Logarithmic-Depth Quantum Circuits for Hamming Weight Projections
arXiv:2404.07151 · doi:10.1103/PhysRevA.110.052401
Abstract
A pure state of fixed Hamming weight is a superposition of computational basis states such that each bitstring in the superposition has the same number of ones. Given a Hilbert space of the form , or an -qubit system, the identity operator can be decomposed as a sum of projectors onto subspaces of fixed Hamming weight. In this work, we propose several quantum algorithms that realize a coherent Hamming weight projective measurement on an input pure state, meaning that the post-measurement state of the algorithm is the projection of the input state onto the corresponding subspace of fixed Hamming weight. We analyze a depth-width trade-off for the corresponding quantum circuits, allowing for a depth reduction of the circuits at the cost of more control qubits. For an -qubit input, the depth-optimal algorithm uses control qubits and the corresponding circuit has depth , assuming that we have the ability to perform qubit resets. Furthermore, the proposed algorithm construction uses only one- and two-qubit gates.
17 pages, 14 figures; see independent and concurrent work of Zi, Nie, Sun at arXiv:2404.06052 and Piroli, Styliaris, Cirac at arXiv:2403.07604. Accepted for publication in Physical Review A
References in corpus (13)
- Operational Resource Theory of Coherence
- From Classical to Quantum Shannon Theory
- Quantum Information Processing with Finite Resources -- Mathematical Foundations
- Pretending to factor large numbers on a quantum computer
- Quantum Circuits with Unbounded Fan-out
- Efficient compression of quantum information
- Quantum Algorithmic Readout in Multi-Ion Clocks
- Multivariate trace estimation in constant quantum depth
- Avoiding coherent errors with rotated concatenated stabilizer codes
- Quantum Networks for Concentrating Entanglement
- Testing symmetry on quantum computers
- Entanglement of two non-interacting qubits via a mesoscopic system
- Multicasting Homogeneous and Heterogeneous Quantum States in Quantum Networks