Factory-based Fault-tolerant Preparation of Quantum Polar Codes Encoding One logical Qubit
A fault-tolerant way to prepare logical code-states of Q1 codes, i.e., quantum polar codes encoding one qubit, has been recently proposed. The fault tolerance therein is guaranteed by an error detection gadget, where if an error is detected during the preparation, one discards entirely the preparati...
Gespeichert in:
Hauptverfasser: | , , |
---|---|
Format: | Artikel |
Sprache: | eng |
Schlagworte: | |
Online-Zugang: | Volltext bestellen |
Tags: |
Tag hinzufügen
Keine Tags, Fügen Sie den ersten Tag hinzu!
|
Zusammenfassung: | A fault-tolerant way to prepare logical code-states of Q1 codes, i.e.,
quantum polar codes encoding one qubit, has been recently proposed. The fault
tolerance therein is guaranteed by an error detection gadget, where if an error
is detected during the preparation, one discards entirely the preparation. Due
to error detection, the preparation is probabilistic, and its success rate,
referred to as the preparation rate, decreases rapidly with the code-length,
preventing the preparation of code-states of large code-lengths. In this paper,
to improve the preparation rate, we consider a factory preparation of Q1
code-states, where one attempts to prepare several copies of Q1 code-states in
parallel. Using an extra scheduling step, we can avoid discarding the
preparation entirely, every time an error is detected, hence, achieving an
increased preparation rate in turn. We further provide a theoretical method to
estimate preparation and logical error rates of Q1 codes, prepared using
factory preparation, which is shown to tightly fit the Monte-Carlo simulation
based numerical results. Therefore, our theoretical method is useful for
providing estimates for large code-lengths, where Monte-Carlo simulations are
practically not feasible. Our numerical results, for a circuit-level
depolarizing noise model, indicate that the preparation rate increases
significantly, especially for large code-length N. For example, for N = 256, it
increases from 0.02\% to 27\% for a practically interesting physical error rate
of p = 10^{-3}. Remarkably, a Q1 code with N = 256 achieves logical error rates
around 10^{-11} and 10^{-15} for p = 10^{-3} and p = 3 x 10^{-4}, respectively.
This corresponds to an improvement of about three orders of magnitude compared
to a surface code with similar code-length and minimum distance, thus showing
the promise of the proposed scheme for large-scale fault-tolerant quantum
computing. |
---|---|
DOI: | 10.48550/arxiv.2307.15226 |