Wei-Ting Kuo, Daniel Arovas, Smitha Vishveshwara, and Yi-Zhuang You
SciPost Phys. 11, 084 (2021) ·
published 28 October 2021
|
· pdf
We present a formulation for investigating quench dynamics across quantum phase transitions in the presence of decoherence. We formulate decoherent dynamics induced by continuous quantum non-demolition measurements of the instantaneous Hamiltonian. We generalize the well-studied universal Kibble-Zurek behavior for linear temporal drive across the critical point. We identify a strong decoherence regime wherein the decoherence time is shorter than the standard correlation time, which varies as the inverse gap above the groundstate. In this regime, we find that the freeze-out time $\bar{t}\sim\tau^{{2\nu z}/({1+2\nu z})}$ for when the system falls out of equilibrium and the associated freeze-out length $\bar{\xi}\sim\tau^{\nu/({1+2\nu z})}$ show power-law scaling with respect to the quench rate $1/\tau$, where the exponents depend on the correlation length exponent $\nu$ and the dynamical exponent $z$ associated with the transition. The universal exponents differ from those of standard Kibble-Zurek scaling. We explicitly demonstrate this scaling behavior in the instance of a topological transition in a Chern insulator system. We show that the freeze-out time scale can be probed from the relaxation of the Hall conductivity. Furthermore, on introducing disorder to break translational invariance, we demonstrate how quenching results in regions of imbalanced excitation density characterized by an emergent length scale which also shows universal scaling. We perform numerical simulations to confirm our analytical predictions and corroborate the scaling arguments that we postulate as universal to a host of systems.
SciPost Phys. 8, 061 (2020) ·
published 17 April 2020
|
· pdf
Magnetotransport theory of layered superconductors in the flux flow steady
state is revisited. Longstanding controversies concerning observed Hall sign
reversals are resolved. The conductivity separates into a Bardeen-Stephen
vortex core contribution, and a Hall conductivity due to moving vortex charge.
This charge, which is responsible for Hall anomaly, diverges logarithmically at
weak magnetic field. Its values can be extracted from magetoresistivity data by
extrapolation of vortex core Hall angle from the normal phase. Hall anomalies
in YBCO, BSCCO, and NCCO data are consistent with theoretical estimates based
on doping dependence of London penetration depths. In the appendices, we derive
the Streda formula for the hydrodynamical Hall conductivity, and refute
previously assumed relevance of Galilean symmetry to Hall anomalies.
