Noncommutative fluid dynamics in the K\"{a}hler parametrization

TL;DR

This paper develops a noncommutative fluid model using Kähler parametrization, deriving equations of motion, energy-momentum tensor, and constraints, revealing dissipative effects absent in commutative fluids and connecting to topological invariants.

Contribution

It introduces a first order action for noncommutative fluids in Kähler parametrization, extending relativistic perfect fluids to noncommutative spacetimes with new constraints and conserved quantities.

Findings

Energy-momentum tensor includes noncommutative dissipative term

Density current remains conserved without noncommutative corrections

Model exhibits infinitely many conserved currents and topological invariants

Abstract

In this paper, we propose a first order action functional for a large class of systems that generalize the relativistic perfect fluids in the K\"{a}hler parametrization to noncommutative spacetimes. We calculate the equations of motion for the fluid potentials and the energy-momentum tensor in the first order in the noncommutative parameter. The density current does not receive any noncommutative corrections and it is conserved under the action of the commutative generators $P_{\mu}$ but the energy-momentum tensor is not. Therefore, we determine the set of constraints under which the energy-momentum tensor is divergenceless. Another set of constraints on the fluid potentials is obtained from the requirement of the invariance of the action under the generalization of the volume preserving transformations of the noncommutative spacetime. We show that the proposed action describes noncommutative fluid models by casting the energy-momentum tensor in the familiar fluid form and identifying the corresponding energy and momentum densities. In the commutative limit, they are identical to the corresponding quantities of the relativistic perfect fluids. The energy-momentum tensor contains a dissipative term that is due to the noncommutative spacetime and vanishes in the commutative limit. Finally, we particularize the theory to the case when the complex fluid potentials are characterized by a function $K(z,\bar{z})$ that is a deformation of the complex plane and show that this model has important common features with the commutative fluid such as infinitely many conserved currents and a conserved axial current that in the commutative case is associated to the topologically conserved linking number.