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The Chiral Magnetic Effect and an experimental bound on the late time magnetic field strength
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abstract
We first compare different approaches to estimates of the magnitude of the chiral magnetic effect in relativistic heavy ion collisions and show that their main difference lies in the assumptions on the length of persistence of the magnetic field generated by the colliding nuclei. We then analyze recent measurements of the global polarization of $\Lambda$ and $\bar \Lambda$ hyperons in terms of the bounds they set on the magnitude of the late time magnetic field.
Forward citations
Cited by 2 Pith papers
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Hyperon global polarization in isobar Ru+Ru and Zr+Zr collisions at $\sqrt{s_{NN}}$ = 200 GeV
In Ru+Ru and Zr+Zr collisions at 200 GeV, STAR finds Lambda polarization growing toward peripheral collisions, a first 2.4-sigma hint of in-plane-enhanced polarization, and a 2.9-sigma positive Xi polarization.
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Global polarization of $\Lambda$, $\Xi^{-}$, and $\Omega^{-}$ hyperons in Au+Au collisions at RHIC BES-II energies
Hydrodynamic calculations show Omega hyperon polarization exceeds that of Lambda and Xi due to spin but falls below STAR data, with particle-antiparticle splitting growing at lower energies and driven by chemical pote...
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