hardware simulation

Split-Evolution Quantum Phase Estimation for Particle-Conserving Hamiltonians

Curator's Take

This article demonstrates a clever modification to quantum phase estimation that could significantly reduce the resource requirements for quantum chemistry simulations on near-term devices. By replacing expensive controlled time evolution operations with CSWAP-based interference between two registers, the split-evolution approach achieves substantial reductions in gate counts and circuit depth while maintaining compatibility with approximate eigenstates that arise in practical quantum simulations. The demonstration on Quantinuum's H2 system with ethylene molecules shows this isn't just theoretical - the method works on real hardware and includes built-in error detection capabilities through auxiliary registers. These resource savings become more pronounced at higher precision levels, making this technique particularly valuable for the complex molecular systems that represent quantum computing's most promising near-term applications in drug discovery and materials science.

— Mark Eatherly

Summary

We present a hardware demonstration and resource analysis of split-evolution quantum phase estimation (SE-QPE) on a Quantinuum System Model H2 quantum computer. SE-QPE is a modification to canonical QPE for particle-conserving Hamiltonians in which controlled time evolution is replaced by CSWAP-based interference between a target register and a reference register. For factorizations of time evolution with a shared eigenbasis, SE-QPE preserves the phase-register outcome distribution of canonical QPE and, unlike with compute--uncompute substitutions, it remains compatible with non-exact eigenstates. The substitution removes controlled-simulation overhead and enables parallel evolution on two registers, reducing the depth of each phase-kickback block. Resource analysis for Trotterized double-factorized chemistry Hamiltonians shows that the substitution becomes increasingly favorable at higher phase powers, as such combining QPE and SE-QPE implementations can be a useful option. Over a range of FeMoco active spaces, SE-QPE reduces time evolution resources, with asymptotic reductions of about 33% in CX count, 25% in $T$ count, and an asymptotic depth ratio of $3/N$ for CX layers. On Quantinuum H2-2, a four-qubit model ethylene demonstration with explicit inverse QFT and repeated phase-kickback steps up to 6 phase bits yields distinct energies and shows the auxiliary registers provide useful error detection filters.