PyMatching 2.0.dev0

A package for decoding quantum error correcting codes using minimum-weight perfect matching.

PyMatching 2.0

PyMatching is a fast Python/C++ library for decoding quantum error correcting (QEC) codes using the Minimum Weight Perfect Matching (MWPM) decoder. Given the syndrome measurements from a quantum error correction circuit, the MWPM decoder finds the most probable set of errors, given the assumption that error mechanisms are independent, as well as graphlike (each error causes either one or two detection events). The MWPM decoder is the most popular decoder for decoding surface codes, and can also be used to decode various other code families, including subsystem codes, honeycomb codes and 2D hyperbolic codes.

Version 2.0 includes a new implementation of the blossom algorithm which is 100-1000x faster than previous versions of PyMatching. PyMatching can be configured using arbitrary weighted graphs, with or without a boundary, and can be combined with Craig Gidney's Stim library to simulate and decode error correction circuits in the presence of circuit-level noise. The sinter package combines Stim and PyMatching to perform fast, parallelised monte-carlo sampling of quantum error correction circuits.

Documentation for PyMatching can be found at: pymatching.readthedocs.io

To see how stim, sinter and pymatching can be used to estimate the threshold of an error correcting code with circuit-level noise, try out the stim getting started notebook.

The new >100x faster implementation for Version 2.0

Version 2.0 features a new implementation of the blossom algorithm, which I wrote with Craig Gidney. Our new implementation, which we refer to as the sparse blossom algorithm, can be seen as a generalisation of the blossom algorithm to handle the decoding problem relevant to QEC. We solve the problem of finding minimum-weight paths between detection events in a detector graph directly, which avoids the need to use costly all-to-all Dijkstra searches to find a MWPM in a derived graph using the original blossom algorithm. The new version is also exact - unlike previous versions of PyMatching, no approximation is made.

Our new implementation is over 100x faster than previous versions of PyMatching, and is over 100,000x faster than NetworkX (benchmarked with surface code circuits). At 0.1% circuit-noise, PyMatching v2.0 can decode a distance 19 surface code in less than 1 microsecond per measurement round, and the runtime is approximately linear in the size of the graph.

The benchmarks in the two plots below (run on an M1 chip) compare the performance of PyMatching v2.0 with the previous version (v0.7) as well as with NetworkX for decoding surface code circuits with circuit-level depolarising noise. The equations T=N^x in the legends (and plotted as dashed lines) are obtained from a fit to the same dataset for distance > 10, where N is the number of detectors (nodes) per round, and T is the decoding time per round.

Decoding time per round for p=0.1% circuit-level noise	Decoding time per round for p=0.5% circuit-level noise

Sparse blossom is conceptually similar to the approach described in this paper by Austin Fowler, although our approach differs in many of the details (which will be explained in our upcoming paper). There are even more similarities with the very nice independent work by Yue Wu, who recently released the fusion-blossom library. One of the differences with our approach is that fusion-blossom grows the exploratory regions of alternating trees in a similar way to how clusters are grown in Union-Find, whereas our approach instead progresses along a timeline, and uses a global priority queue to grow alternating trees. Yue also has a paper coming soon, so stay tuned for that as well.

Installation

The latest version of PyMatching can be downloaded and installed from PyPI with the command:

pip install pymatching --upgrade

Usage

PyMatching can load matching graphs from a check matrix, a stim.DetectorErrorModel, a networkx.Graph, a retworkx.PyGraph or by adding edges individually with pymatching.Matching.add_edge and pymatching.Matching.add_boundary_edge.

Decoding Stim circuits

PyMatching can be combined with Stim. Generally, the easiest and fastest way to do this is using sinter (use v1.10.0 or later), which uses PyMatching and Stim to run parallelised monte carlo simulations of quantum error correction circuits. However, in this section we will use Stim and PyMatching directly, to demonstrate how their Python APIs can be used. To install stim, run pip install stim --upgrade.

First, we generate a stim circuit. Here, we use a surface code circuit included with stim:

import numpy as np
import stim
import pymatching
circuit = stim.Circuit.generated("surface_code:rotated_memory_x", 
                                 distance=5, 
                                 rounds=5, 
                                 after_clifford_depolarization=0.005)

Next, we use stim to generate a stim.DetectorErrorModel (DEM), which is effectively a Tanner graph describing the circuit-level noise model. By setting decompose_errors=True, stim decomposes all error mechanisms into edge-like error mechanisms (which cause either one or two detection events). This ensures that our DEM is graphlike, and can be loaded by pymatching:

model = circuit.detector_error_model(decompose_errors=True)
matching = pymatching.Matching.from_detector_error_model(model)

Next, we will sample 1000 shots from the circuit. Each shot (a row of shots) contains the full syndrome (detector measurements), as well as the logical observable measurements, from simulating the noisy circuit:

sampler = circuit.compile_detector_sampler()
syndrome, actual_observables = sampler.sample(shots=1000, separate_observables=True)

Now we can decode! We compare PyMatching's predictions of the logical observables with the actual observables sampled with stim, in order to count the number of mistakes and estimate the logical error rate:

num_errors = 0
for i in range(syndrome.shape[0]):
    predicted_observables = matching.decode(syndrome[i,:])
    num_errors += not np.array_equal(actual_observables[i,:], predicted_observables)

print(num_errors)  # prints 8

Loading from a parity check matrix

We can also load a pymatching.Matching object from a binary parity check matrix, another representation of a Tanner graph. Each row in the parity check matrix H corresponds to a parity check, and each column corresponds to an error mechanism. The element H[i,j] of H is 1 if parity check i is flipped by error mechanism j, and 0 otherwise. To be used by PyMatching, the error mechanisms in H must be graphlike. This means that each column must contain either one or two 1s (if a column has a single 1, it represents a half-edge connected to the boundary).

