Quantum annealing processors implement analog-digital quantum computing via effective XY-model evolution combined with auxiliary-qubit arbitrary-basis initialization and measurement, demonstrated through oscillations, fermionic quantum walks, and Anderson localization.
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The Triangle Criterion detects mixed-state magic, proves multi-qubit distillation is strictly stronger than single-qubit schemes, and identifies a purity bound plus undetectable unfaithful magic states.
Rydberg atoms on a triangular lattice host a deconfined quantum critical point between 1/3 and 2/3 filling phases, with predicted critical exponents, emergent U(1) symmetry in a CFT, and numerical confirmation.
Optimizing collision gates for ultracold fermions in double-well potentials reveals momentum-dependent interaction energies that are higher for atoms starting in separate subwells than the same subwell, supporting case-specific high-fidelity gates beyond Fermi-Hubbard models.
citing papers explorer
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Analog-Digital Quantum Computing with Quantum Annealing Processors
Quantum annealing processors implement analog-digital quantum computing via effective XY-model evolution combined with auxiliary-qubit arbitrary-basis initialization and measurement, demonstrated through oscillations, fermionic quantum walks, and Anderson localization.
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Triangle Criterion: a mixed-state magic criterion with applications in distillation and detection
The Triangle Criterion detects mixed-state magic, proves multi-qubit distillation is strictly stronger than single-qubit schemes, and identifies a purity bound plus undetectable unfaithful magic states.
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Deconfined quantum criticality on a triangular Rydberg array
Rydberg atoms on a triangular lattice host a deconfined quantum critical point between 1/3 and 2/3 filling phases, with predicted critical exponents, emergent U(1) symmetry in a CFT, and numerical confirmation.
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Optimizing two-qubit gates for ultracold fermions in optical lattices
Optimizing collision gates for ultracold fermions in double-well potentials reveals momentum-dependent interaction energies that are higher for atoms starting in separate subwells than the same subwell, supporting case-specific high-fidelity gates beyond Fermi-Hubbard models.