Author: Thiago Girao - PhD candidate in Physics, researching quantum information and quantum computing
This repository contains a complete, production-quality implementation of the Quantum Approximate Optimization Algorithm (QAOA) applied to the Maximum Cut (MaxCut) problem. QAOA is a hybrid quantum-classical algorithm that leverages current near-term quantum devices to solve combinatorial optimization problems.
The MaxCut problem is a fundamental NP-hard problem in computer science: given an undirected graph, partition the vertices into two sets to maximize the number of edges between the sets. This implementation demonstrates how variational quantum algorithms can approximate solutions to such hard problems.
Given an undirected graph G = (V, E), the Maximum Cut problem seeks to partition vertices into two disjoint sets S and S̄ such that the number of edges between S and S̄ is maximized:
MaxCut = max |{(u,v) ∈ E : u ∈ S, v ∈ S̄}|
MaxCut is NP-hard, meaning there is no known polynomial-time algorithm to solve it for large instances. The best classical polynomial-time approximation algorithm (Goemans-Williamson) achieves 0.878 approximation ratio.
QAOA provides an alternative approach using quantum computing, potentially offering better approximation ratios for certain problem instances. Even on current NISQ (Noisy Intermediate-Scale Quantum) devices, QAOA can provide useful approximate solutions.
QAOA is a variational quantum algorithm that works as follows:
For MaxCut, the cost Hamiltonian is:
H_C = (1/2) * Σ_{(i,j) ∈ E} (I - Z_i Z_j)
This Hamiltonian has eigenvalues aligned with the MaxCut objective. A bitstring where Z_i Z_j = -1 (qubits in different partitions) contributes positively to the energy.
The mixer Hamiltonian enables quantum tunneling between different regions of the search space:
H_M = Σ_i X_i
This is the transverse field that allows the quantum state to explore different computational basis states.
The QAOA state after p layers is:
|ψ(γ, β)⟩ = e^{-i β_p H_M} e^{-i γ_p H_C} ... e^{-i β_1 H_M} e^{-i γ_1 H_C} |+⟩^⊗n
Where:
- |+⟩ = (|0⟩ + |1⟩)/√2 is the initial equal superposition
- γ = (γ_1, ..., γ_p) are cost function angles
- β = (β_1, ..., β_p) are mixer angles
- p is the depth (number of layers)
The expected value of the cost Hamiltonian is:
E(γ, β) = ⟨ψ(γ, β)| H_C |ψ(γ, β)⟩
A classical optimizer (COBYLA in this implementation) minimizes -E(γ, β) to find optimal parameters.
The approximation ratio r is:
r = E_QAOA / E_MAX
where E_QAOA is the energy found by QAOA and E_MAX is the optimal value. QAOA guarantees r ≥ 0.692 for MaxCut with p=1, and the ratio typically improves with larger p.
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Cost Hamiltonian Construction (
create_maxcut_hamiltonian)- Builds SparsePauliOp representation of the MaxCut cost function
- Efficient for both sparse and dense graphs
-
QAOA Circuit Building (
build_qaoa_circuit)- Constructs parametrized quantum circuits
- Implements exp(-i γ H_C) using controlled-Z gates
- Implements exp(-i β H_M) using RX rotations
- Supports arbitrary number of layers p
-
Expectation Value Computation (
compute_expectation)- Uses Qiskit's Statevector simulator for exact simulation
- Computes ⟨ψ| H_C |ψ⟩ efficiently
-
Classical Optimization (
optimize_qaoa)- Uses scipy.optimize.minimize with COBYLA method
- Tracks convergence via callback function
- Supports random restarts for global optimization
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Solution Extraction (
extract_solution)- Samples most probable bitstring from QAOA state
- Returns probability of the solution
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Exact Solver (
brute_force_maxcut)- Computes exact solution for small graphs (n ≤ 20)
- Used for validation and benchmarking
-
Graph with Cut (
plot_graph_with_cut)- Visualizes graph with partition coloring
- Green edges indicate cut edges
- Shows exact and approximate solution quality
-
Optimization Landscape (
plot_optimization_landscape)- 2D heatmap of energy vs (gamma, beta) for p=1
- Reveals structure of parameter space
-
Convergence Plot (
plot_convergence)- Tracks optimization progress over iterations
- Useful for hyperparameter tuning
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Qiskit (≥1.0): IBM's quantum computing framework
- QuantumCircuit for circuit building
- Statevector for state representation and simulation
- SparsePauliOp for Hamiltonian representation
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NumPy (≥1.24): Numerical computations
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SciPy (≥1.10): Optimization algorithms
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NetworkX (≥3.0): Graph representation and analysis
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Matplotlib (≥3.7): Visualization
# Clone the repository
git clone <repository-url>
cd 04-qaoa-maxcut
# Create virtual environment (recommended)
python -m venv venv
source venv/bin/activate # On Windows: venv\Scripts\activate
# Install dependencies
pip install -r requirements.txtpython qaoa_maxcut.pyThe script demonstrates QAOA on three test cases:
-
6-node Random 3-regular Graph
- Solves with QAOA at depths p=1, 2, 3
- Compares with exact brute-force solution
