Effects of topological and non-topological edge states on information
propagation and scrambling in a Floquet spin chain
- URL: http://arxiv.org/abs/2210.15302v2
- Date: Mon, 11 Dec 2023 10:46:21 GMT
- Title: Effects of topological and non-topological edge states on information
propagation and scrambling in a Floquet spin chain
- Authors: Samudra Sur, Diptiman Sen
- Abstract summary: We numerically study the information propagation from one end of a periodically driven spin-1/2 $XY$ chain with open boundary conditions.
For sinusoidal driving, the model can be shown to host different types of edge states.
- Score: 0.0
- License: http://creativecommons.org/licenses/by/4.0/
- Abstract: The action of any local operator on a quantum system propagates through the
system carrying the information of the operator. This is usually studied via
the out-of-time-order correlator (OTOC). We numerically study the information
propagation from one end of a periodically driven spin-1/2 $XY$ chain with open
boundary conditions using the Floquet infinite-temperature OTOC. We calculate
the OTOC for two different spin operators, $\sigma^x$ and $\sigma^z$. For
sinusoidal driving, the model can be shown to host different types of edge
states, namely, topological (Majorana) edge states and non-topological edge
states. We observe a localization of information at the edge for both
$\sigma^z$ and $\sigma^x$ OTOCs whenever edge states are present. In addition,
in the case of non-topological edge states, we see oscillations of the OTOC in
time near the edge, the oscillation period being inversely proportional to the
gap between the Floquet eigenvalues of the edge states. We provide an
analytical understanding of these effects due to the edge states. It was known
earlier that the OTOC for the spin operator which is local in terms of
Jordan-Wigner fermions ($\sigma^z$) shows no signature of information
scrambling inside the light cone of propagation, while the OTOC for the spin
operator which is non-local in terms of Jordan-Wigner fermions ($\sigma^x$)
shows signatures of scrambling. We report a remarkable `unscrambling effect' in
the $\sigma^x$ OTOC after reflections from the ends of the system. Finally, we
demonstrate that the information propagates into the system mainly via the bulk
states with the maximum value of the group velocity, and we show how this
velocity is controlled by the driving frequency and amplitude.
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