Abstract

Consider two quantum critical Hamiltonians HH and H~\tilde{H} on a dd-dimensional lattice that only differ in some region R\mathcal{R}. We study the relation between holographic representations, obtained through real-space renormalization, of their corresponding ground states ∣ψ⟩\left.| ψ\right\rangle and ∣ψ~⟩\left.| \tildeψ \right\rangle. We observe that, even though ∣ψ⟩\left.| ψ\right\rangle and ∣ψ~⟩\left.| \tildeψ \right\rangle disagree significantly both inside and outside region R\mathcal{R}, they still admit holographic descriptions that only differ inside the past causal cone C(R)\mathcal{C}(\mathcal{R}) of region R\mathcal{R}, where C(R)\mathcal{C}(\mathcal{R}) is obtained by coarse-graining region R\mathcal{R}. We argue that this result follows from a notion of directed influence in the renormalization group flow that is closely connected to the success of Wilson's numerical renormalization group for impurity problems. At a practical level, directed influence allows us to exploit translation invariance when describing a homogeneous system with e.g. an impurity, in spite of the fact that the Hamiltonian is no longer invariant under translations.

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