Mixing and localisation in random time-periodic quantum circuits of
Clifford unitaries
- URL: http://arxiv.org/abs/2007.03339v4
- Date: Mon, 17 Jan 2022 16:44:22 GMT
- Title: Mixing and localisation in random time-periodic quantum circuits of
Clifford unitaries
- Authors: Tom Farshi, Daniele Toniolo, Carlos E. Gonz\'alez-Guill\'en, \'Alvaro
M. Alhambra, Lluis Masanes
- Abstract summary: We analyse a Floquet model with disorder, characterised by a family of local, time-periodic, random quantum circuits in one spatial dimension.
We prove that the evolution operator cannot be distinguished from a (Haar) random unitary when all qubits are measured with Pauli operators.
In the opposite regime our system displays a novel form of localisation, produced by the appearance of effective one-sided walls.
- Score: 0.0
- License: http://arxiv.org/licenses/nonexclusive-distrib/1.0/
- Abstract: How much does local and time-periodic dynamics resemble a random unitary? In
the present work we address this question by using the Clifford formalism from
quantum computation. We analyse a Floquet model with disorder, characterised by
a family of local, time-periodic, random quantum circuits in one spatial
dimension. We observe that the evolution operator enjoys an extra symmetry at
times that are a half-integer multiple of the period. With this we prove that
after the scrambling time, namely when any initial perturbation has propagated
throughout the system, the evolution operator cannot be distinguished from a
(Haar) random unitary when all qubits are measured with Pauli operators. This
indistinguishability decreases as time goes on, which is in high contrast to
the more studied case of (time-dependent) random circuits. We also prove that
the evolution of Pauli operators displays a form of mixing. These results
require the dimension of the local subsystem to be large. In the opposite
regime our system displays a novel form of localisation, produced by the
appearance of effective one-sided walls, which prevent perturbations from
crossing the wall in one direction but not the other.
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