Negative Barnett effect, negative moment of inertia of the gluon plasma, and thermal evaporation of the chromomagnetic condensate

We discuss the negativity of the moment of inertia of (quark-)gluon plasma in a window of “supervortical” range of temperatures above the deconfining phase transition, T ≃ ( 1 … 1.5 ) T c , found recently in numerical Monte Carlo simulations by two independent methods. In our work, we confirm numeri...

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Published in:Physical review. D 2024-07, Vol.110 (1), Article 014511
Main Authors: Braguta, Victor V., Chernodub, Maxim N., Kudrov, Ilya E., Roenko, Artem A., Sychev, Dmitrii A.
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High Energy Physics - Phenomenology
High Energy Physics - Theory
Physics
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container_title Physical review. D
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Kudrov, Ilya E.
Roenko, Artem A.
Sychev, Dmitrii A.
description We discuss the negativity of the moment of inertia of (quark-)gluon plasma in a window of “supervortical” range of temperatures above the deconfining phase transition, T ≃ ( 1 … 1.5 ) T c , found recently in numerical Monte Carlo simulations by two independent methods. In our work, we confirm numerically that the origin of this effect is rooted in the thermal evaporation of the nonperturbative chromomagnetic condensate. We argue that the negative moment of inertia of gluon plasma indicates the presence of a novel effect, the negative spin-vortical coupling for gluons resulting in a negative gluonic Barnett effect: the spin polarization of gluons exceeds the total angular momentum of rotating plasma, thus forcing the orbital angular momentum to take negative values in the supervortical range of temperatures.
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title Negative Barnett effect, negative moment of inertia of the gluon plasma, and thermal evaporation of the chromomagnetic condensate
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