Abstract
We consider charge transport properties of $2+1$ dimensional conformal field theories at nonzero temperature. For theories with only Abelian U(1) charges, we describe the action of particle-vortex duality on the hydrodynamic-to-collisionless crossover function: this leads to powerful functional constraints for self-dual theories. For $\mathcal{N}=8$ supersymmetric, $\mathrm{SU}(N)$ Yang-Mills theory at the conformal fixed point, exact hydrodynamic-to-collisionless crossover functions of the SO(8) R-currents can be obtained in the large $N$ limit by applying the anti-de Sitter/conformal field theory (AdS/CFT) correspondence to M theory. In the gravity theory, fluctuating currents are mapped to fluctuating gauge fields in the background of a black hole in $3+1$ dimensional anti-de Sitter space. The electromagnetic self-duality of the $3+1$ dimensional theory implies that the correlators of the R-currents obey a functional constraint similar to that found from particle-vortex duality in $2+1$ dimensional Abelian theories. Thus the $2+1$ dimensional, superconformal Yang Mills theory obeys a ``holographic self-duality'' in the large $N$ limit, and perhaps more generally.
Highlights
The quantum phase transitions of two dimensional systems have been the focus of much study in the condensed matter community
Examples are (i ) the superfluidinsulator transition in the boson Hubbard model at integer filling [9–11], which is described by the φ4 field theory with O(2) symmetry, and so is controlled by the Wilson-Fisher fixed point in D = 2+1; (ii ) the spin-gap paramagnet to Neel order transition of coupled spin dimers/ladders/layers which is described by the O(3) φ4 field theory [12, 13]; and (iii ) the ‘deconfined’ critical point of a S = 1/2 antiferromagnet between a Neel and a valence bond solid state [14, 15], which is described by the CP1 model with a non-compact U(1) gauge field [16]
In all these cases the critical point is described by a relativistic conformal field theory (CFT)
Summary
The quantum phase transitions of two (spatial) dimensional systems have been the focus of much study in the condensed matter community. More relevant is the self-dual field theory proposed recently by Motrunich and Vishwanath [16], and we discuss its charge transport properties below It was subsequently pointed out [29–31] that the Kab are not the d.c. conductivities observed at small but non-zero temperature. We have considered a similar connection at non-zero temperature for the N =8 SCFT, and shown that it is “holographically self dual” in the large N limit; combined with the non-Abelian SO(8) symmetry (which implies a single K), the constraints for the current correlators are stronger than those for Abelian theories.
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