Skip to content
aiqbench takeQuantum Computing

aiqbench analysis

This paper presents exact quantum circuit constructions for simulating Heisenberg triangle models with Dzyaloshinskii-Moriya interactions, optimizing qubit operations to as few as 8 CNOT gates under specific symmetry conditions. By reducing complex multi-spin evolutions to single-qubit rotations and providing scalable local blocks, the work offers practical tools for lattice simulations on near-term quantum hardware.
Source coveringarXiv
What this isA model's reading of the article and related coverage, written for aiqbench. Not the publisher's words.

Exact quantum circuits for a Heisenberg triangle with Dzyaloshinskii-Moriya interaction

arXiv2 min read

arXiv:2609.15411v1 Announce Type: new Abstract: We construct exact quantum circuits for a three-spin Heisenberg triangle with Dzyaloshinskii-Moriya (DM) interaction. A change of basis reduces pure DM evolution with arbitrary couplings to two single-qubit rotations, giving a circuit with at most 8 CNOT gates. When $J$ and $D$ are each the same on all bonds, one fixed basis gives a circuit with at most 10 CNOT gates for any real $J,D,t$. Local spin rotations extend the construction to a family with unequal DM couplings and nonzero exchange, requiring at most 14 CNOT gates. All circuits act on the full Hilbert space. An alternative pure DM implementation uses five two-qubit DM gates: analytically retuning the angles of one symmetric Strang step makes it exact. A 12-spin kagome example illustrates the use of these exact local blocks in lattice simulation.

Abstract:We construct exact quantum circuits for a three-spin Heisenberg triangle with Dzyaloshinskii-Moriya (DM) interaction. A change of basis reduces pure DM evolution with arbitrary couplings to two single-qubit rotations, giving a circuit with at most 8 CNOT gates. When $J$ and $D$ are each the same on all bonds, one fixed basis gives a circuit with at most 10 CNOT gates for any real $J,D,t$. Local spin rotations extend the construction to a family with unequal DM couplings and nonzero exchange, requiring at most 14 CNOT gates. All circuits act on the full Hilbert space. An alternative pure DM implementation uses five two-qubit DM gates: analytically retuning the angles of one symmetric Strang step makes it exact. A 12-spin kagome example illustrates the use of these exact local blocks in lattice simulation.

13 pages, 6 figures. Supplementary material and code are available at this https URL

arXiv:2609.15411 [quant-ph]

(or arXiv:2609.15411v1 [quant-ph] for this version)

https://doi.org/10.48550/arXiv.2609.15411 Focus to learn more arXiv-issued DOI via DataCite (pending registration)

arXivLabs is a framework that allows collaborators to develop and share new arXiv features directly on our website.

Both individuals and organizations that work with arXivLabs have embraced and accepted our values of openness, community, excellence, and user data privacy. arXiv is committed to these values and only works with partners that adhere to them.

Have an idea for a project that will add value for arXiv's community? Learn more about arXivLabs.

Full text under the publisher's open licence · 237 words

Related coverage