- Computes approximation ratios
- Generates convergence plots and visualizations
- Plots optimization landscape for p=1
-
12-node Cycle Graph
- Demonstrates QAOA on a larger instance
- Uses p=2 layers
- Shows practical applicability
-
Complete Graph K_5
- MaxCut has known optimal value (5)
- Demonstrates QAOA performance on dense graphs
- Uses p=2 layers
The script produces:
Console Output:
- Iteration counts and convergence status
- Best energies found during optimization
- QAOA bitstring solutions
- Cut values and approximation ratios
- Summary statistics
Generated Files:
maxcut_exact.png: Exact solution visualizationmaxcut_qaoa_p1.png,maxcut_qaoa_p2.png,maxcut_qaoa_p3.png: QAOA solutions at different depthsmaxcut_cycle.png: Solution on 12-node cyclemaxcut_k5.png: Solution on K_5convergence_p1.png,convergence_p2.png,convergence_p3.png: Optimization convergenceoptimization_landscape.png: Energy landscape for p=1
import networkx as nx
from qaoa_maxcut import optimize_qaoa, extract_solution, plot_graph_with_cut
# Create or load your graph
G = nx.read_edgelist('your_graph.edgelist')
# Run QAOA
result = optimize_qaoa(G, p=2)
# Extract and visualize
circuit = build_qaoa_circuit(G, result['gamma'], result['beta'], p=2)
bitstring, prob = extract_solution(circuit)
plot_graph_with_cut(G, bitstring, "Your Graph", "output.png")Increasing p typically improves approximation quality at the cost of:
- Longer classical optimization time
- Deeper quantum circuits (more noise on real hardware)
- More parameters to optimize (2p parameters total)
result = optimize_qaoa(G, p=3) # Deeper circuitQAOA optimization works with any scipy optimizer:
result = optimize_qaoa(G, p=2, method='L-BFGS-B') # Bounded optimization
result = optimize_qaoa(G, p=2, method='SLSQP') # Sequential Least Squares- Circuit Simulation: O(2^n) where n is number of qubits
- Per Iteration: O(n_edges × p) for circuit construction + O(2^n) for state simulation
- Optimization: Typically converges in 100-500 iterations
- Total Time: O(n^2 × 2^n) for n ≤ 12-15 qubits
Current implementation uses statevector simulation, which scales exponentially:
- n ≤ 10: Very fast (< 1 second)
- n = 15: Few seconds
- n = 20: Minutes
- n > 20: Infeasible on classical simulators
For larger instances, consider:
- Noise-aware simulation (Qiskit Aer)
- Approximate simulation methods
- Real quantum hardware via IBM Quantum
-
Farhi, E., Goldstone, J., & Gutmann, S. (2014) A Quantum Approximate Optimization Algorithm arXiv:1411.4028
- Original QAOA paper introducing the algorithm
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Hadfield, S., Wang, Z., O'Gorman, B., et al. (2019) From the Perturbed Single Layer to the Collective Optimal QAOA arXiv:1910.08980
- Analysis of QAOA performance
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Zhou, L., Wang, S.-T., Choi, S., et al. (2020) Quantum Approximate Optimization Algorithm: Performance, Mechanism, and Implementation on Near-Term Devices Physical Review X 10, 021067
- Comprehensive review and implementation guide
- Goemans, M. X., & Williamson, D. P. (1995). "Improved approximation algorithms for maximum cut and satisfiability problems using semidefinite programming." Journal of the ACM, 42(6), 1115-1145.
- Karp, R. M. (1972). "Reducibility among combinatorial problems." In Complexity of computer computations.
QAOA bridges quantum and classical computing:
- Quantum Advantage: Explores parameter space using quantum superposition
- Variational: Uses classical optimizer to find good parameters
- NISQ-Friendly: Works with shallow circuits suitable for near-term devices
- Hybrid: Combines quantum circuit evaluation with classical optimization
This approach is considered one of the most promising near-term applications of quantum computers.
This implementation emphasizes:
- Correctness: Validated against exact solutions for small instances
- Clarity: Well-documented functions with comprehensive docstrings
- Efficiency: Optimized Hamiltonian construction and simulation
- Reproducibility: Fixed random seeds, detailed output
- Extensibility: Modular design for custom graphs and optimizers
Install dependencies:
pip install -r requirements.txtFor large graphs (n > 15), statevector simulation becomes slow. Consider:
- Reducing graph size for testing
- Using sparse graphs (fewer edges)
- Using only p=1 or p=2 layers
Try:
- Increasing
maxiterin scipy.optimize.minimize - Using different optimizer (e.g., 'SLSQP')
- Checking graph structure (disconnected components often harder)
Potential extensions of this implementation:
- Noise Models: Add quantum noise simulation for realistic NISQ analysis
- Warm Starting: Use classical approximate solutions to initialize QAOA
- Parameter Transferability: Analyze parameter reuse across graph families
- Hybrid Algorithms: Combine QAOA with classical heuristics
- Hardware Compilation: Prepare circuits for specific quantum backends
- Detailed Analytics: More sophisticated performance benchmarking
This implementation is provided as-is for educational and research purposes.
For questions or collaborations:
- Thiago Girao
- PhD candidate in Physics
- Focus: Quantum Information and Quantum Computing
Last Updated: March 2026 QAOA Implementation Version: 1.0