| name | fourier-lcu-quantum-optimization |
| description | Fourier-based Linear Combination of Unitaries (LCU) methodology for efficient quantum circuit decomposition in optimization algorithms. Covers ancilla-free LCU constructions, Fourier decomposition of diagonal/non-diagonal unitaries, formal connection to Lagrangian relaxation, and hardware-friendly gate layer simplification. Activation: LCU, linear combination of unitaries, Fourier quantum, quantum optimization decomposition, constraint penalty, XY-mixer, cardinality constraint, ancilla-free quantum, sampling overhead, circuit complexity tradeoff |
| license | Complete terms in LICENSE.txt |
| metadata | {"arxiv_id":"2605.18985","published":"2026-05-18","authors":"Almudena Carrera Vazquez, Daniel J. Egger, Stefan Woerner","tags":["LCU","Fourier","quantum-optimization","QAOA","constraint-handling","ancilla-free","Lagrangian-relaxation"]} |
Fourier-Based LCU for Quantum Optimization
Efficient circuit decomposition via Fourier-based Linear Combination of Unitaries (LCU) for quantum optimization algorithms.
Context
Quantum optimization algorithms (QAOA, VQE) require complex multi-qubit interactions that are expensive to implement. LCU provides a framework for approximating these circuits by decomposing unitaries into simpler components with polynomial sampling overhead.
Core Methodology
1. Fourier-Based LCU Decomposition
Decompose complex unitaries U = exp(-iH) via Fourier series:
U ≈ Σ_k c_k · V_k
where V_k are simple single-qubit or low-connectivity gate layers, and c_k are Fourier coefficients.
2. Ancilla-Free Sampling Pattern
Key insight: when the goal is sampling high-quality bitstrings (not reproducing full output distribution), ancilla qubits can be eliminated:
- Classically evaluate candidate solutions
- Sample from the decomposed distribution
- Trade circuit complexity for polynomial sampling overhead
- No ancilla qubits needed → more available qubits for problem encoding
3. Constraint Handling via Fourier Penalties
Fourier-based penalty constructions handle constraints efficiently:
- Cardinality constraints: Decompose into single-qubit gate layers
- Fully connected XY-mixer: Replace multi-qubit interactions with simpler structures
- Formal connection: Fourier penalties ≡ Lagrangian relaxation (unified view of quantum and classical constraint handling)
4. Hardware-Friendly Implementation
Replace highly connected qubit interactions with:
- Single-qubit gate layers (O(n) gates)
- Significantly simpler structures (O(n log n) vs O(n²))
- Maintained performance guarantees vs fully coherent implementations
Implementation Steps
- Identify complex unitary: Find highly connected terms in Hamiltonian (e.g., fully connected penalties, XY-mixers)
- Compute Fourier decomposition: Express as sum of simpler unitaries with known coefficients
- Implement sampling circuit: Build ancilla-free circuit that samples from decomposed distribution
- Classical evaluation loop: Evaluate sampled bitstrings classically, keep high-quality solutions
- Budget tradeoff: Balance circuit depth reduction against sampling overhead multiplier
Pitfalls
- Sampling overhead grows polynomially: For very high precision requirements, fully coherent implementation may still be better
- Not for state preparation: This pattern works for optimization (sampling) but NOT for algorithms requiring exact state preparation
- Fourier series convergence: Number of terms depends on function smoothness — discontinuous penalties need more terms
- Classical evaluation bottleneck: Requires efficient classical evaluation of objective function
Verification
- Compare solution quality: Fourier-LCU vs fully coherent on same problem
- Validate constraint satisfaction: Check that penalties enforce constraints correctly
- Measure resource savings: Gate count reduction vs sampling overhead ratio