Skip to content
DraconiticResearch
Search Sources API
197,357 studies31 sourcesUpdated 3 min ago
PreprintCC BY-NC-ND 4.0arXiv

Using domain walls to benchmark fast quantum anneals

Abstract

We consider the distribution of domain walls arising in ground states of frustrated 1-dimensional Ising spin chains with anti-parallel boundary spins. For ideal chains, a sine-squared particle-in-a-box distribution of domain walls is expected in the quantum setting, and a uniform distribution expected classically. However, for chains with random imperfections, prior work [Chancellor et al., npj Quantum Inf. 8, 73, 2022] found that the distribution in a physical implementation corresponded to neither. Instead, the domain wall distribution forms a U-shaped profile arising from a classical model with random fields, where the combination of averaging over these fields and thermal averaging produces the characteristic U-shape. With D-Wave's newer fast anneal feature, we access anneal times shorter than the coherence time and observe the expected coherent quantum behavior in the form of a sine-squared distribution. For the shortest available anneal time, the dynamics have not yet reached the sine-squared shape and instead display a different U-shape in the middle of the chains. This motivates using the extent of the domain wall distribution tail in this regime as a platform independent metric that provides a signature of both coherence time and noise levels.

Related

  1. Big Bang Nucleosynthesis Confronts Domain Walls and First-Order Phase Transitions as the Pulsar Timing Array Explanations
    Fatemeh Elahi, Diego Fortini, Yann Gouttenoire +2
    HALPreprintCC BY-NC-ND 4.0Full textCosmologyHigh-energy & particle physicsHALarXiv
  2. Fermionic Signatures of Antispacetime-spacetime Domain Walls
    Justine Charles A. Elveña, Kristian Hauser Villegas
    arXivPreprintarXiv licenceFull textGravitation & general relativityarXiv
  3. Ferron-driven motion of non-collinear ferroelectric domain walls
    Huanhuan Yang, Gerrit E. W. Bauer
    arXivPreprintarXiv licenceFull textCondensed matterarXiv
  4. Exact solutions of nonreciprocal Su-Schrieffer-Heeger model with domain walls
    Tong Wang, Mengjie Yang, Flore K. Kunst
    arXivPreprintCC BY-NC-SA 4.0Full textCondensed matterQuantum physics & quantum informationarXiv
  5. Domain walls in R3c-structured NaNbO3
    Jack G. Nedell, Craig J. Fennie
    arXivPreprintarXiv licenceFull textCondensed matterarXiv
BibTeX
@misc{chowdhury2026using,
  title = {{Using domain walls to benchmark fast quantum anneals}},
  author = {Shushmi Chowdhury and Asa Hopkins and Nick Chancellor and Viv Kendon},
  howpublished = {arXiv},
  year = {2026},
  month = oct,
  doi = {10.48550/arxiv.2610.40504},
  eprint = {2610.40504},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2610.40504},
  note = {CC BY-NC-ND 4.0},
}
RIS
TY  - UNPB
TI  - Using domain walls to benchmark fast quantum anneals
AU  - Shushmi Chowdhury
AU  - Asa Hopkins
AU  - Nick Chancellor
AU  - Viv Kendon
PY  - 2026
DA  - 2026/10/29
PB  - arXiv
DO  - 10.48550/arxiv.2610.40504
UR  - https://arxiv.org/abs/2610.40504
AB  - We consider the distribution of domain walls arising in ground states of frustrated 1-dimensional Ising spin chains with anti-parallel boundary spins. For ideal chains, a sine-squared particle-in-a-box distribution of domain walls is expected in the quantum setting, and a uniform distribution expected classically. However, for chains with random imperfections, prior work [Chancellor et al., npj Quantum Inf. 8, 73, 2022] found that the distribution in a physical implementation corresponded to neither. Instead, the domain wall distribution forms a U-shaped profile arising from a classical model with random fields, where the combination of averaging over these fields and thermal averaging produces the characteristic U-shape. With D-Wave's newer fast anneal feature, we access anneal times shorter than the coherence time and observe the expected coherent quantum behavior in the form of a sine-squared distribution. For the shortest available anneal time, the dynamics have not yet reached the sine-squared shape and instead display a different U-shape in the middle of the chains. This motivates using the extent of the domain wall distribution tail in this regime as a platform independent metric that provides a signature of both coherence time and noise levels.
ER  -