The free energy of the large-NN fermionic Chern−\small-Simons theory in the 'temporal' gauge

Most of the computational evidence for the Bose$\small-$Fermi duality of fundamental fields coupled to $U(N)$ Chern$\small-$Simons theories originates in the large-$N$ calculations performed in the light-cone gauge. In this paper, we use another gauge, the 'temporal' gauge, to evaluate the finite temperature partition function of $U(N)$ coupled regular and critical fermions on $\mathbb{R}^2$ at large $N$. We first set up the finite temperature gap equations, and then use tricks explored in arXiv:1410.0558 to solve these equations and evaluate the partition function. Our final results are in perfect agreement with earlier light-cone gauge results. The success of our 'temporal' gauge calculation potentially opens a path to computations that are awkward in light-cone gauge but more natural in the 'temporal' gauge, e.g. the evaluation of the thermal free energy on a finite-sized sphere.Comment: 75 page

Complexity growth and the Krylov-Wigner function

Abstract For any state in a D-dimensional Hilbert space with a choice of basis, one can define a discrete version of the Wigner function — a quasi-probability distribution which represents the state on a discrete phase space. The Wigner function can, in general, take on negative values, and the amount of negativity in the Wigner function has an operational meaning as a resource for quantum computation. In this note, we study the growth of Wigner negativity for a generic initial state under time evolution with chaotic Hamiltonians. We introduce the Krylov-Wigner function, i.e., the Wigner function defined with respect to the Krylov basis (with appropriate phases), and show that this choice of basis minimizes the early time growth of Wigner negativity in the large D limit. We take this as evidence that the Krylov basis (with appropriate phases) is ideally suited for a dual, semi-classical description of chaotic quantum dynamics at large D. We also numerically study the time evolution of the Krylov-Wigner function and its negativity in random matrix theory for an initial pure state. We observe that the negativity broadly shows three phases: it rises gradually for a time of O D $$O\left(\sqrt{D}\right)$$ , then hits a sharp ramp and finally saturates close to its upper bound of D $$\sqrt{D}$$