hardware algorithms simulation

Quantum dynamics of two $XX$ interacting PT-symmetric non-Hermitian qubits: enhancement of quantum annealing

Curator's Take

This research explores a fascinating twist on quantum annealing by incorporating PT-symmetric non-Hermitian qubits, which could dramatically improve success rates in finding optimal solutions to complex optimization problems. While individual PT-symmetric qubits have been demonstrated across multiple quantum platforms, this work breaks new ground by theoretically investigating how networks of these unconventional qubits interact and evolve together. The key finding that even small non-Hermitian modifications can greatly enhance the probability of reaching the ground state suggests a potentially powerful new approach to quantum optimization that could outperform traditional annealing methods. This theoretical framework opens exciting possibilities for next-generation quantum annealers that leverage the unique properties of non-Hermitian quantum systems.

— Mark Eatherly

Summary

Quantum information platforms enable analog quantum simulations, such as quantum annealing, offering a promising route to solving complex combinatorial optimization problems. Here, we propose a quantum information architecture based on networks of interacting parity-time (PT)-symmetric non-Hermitian qubits. While the dynamics of individual PT-symmetric qubits have been experimentally demonstrated across multiple platforms including NV centers, superconducting circuits, and trapped-ion systems yet coherent dynamics in interacting systems remain largely unexplored. To address this issue we theoretically investigate stationary and time-dependent Hamiltonians relevant to quantum annealing using a minimal model of two interacting XX-coupled PT-symmetric non-Hermitian qubits. We analyze both symmetry-preserving and symmetry-broken regimes and demonstrate that adding even tiny PT-symmetric non-Hermitian terms in the qubits Hamiltonian allows to greatly enhance the probability of reaching the ground state after annealing.