Abstract

We study the Fourier coefficients bk(T) of the net baryon number density in strongly interacting matter at finite temperature. We show that singularities in the complex chemical potential plane connected with phase transitions are reflected in the asymptotic behavior of the coefficients at large k. We derive the scaling properties of bk(T) near a second order phase transition in the O(4) and Z(2) universality classes. The impact of first order and crossover transitions is also examined. The scaling properties of bk(T) are linked to the QCD phase diagram in the temperature and complex chemical potential plane.

Highlights

  • h is the strength of the external symmetry-breaking field while α

  • Fourier decomposition is a useful technique for exploring characteristic features of a system

  • μ B has been discussed as a tool which connects thermodynamic quantities

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Summary

Introduction

Fourier decomposition is a useful technique for exploring characteristic features of a system. Transition, in which case the density is analytic along the integration path, there are singularities in the complex chemical potential plane, which do affect the behavior of the Fourier coefficients. First we study the Fourier expansion of the net baryon density in the Landau theory of the phase transitions, in order to illustrate in a transparent framework how critical singularities in the complex chemical potential plane are reflected in the Fourier coefficients. For physical quark masses, the O (4) chiral transition is of the crossover type In this case the critical singularities are located in the complex μ B plane and the k dependence of the Fourier coefficients bk(T ) corresponds to damped oscillations superimposed on a power-law dependence. The damping rate is determined by the real and the oscillation frequency by the imaginary part of the baryon chemical potential at the crossover branch point singularity.

Critical singularities in the complex μB plane
Landau theory
Scaling theory
Asymptotics of Fourier coefficients
First order transition at imaginary μB
Second order transition
Crossover
Conclusion

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