Hierarchy of linear light cones with long-range interactions
- URL: http://arxiv.org/abs/2001.11509v4
- Date: Mon, 18 Jul 2022 14:18:12 GMT
- Title: Hierarchy of linear light cones with long-range interactions
- Authors: Minh C. Tran, Chi-Fang Chen, Adam Ehrenberg, Andrew Y. Guo, Abhinav
Deshpande, Yifan Hong, Zhe-Xuan Gong, Alexey V. Gorshkov, Andrew Lucas
- Abstract summary: In quantum many-body systems, quantum information and entanglement cannot spread outside of a linear light cone.
In one spatial dimension, this linear light cone exists for every many-body state when $alpha>3$ (Lieb-Robinson light cone)
We show that universal quantum state transfer, as well as many-body quantum chaos, are bounded by the Frobenius light cone.
- Score: 0.4643589635376552
- License: http://arxiv.org/licenses/nonexclusive-distrib/1.0/
- Abstract: In quantum many-body systems with local interactions, quantum information and
entanglement cannot spread outside of a linear light cone, which expands at an
emergent velocity analogous to the speed of light. Local operations at
sufficiently separated spacetime points approximately commute -- given a
many-body state, $\mathcal{O}_x(t) \mathcal{O}_y |\psi\rangle \approx
\mathcal{O}_y\mathcal{O}_x(t) |\psi\rangle$ with arbitrarily small errors -- so
long as $|x-y|\gtrsim vt$, where $v$ is finite. Yet most non-relativistic
physical systems realized in nature have long-range interactions: two degrees
of freedom separated by a distance $r$ interact with potential energy $V(r)
\propto 1/r^{\alpha}$. In systems with long-range interactions, we rigorously
establish a hierarchy of linear light cones: at the same $\alpha$, some quantum
information processing tasks are constrained by a linear light cone while
others are not. In one spatial dimension, this linear light cone exists for
every many-body state when $\alpha>3$ (Lieb-Robinson light cone); for a typical
state chosen uniformly at random from the Hilbert space when
$\alpha>\frac{5}{2}$ (Frobenius light cone); for every state of a
non-interacting system when $\alpha>2$ (free light cone). These bounds apply to
time-dependent systems and are optimal up to subalgebraic improvements. Our
theorems regarding the Lieb-Robinson and free light cones -- and their
tightness -- also generalize to arbitrary dimensions. We discuss the
implications of our bounds on the growth of connected correlators and of
topological order, the clustering of correlations in gapped systems, and the
digital simulation of systems with long-range interactions. In addition, we
show that universal quantum state transfer, as well as many-body quantum chaos,
are bounded by the Frobenius light cone, and therefore are poorly constrained
by all Lieb-Robinson bounds.
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