo U.

We present a holographic perspective on momentum transport in strongly coupled, anisotropic non-Abelian plasmas in the presence of strong magnetic fields. We compute the anisotropic heavy quark drag forces and Langevin diffusion coefficients and also the anisotropic shear viscosities for two different holographic models, namely, a top-down deformation of strongly coupled $\mathcal{N} = 4$ Super-Yang-Mills (SYM) theory triggered by an external Abelian magnetic field, and a bottom-up Einstein-Maxwell-dilaton (EMD) model which is able to provide a quantitative description of lattice QCD thermodynamics with $(2+1)$-flavors at both zero and nonzero magnetic fields. We find that, in general, energy loss and momentum diffusion through strongly coupled anisotropic plasmas are enhanced by a magnetic field being larger in transverse directions than in the direction parallel to the magnetic field. Read More

**Affiliations:**

^{1}Sao Paulo U.,

^{2}Sao Paulo U.,

^{3}Sao Paulo U. and Columbia U.

Lattice data for the QCD equation of state and the magnetic susceptibility computed near the crossover transition at zero magnetic field are used to determine the input parameters of a five dimensional Einstein-Maxwell-Dilaton holographic model. Once the model parameters are fixed at zero magnetic field, one can use this holographic construction to study the effects of a magnetic field on the equilibrium and transport properties of the quark-gluon plasma. In this paper we use this model to study the dependence of the crossover temperature with an external magnetic field. Read More