PreprintCC BY-NC-SA 4.0arXiv
A classical oracle separation between QMA and QMA(2)
Abstract
We exhibit a classical oracle relative to which QMA \neq QMA(2). The separation is based on a separable Hamiltonian problem defined by signed edge constraints on a graph. The YES instances have zero-energy product states, while the NO instances, constructed using the antisymmetric subspace, have entangled zero-energy states but no low-energy product states. For the QMA lower bound, we use compressed-oracle techniques to track the information learned by a quantum computation making few queries to a YES instance. The key step is to map the resulting superpositions of partial oracle records to the NO family without significantly changing the verifier's behavior.
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BibTeX
@misc{grewal2026classical,
title = {{A classical oracle separation between QMA and QMA(2)}},
author = {Sabee Grewal and Saachi Mutreja and Kabir Tomer},
howpublished = {arXiv},
year = {2026},
month = oct,
doi = {10.48550/arxiv.2610.06760},
eprint = {2610.06760},
archivePrefix = {arXiv},
url = {https://arxiv.org/abs/2610.06760},
note = {CC BY-NC-SA 4.0},
}
RIS
TY - UNPB
TI - A classical oracle separation between QMA and QMA(2)
AU - Sabee Grewal
AU - Saachi Mutreja
AU - Kabir Tomer
PY - 2026
DA - 2026/10/05
PB - arXiv
DO - 10.48550/arxiv.2610.06760
UR - https://arxiv.org/abs/2610.06760
AB - We exhibit a classical oracle relative to which QMA \neq QMA(2). The separation is based on a separable Hamiltonian problem defined by signed edge constraints on a graph. The YES instances have zero-energy product states, while the NO instances, constructed using the antisymmetric subspace, have entangled zero-energy states but no low-energy product states. For the QMA lower bound, we use compressed-oracle techniques to track the information learned by a quantum computation making few queries to a YES instance. The key step is to map the resulting superpositions of partial oracle records to the NO family without significantly changing the verifier's behavior.
ER -