# Percolation thresholds for photonic quantum computing

## TL;DR

This paper establishes fundamental limits and practical methods for creating percolated photonic cluster states for quantum computing, demonstrating that 3-photon microclusters can form renormalizable clusters without feedforward.

## Contribution

It proves a lower bound on success probability for fusion operations, formulates the problem as a percolation threshold, and constructs explicit 3-photon microcluster schemes without feedforward.

## Key findings

- Proves that the success probability must satisfy /(n-1) for renormalization.
- Shows 3-photon microclusters can form percolated clusters without feedforward.
- Improves bounds on the percolation threshold for 3-photon microclusters.

## Abstract

Any quantum algorithm can be implemented by an adaptive sequence of single node measurements on an entangled cluster of qubits in a square lattice topology. Photons are a promising candidate for encoding qubits but assembling a photonic entangled cluster with linear optical elements relies on probabilistic operations. Given a supply of $n$-photon-entangled microclusters, using a linear optical circuit and photon detectors, one can assemble a random entangled state of photons that can be subsequently "renormalized" into a logical cluster for universal quantum computing. In this paper, we prove that there is a fundamental tradeoff between $n$ and the minimum success probability $\lambda_c^{(n)}$ that each two-photon linear-optical fusion operation must have, in order to guarantee that the resulting state can be renormalized: $\lambda_c^{(n)} \ge 1/(n-1)$. We present a new way of formulating this problem where $\lambda_c^{(n)}$ is the bond percolation threshold of a logical graph and provide explicit constructions to produce a percolated cluster using $n=3$ photon microclusters (GHZ states) as the initial resource. We settle a heretofore open question by showing that a renormalizable cluster can be created with $3$-photon microclusters over a 2D graph without feedforward, which makes the scheme extremely attractive for an integrated-photonic realization. We also provide lattice constructions, which show that $0.5 \le \lambda_c^{(3)} \le 0.5898$, improving on a recent result of $\lambda_c^{(3)} \le 0.625$. Finally, we discuss how losses affect the bounds on the threshold, using loss models inspired by a recently-proposed method to produce photonic microclusters using quantum dot emitters.