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Fast Amplification of QMA

2 Pith papers cite this work. Polarity classification is still indexing.

2 Pith papers citing it
abstract

Given a verifier circuit for a problem in QMA, we show how to exponentially amplify the gap between its acceptance probabilities in the `yes' and `no' cases, with a method that is quadratically faster than the procedure given by Marriott and Watrous. Our construction is natively quantum, based on the analogy of a product of two reflections and a quantum walk. Second, in some special cases we show how to amplify the acceptance probability for good witnesses to 1, making a step towards the proof that QMA with one-sided error is equal to QMA. Finally, we simplify the filter-state method to search for QMA witnesses by Poulin and Wocjan.

fields

quant-ph 2

years

2024 1 2023 1

representative citing papers

A shortcut to an optimal quantum linear system solver

quant-ph · 2024-06-17 · accept · novelty 7.0

The paper gives a QLSS with query complexity (1+O(ε))κ ln(2√2/ε) using one kernel reflection when ||x|| is known, or O(κ log(1/ε)) overall, with explicit bound 56κ + 1.05κ ln(1/ε).

Quantum Algorithms for Simulating Nuclear Effective Field Theories

quant-ph · 2023-12-08 · unverdicted · novelty 6.0

Resource estimates for quantum simulation of pionless and pionful nuclear lattice EFTs, including time evolution and energy estimation, with new error bounds from symmetries and locality yielding orders-of-magnitude improvements for the pionless case.

citing papers explorer

Showing 2 of 2 citing papers.

  • A shortcut to an optimal quantum linear system solver quant-ph · 2024-06-17 · accept · none · ref 25 · internal anchor

    The paper gives a QLSS with query complexity (1+O(ε))κ ln(2√2/ε) using one kernel reflection when ||x|| is known, or O(κ log(1/ε)) overall, with explicit bound 56κ + 1.05κ ln(1/ε).

  • Quantum Algorithms for Simulating Nuclear Effective Field Theories quant-ph · 2023-12-08 · unverdicted · none · ref 198 · internal anchor

    Resource estimates for quantum simulation of pionless and pionful nuclear lattice EFTs, including time evolution and energy estimation, with new error bounds from symmetries and locality yielding orders-of-magnitude improvements for the pionless case.