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Transforms stabilizer state into graph state

Project description

StabGraph

Every stabilizer state can be transformed into a graph state by means of a local Clifford unitary. stabgraph provides a single public function, convert, that takes a stabilizer description of an n-qubit stabilizer state and returns a graph-state representation together with the local Clifford bookkeeping needed to recover the original state.

The package is useful when you want a graph-state form as an intermediate step for circuit synthesis or state-preparation workflows. Internally, the binary linear algebra is carried out over GF(2). On supported Python versions, stabgraph uses the maintained galois package for this backend. If that backend is unavailable, it falls back to a bundled NumPy implementation so the package still works.

[1] Design and Experimental Performance of Local Entanglement Witness Operators https://arxiv.org/abs/1911.01144

Installation

Install from PyPI:

python -m pip install stabgraph

For the accelerated backend on Python versions where galois is supported:

python -m pip install "stabgraph[accel]"

For local development:

git clone https://github.com/davamaro/stabgraph.git
cd stabgraph
python -m pip install -e .[test]

Usage

import stabgraph

G, c, t, z, R = stabgraph.convert(stabs, control=None, target=None, shuffle=False)

Reconstruct the signed post-processing generators and compare them with another stabilizer description:

signed_output = stabgraph.reconstruct_generators(G, t, z)
same_group = stabgraph.same_binary_stabilizer_group(
    [stab for _, stab in signed_output],
    stabs,
)
phase_signs = stabgraph.infer_generator_phase_signs(stabs, signed_output)

Input contract

  • stabs must be a non-empty list of exactly n independent commuting Pauli strings on n qubits.
  • Every stabilizer string must have the same length and use only the symbols I, X, Y, and Z.
  • control and target are optional lists of qubit labels in 0..n-1.
  • control and target must be disjoint and contain no duplicates.
  • shuffle=True randomizes the internal qubit ordering before selecting a valid control/target partition. This can be useful when searching for lower-degree graph representations.

At the moment, convert() expects exactly n independent commuting generators on n qubits. If you provide extra generators, the package now raises a clear error instead of failing later in the algorithm.

Return values

  • G is the adjacency matrix of the resulting graph state.
  • c is the completed list of control qubits.
  • t is the completed list of target qubits.
  • z is the subset of c where a pi/2 z-rotation is applied.
  • R is the binary matrix describing the stabilizer recombinations used during the transformation.

Reconstruction Helpers

The package also provides a few lightweight helper functions for checking and post-processing the output of convert():

  • reconstruct_generators(G, t, z) builds the signed generators obtained after applying the returned local Cliffords to the graph-state generators.
  • same_binary_stabilizer_group(left, right) checks whether two generator lists span the same binary stabilizer group over GF(2).
  • infer_generator_phase_signs(reference_stabs, signed_generators) infers the +/-1 phase of each reference generator relative to a signed generator basis, without requiring phase tracking inside convert().
  • recombine_generators(generators, R) applies a binary recombination matrix to either unsigned or signed generators.

Examples

Bell pair

>>> stabs = ['XX','ZZ']
>>> G , c , t , z , R = stabgraph.convert(stabs)
>>> G
np.array([[0,1],[1,0]])
>>> c
[0]
>>> t
[1]
>>> z
[]
>>> R
np.array([[1,0],[0,1]])

GHZ state fixing 0 as a control qubit and 1 as a target qubit

>>> stabs = ['XXX','ZZI','IZZ']
>>> G , c , t , z , R = stabgraph.convert(stabs,[0],[1])
>>> c
[0]
>>> t
[1,2]

Steane code in the |0> logical state. Multiple graphs can be obtained, so put shuffle=True to obtain one of them randomly chosen. The result respects the selection of control and target qubits

>>> stabs = ['XXXXIII','IXXIXXI','IIXXIXX','ZZZZIII','IZZIZZI','IIZZIZZ','ZZZZZZZ']
>>> G , c , t , z , R = stabgraph.convert(stabs, control = [0], shuffle=True)
>>> c
[0,1,2]
>>> G , c , t , z , R = stabgraph.convert(stabs, control = [2, 5], shuffle=True)
>>> c
[2,5,6]

Testing

Run the unit tests with:

python -m pytest

Continuous integration runs the test suite on supported Python versions through GitHub Actions.

Performance

Large stabilizer states can be slow because the heavy work is dense binary linear algebra over GF(2). This release also removes a few obvious Python-level bottlenecks in qubit reordering and Pauli-to-binary conversion. Notes for future backend work live in docs/ACCELERATION_NOTES.md.

Release notes

Recent user-facing changes are tracked in CHANGELOG.md.

Citation

@misc{amaro2019,
  author = 	"David Amaro",
  title = 	"StabGraph",
  year = 	"2019",
  month =   "July",
  publisher = {GitHub},
  journal = {GitHub repository},
  howpublished = {\url{https://github.com/davamaro/stabgraph}}
}

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