2019
DOI: 10.1016/j.ppnp.2019.04.001
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Extreme matter in electromagnetic fields and rotation

Abstract: We look over recent developments on our understanding about relativistic matter under external electromagnetic fields and mechanical rotation. I review various calculational approaches for concrete physics problems, putting my special emphasis on generality of the method and the consequence, rather than going into phenomenological applications in a specific field of physics. The topics covered in this article include static problems with magnetic fields, dynamical problems with electromagnetic fields, and phen… Show more

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Cited by 74 publications
(38 citation statements)
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References 105 publications
(189 reference statements)
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“…where we have written the result in terms of the trace of the charge matrix Q. This expression agrees with the results found in [58] for the baryon and isospin number densities of a hadronic fluid under rotation [59], which shows the existence of a vorticity coupling with the pion gradient in the absence of chiral imbalance. It is nevertheless surprising that no such effect survives in the spatial currents themselves, as it is seen from our explicit results.…”
Section: Corrections To the Leading Order Constitutive Relationssupporting
confidence: 84%
“…where we have written the result in terms of the trace of the charge matrix Q. This expression agrees with the results found in [58] for the baryon and isospin number densities of a hadronic fluid under rotation [59], which shows the existence of a vorticity coupling with the pion gradient in the absence of chiral imbalance. It is nevertheless surprising that no such effect survives in the spatial currents themselves, as it is seen from our explicit results.…”
Section: Corrections To the Leading Order Constitutive Relationssupporting
confidence: 84%
“…to consider a rotating plasma in a constant magnetic field. As it is shown in [35], the Dirac equation, in this case, has an analytical solution, that can be used to determine the corresponding Wigner function. The latter can then be used to determine the proper time dependence of the temperature and other thermodynamic quantities by carrying out the method presented in this paper.…”
Section: Discussionmentioning
confidence: 99%
“…The solutions presented in (II.34), (II. 35), and (II.36) for vanishing magnetic fields are denoted by "Bjorken", "Hubble at r = 0" and "Gubser at r = 0", respectively. The results corresponding to the solution of the energy equation with point to point varying magnetic fields are denoted by δB HI and δB LI in the high-and low-temperature approximations.…”
Section: Fig 3 (Color Online)mentioning
confidence: 99%
“…Simulations suggest that the produced magnetic field is on order of 10 18 −10 20 Gauss and linearly proportional to the collision energy [3][4][5][6]. The estimated magnetic characteristic length [7], i.e. 1/ √ eB 1 , at its peak is comparable to the typical length scale of strong interactions at low energies, namely 1/Λ QCD .…”
Section: Introductionmentioning
confidence: 90%