Skip to content
DraconiticResearch
Search Sources API
178,970 studies31 sourcesUpdated 28 min ago
PreprintarXiv licencearXiv

Sampling isometric tensor network states with monitored quantum circuits

Abstract

Projected entangled pair states (PEPS) provide an efficient variational ansatz for two-dimensional quantum phases, but computing observables remains challenging because PEPS contraction is generally costly. Here, we parameterize two-dimensional quantum states using variational PEPS subject to isometric constraints and map the resulting ansatz onto monitored quantum circuits, replacing tensor-network contraction with circuit sampling. For infinite cylinders, the transfer matrix defines a quantum channel on the virtual boundary. We use a fixed-point treatment and a monitored-circuit unraveling of this channel to evaluate observables efficiently. Using a constant number of variational parameters and a number of qubits that scales only with the cylinder width, our method yields a phase diagram for the J1-J2 model in qualitative agreement with DMRG results. Because the monitored circuits are compatible with near-term quantum hardware, this approach provides a hybrid quantum-classical framework for simulating two-dimensional quantum many-body systems.

Related

  1. Surviving readout errors and incomplete postselection in monitored quantum circuits
    Murtaza Ali Mir, Teemu Ojanen, Ali G. Moghaddam
    arXivPreprintCC BY-NC-ND 4.0Full textCondensed matterQuantum physics & quantum informationarXiv
  2. Universal purification dynamics of monitored Clifford circuits
    Beatrice Magni, Federico Gerbino, Xhek Turkeshi +1
    HALPreprintPublisher termsFull textQuantum physics & quantum informationHAL
  3. Multinomial shot sampling for quantum circuits
    Ijaz Ahamed Mohammad, Daniel Nagaj, Martin Plesch
    arXivPreprintarXiv licenceFull textQuantum physics & quantum informationarXiv
  4. Zero- Versus Infinite-Temperature Damping in Variational Quantum Circuits: Feature Scale, Sampling Cost, and Frame Gauge
    Vu-Quoc-Minh Nguyen, Tuan-Vu Truong, Hoang-Long Nguyen +1
    arXivPreprintarXiv licenceFull textQuantum physics & quantum informationarXiv
  5. Measurement-Induced Phase Transitions and Logical-Space Localization in Floquet Monitored Clifford Circuits
    Hyunsoo Ha, David A. Huse
    arXivPreprintarXiv licenceFull textQuantum physics & quantum informationarXiv
BibTeX
@misc{rong2026sampling,
  title = {{Sampling isometric tensor network states with monitored quantum circuits}},
  author = {Yuqing Rong and Huan-Hai Zhou and Guo-Yi Zhu and Jinguo Liu},
  howpublished = {arXiv},
  year = {2026},
  month = aug,
  doi = {10.48550/arxiv.2608.18511},
  eprint = {2608.18511},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2608.18511},
}
RIS
TY  - UNPB
TI  - Sampling isometric tensor network states with monitored quantum circuits
AU  - Yuqing Rong
AU  - Huan-Hai Zhou
AU  - Guo-Yi Zhu
AU  - Jinguo Liu
PY  - 2026
DA  - 2026/08/29
PB  - arXiv
DO  - 10.48550/arxiv.2608.18511
UR  - https://arxiv.org/abs/2608.18511
AB  - Projected entangled pair states (PEPS) provide an efficient variational ansatz for two-dimensional quantum phases, but computing observables remains challenging because PEPS contraction is generally costly. Here, we parameterize two-dimensional quantum states using variational PEPS subject to isometric constraints and map the resulting ansatz onto monitored quantum circuits, replacing tensor-network contraction with circuit sampling. For infinite cylinders, the transfer matrix defines a quantum channel on the virtual boundary. We use a fixed-point treatment and a monitored-circuit unraveling of this channel to evaluate observables efficiently. Using a constant number of variational parameters and a number of qubits that scales only with the cylinder width, our method yields a phase diagram for the J_1-J_2 model in qualitative agreement with DMRG results. Because the monitored circuits are compatible with near-term quantum hardware, this approach provides a hybrid quantum-classical framework for simulating two-dimensional quantum many-body systems.
ER  -