The Quantum Perfect Fluid in 2D

TL;DR

This paper develops a quantum field theory framework for 2D incompressible fluids, revealing the existence of localized vortex excitations called vortons with unique dispersion and symmetry properties.

Contribution

It introduces a novel quantum description of 2D perfect fluids using Lie group quantization, identifying vortons as fundamental excitations with specific dispersion relations.

Findings

Existence of ungapped localized vortons with quadratic dispersion

Vortons carry vorticity dipole and have symmetry-fixed derivative interactions

Continuum limit N→∞ yields robust physical quantities

Abstract

We consider the field theory that defines a perfect incompressible 2D fluid. One distinctive property of this system is that the quadratic action for fluctuations around the ground state features neither mass nor gradient term. Quantum mechanically this poses a technical puzzle, as it implies the Hilbert space of fluctuations is not a Fock space and perturbation theory is useless. As we show, the proper treatment must instead use that the configuration space is the area preserving Lie group $S\mathrm{Diff}$. Quantum mechanics on Lie groups is basically a group theory problem, but a harder one in our case, since $S\mathrm{Diff}$ is infinite dimensional. Focusing on a fluid on the 2-torus $T^2$, we could however exploit the well known result $S\mathrm{Diff}(T^2)\sim SU(N)$ for $N\to \infty$, reducing for finite $N$ to a tractable case. $SU(N)$ offers a UV-regulation, but physical quantities can be robustly defined in the continuum limit $N\to\infty$. The main result of our study is the existence of ungapped localized excitations, the vortons, satisfying a dispersion $\omega \propto k^2$ and carrying a vorticity dipole. The vortons are also characterized by very distinctive derivative interactions whose structure is fixed by symmetry. Departing from the original incompressible fluid, we constructed a class of field theories where the vortons appear, right from the start, as the quanta of either bosonic or fermionic local fields.