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Lloyd, Universal quantum simulators, Science273, 1073 (1996)

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36 Pith papers citing it
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representative citing papers

Algorithmic Locality via Provable Convergence in Quantum Tensor Networks

quant-ph · 2026-04-23 · unverdicted · novelty 8.0

For PEPS with strong injectivity above a threshold, belief propagation finds fixed points efficiently and cluster-corrected BP approximates observables to 1/poly(N) error in poly(N) time, with local perturbations affecting the fixed point only locally.

Quantum Accreditation with Non-Clifford Two-qubit Gates

quant-ph · 2026-05-19 · unverdicted · novelty 7.0

Develops practical scalable protocols to upper-bound total variation distance for quantum circuits with non-Clifford two-qubit gates and generalizes Pauli twirling to non-Pauli bases.

Obstructions to universality in globally controlled qubit graphs

quant-ph · 2026-04-20 · unverdicted · novelty 7.0

The conjecture that breaking all non-trivial graph automorphisms suffices for universality in globally controlled qubit systems is disproved by connected graphs with trivial automorphism groups whose generated Lie algebras are nonetheless non-universal.

Taming Trotter Errors with Quantum Resources

quant-ph · 2026-04-15 · conditional · novelty 7.0

Entanglement entropy bounds the variance of Trotter error downward, and magic drives the error kurtosis downward (Kur = α + βM, β<0 for large systems).

Quantum Error-Corrected Computation of Molecular Energies

quant-ph · 2025-05-14 · conditional · novelty 7.0

First end-to-end demonstration of quantum error correction integrated with quantum phase estimation to compute molecular hydrogen ground-state energy to 0.001(13) hartree accuracy on Quantinuum H2-2 hardware.

How thermal is a filtered state?

quant-ph · 2026-07-07 · conditional · novelty 6.0

Under Floquet ETH, the trace distance between energy-filtered and thermal states is bounded by O(√δ), where δ is the filter width.

Adiabatic Quantum Phase Estimation

quant-ph · 2026-05-21 · unverdicted · novelty 6.0

An adiabatic protocol for quantum phase estimation that reaches optimal scaling T = O(1/ε log(1/δ)) by encoding eigenvalues in computational basis populations rather than phases.

Adiabatic Error Cancellation in Berry Phase Estimation

quant-ph · 2026-04-22 · conditional · novelty 6.0

Forward–reverse evolution, Richardson extrapolation, and runtime randomization cancel the leading O(T^{-1}) adiabatic phase error in Berry phase estimation, yielding O(ε^{-3/2}) total cost (QPE) or Θ(ε^{-1/3}) coherent runtime (Hadamard test).

Tensor network surrogate models for variational quantum computation

quant-ph · 2026-04-22 · unverdicted · novelty 6.0

Tensor network simulations act as effective surrogate models for training QAOA on large 2D lattices, overcoming limits of parameter transfer from small instances and remaining classically feasible with moderate bond dimensions.

When is randomization advantageous in quantum simulation?

quant-ph · 2026-04-08 · conditional · novelty 6.0

Randomized sparse-QSVT reduces gate counts by up to 10x for inhomogeneous many-term Hamiltonians at moderate error (around 10^{-3}), but deterministic QSVT becomes cheaper for higher precision.

Quantum Finite Temperature Lanczos Method

quant-ph · 2026-03-26 · unverdicted · novelty 6.0

QFTLM computes thermal expectation values on quantum computers by merging quantum Krylov methods with efficient typical-state preparation for trace estimation.

Universal Predictors for Mixing Time more than Liouvillian Gap

quant-ph · 2026-01-09 · unverdicted · novelty 6.0

Mixing time of Lindblad-governed open quantum systems is determined by the Liouvillian gap plus trace-norm factors of eigenmodes, yielding rapid mixing conditions via sparsity constraints on the Hamiltonian and local Lindblad operators.

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Showing 36 of 36 citing papers.