We can give each edge in the graph a weight, by providing PyMatching with a weights numpy array. Element weights[j] of the weights array sets the edge weight for the edge corresponding to column j of H. If the error mechanisms are treated as independent, then we typically want to set the weight of edge j to the log-likelihood ratio log((1-p_j)/p_j), where p_j is the error probability associated with edge j. With this setting, PyMatching will find the most probable set of error mechanisms, given the syndrome.

With PyMatching configured using H and weights, decoding a binary syndrome vector syndrome (a numpy array of length H.shape[0]) corresponds to finding a set of errors defined in a binary predictions vector satisfying H@predictions % 2 == syndrome while minimising the total solution weight predictions@weights.

In quantum error correction, rather than predicting which exact set of error mechanisms occurred, we typically want to predict the outcome of logical observable measurements, which are the parities of error mechanisms. These can be represented by a binary matrix observables. Similar to the check matrix, observables[i,j] is 1 if logical observable i is flipped by error mechanism j. For example, suppose our syndrome syndrome, was the result of a set of errors noise (a binary array of length H.shape[1]), such that syndrome = H@noise % 2. Our decoding is successful if observables@noise % 2 == observables@predictions % 2.

Putting this together, we can decode a distance 5 repetition code as follows:

import numpy as np
from scipy.sparse import csc_matrix
import pymatching
H = csc_matrix([[1, 1, 0, 0, 0],
                 [0, 1, 1, 0, 0],
                 [0, 0, 1, 1, 0],
                 [0, 0, 0, 1, 1]])
weights = np.array([4, 3, 2, 3, 4])   # Set arbitrary weights for illustration
matching = pymatching.Matching(H, weights=weights)
prediction = matching.decode(np.array([0, 1, 0, 1]))
print(prediction)  # prints: [0 0 1 1 0]
# Optionally, we can return the weight as well:
prediction, solution_weight = matching.decode(np.array([0, 1, 0, 1]), return_weight=True)
print(prediction)  # prints: [0 0 1 1 0]
print(solution_weight)  # prints: 5.0

And in order to estimate the logical error rate for a physical error rate of 10%, we can sample as follows:

import numpy as np
from scipy.sparse import csc_matrix
import pymatching
H = csc_matrix([[1, 1, 0, 0, 0],
                [0, 1, 1, 0, 0],
                [0, 0, 1, 1, 0],
                [0, 0, 0, 1, 1]])
observables = csc_matrix([[1, 0, 0, 0, 0]])
error_probability = 0.1
weights = np.ones(H.shape[1]) * np.log((1-error_probability)/error_probability)
matching = pymatching.Matching.from_check_matrix(H, weights=weights)
num_errors = 0
for i in range(1000):
    noise = (np.random.random(H.shape[1]) < error_probability).astype(np.uint8)
    syndrome = H@noise % 2
    prediction = matching.decode(syndrome)
    predicted_observables = observables@prediction % 2
    actual_observables = observables@noise % 2
    num_errors += not np.array_equal(predicted_observables, actual_observables)
print(num_errors)  # prints 4

Note that we can also ask PyMatching to estimate the logical observables directly, by supplying them to the faults_matrix argument when constructing the pymatching.Matching object. This allows the decoder to make some additional optimisations, that speed up the decoding procedure a bit. The following example uses this approach, and is equivalent to the example above:

import numpy as np
from scipy.sparse import csc_matrix
import pymatching

H = csc_matrix([[1, 1, 0, 0, 0],
                [0, 1, 1, 0, 0],
                [0, 0, 1, 1, 0],
                [0, 0, 0, 1, 1]])
observables = csc_matrix([[1, 0, 0, 0, 0]])
error_probability = 0.1
weights = np.ones(H.shape[1]) * np.log((1-error_probability)/error_probability)
matching = pymatching.Matching.from_check_matrix(H, weights=weights, faults_matrix=observables)
num_errors = 0
for i in range(1000):
    noise = (np.random.random(H.shape[1]) < error_probability).astype(np.uint8)
    syndrome = H@noise % 2
    predicted_observables = matching.decode(syndrome)
    actual_observables = observables@noise % 2
    num_errors += not np.array_equal(predicted_observables, actual_observables)

print(num_errors)  # prints 6

Instead of using a check matrix, the Matching object can also be constructed using the Matching.add_edge and Matching.add_boundary_edge methods, or by loading from a NetworkX or retworkx graph.

For more details on how to use PyMatching, see the documentation.

Attribution

A paper on our new implementation used in PyMatching version 2.0 (sparse blossom) will be published soon. In the meantime, please cite:

@misc{pymatchingv2,
  author = {Higgott, Oscar and Gidney, Craig},
  title = {PyMatching v2},
  year = {2022},
  publisher = {GitHub},
  journal = {GitHub repository},
  howpublished = {\url{https://github.com/oscarhiggott/PyMatching}}
}

Note: the existing PyMatching paper descibes the implementation in version 0.7 and earlier of PyMatching (not v2.0).

Acknowledgements

We are grateful to the Google Quantum AI team for supporting the development of PyMatching v2.0. Earlier versions of PyMatching were supported by Unitary Fund and EPSRC.