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A very fast and easy to use Quantum circuit simulator relying on Pauli propagation. Compatible with qiskit.

Project description

pyrauli: High-Performance Quantum Circuit Simulation

Build and test package Documentation Coverage Status Latest benchmarks

pyrauli is a high-performance Python package for quantum circuit simulation, powered by the C++ ProPauli library. It leverages the Heisenberg picture and a technique called Pauli back-propagation to efficiently calculate the expectation values of observables, making it particularly well-suited for certain classes of variational quantum algorithms and noise analysis.

Key Features

  • High Performance: Core simulation logic is implemented in C++ for maximum speed, wrapped in a user-friendly Python API.
  • Heisenberg Picture Simulation: Observables are evolved instead of the state vector, which can be significantly more efficient for calculating expectation values on large quantum systems.
  • Seamless Qiskit Integration: Use pyrauli as a drop-in backend for your existing Qiskit workflows, or leverage the PyrauliEstimator primitive for modern, algorithm-focused development.
  • Advanced Complexity Management: Fine-grained control over the simulation's resource usage through customizable Truncator and SchedulingPolicy objects.

Installation

pyrauli requires Python 3.9 or later. It can be installed from PyPI using pip.

Standard Installation

For core functionality:

pip install pyrauli

Installation with Qiskit Support

To enable the Qiskit integration features, install the [qiskit] extra:

pip install 'pyrauli[qiskit]'

Quick Start

Simulate a simple 2-qubit Bell state circuit and calculate the expectation value of the $Z \otimes I$ observable.

import pyrauli

# 1. Initialize a 2-qubit circuit
circuit = pyrauli.Circuit(2)

# 2. Add quantum operations
circuit.add_operation("H", 0)      # Hadamard on qubit 0
circuit.add_operation("CX", 0, 1)  # CNOT with control 0, target 1

# 3. Define an observable
# Here, we measure the Pauli Z observable on qubit 0
observable = pyrauli.Observable("ZI")

# 4. Run the simulation
# This evolves the observable backward through the circuit
final_observable = circuit.run(observable)

# 5. Retrieve the final expectation value
# The expectation value is calculated with respect to the initial |00...0> state
expectation_value = final_observable.get_expectation_value()

print(f"Final observable: {final_observable}")
print(f"Expectation value: {expectation_value}")

# Expected output:
# Final observable: +1 XI
# Expectation value: 0.0

Qiskit Backend Usage

from qiskit.circuit import QuantumCircuit, Parameter
from qiskit.transpiler import generate_preset_pass_manager
from qiskit.quantum_info import SparsePauliOp
from pyrauli import PBackend

# Create a parameterized Qiskit circuit
theta = Parameter('theta')
qc = QuantumCircuit(2)
qc.h(0)
qc.rz(theta, 0)
qc.cx(0, 1)

# Define an observable and instantiate the backend
obs = SparsePauliOp("ZI")
backend = PBackend()

# transpilation is supported (but not needed here)
pm = generate_preset_pass_manager(backend)
isa_qc = pm.run(qc)

# Run using the PUB (Primitive Unified Bloc) format
job = backend.run([(qc, obs, [3.14])])
result = job.result()
ev = result[0].data.evs[0]

print(f"Expectation value: {ev}")

Documentation

For comprehensive information, including tutorials, how-to guides, and the full API reference, please visit the official documentation: https://zefresk.github.io/pyrauli/

benchmarks

pyrauli latest benchmarks results are available here: https://zefresk.github.io/pyrauli/dev/bench/

References

This work is based on and implements ideas from the following articles:

  • Pauli Propagation: A Computational Framework for Simulating Quantum Systems, by Manuel S. Rudolph, Tyson Jones, Yanting Teng, Armando Angrisani, Zoë Holmes https://arxiv.org/abs/2505.21606

  • Efficient simulation of parametrized quantum circuits under non-unital noise through Pauli backpropagation, by Victor Martinez, Armando Angrisani, Ekaterina Pankovets, Omar Fawzi, Daniel Stilck França https://arxiv.org/abs/2501.13050

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