Spin lattices with two-body Hamiltonians for which the ground state encodes a cluster state
arXiv:0805.2980 · doi:10.1103/PhysRevA.78.062306
Abstract
We present a general procedure for constructing lattices of qubits with a Hamiltonian composed of nearest-neighbour two-body interactions such that the ground state encodes a cluster state. We give specific details for lattices in one-, two-, and three-dimensions, investigating both periodic and fixed boundary conditions, as well as present a proof for the applicability of this procedure to any graph. We determine the energy gap of these systems, which is shown to be independent of the size of the lattice but dependent on the type of lattice (in particular, the coordination number), and investigate the scaling of this gap in terms of the coupling constants of the Hamiltonian. We provide a comparative analysis of the different lattice types with respect to their usefulness for measurement-based quantum computation.
16 pages, 5 figures, comments welcome; v2 added some new results about exact solutions to this model; v3 published version
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- Verification of Many-Qubit States
- Phase transitions and localizable entanglement in cluster-state spin chains with Ising couplings and local fields
- Verified measurement-based quantum computing with hypergraph states
- Measurement-based quantum computation in a 2D phase of matter
- Generalized Cluster States Based on Finite Groups
- Optical spin-1 chain and its use as a quantum computational wire
- Graph states as ground states of two-body frustration-free Hamiltonians
- Quantum computation via measurements on the low-temperature state of a many-body system
- Entanglement in pure and thermal cluster states
- Bounds on universal quantum computation with perturbed 2d cluster states
- Measurement-Based Quantum Computation on Two-Body Interacting Qubits with Adiabatic Evolution
- Quantum phase transitions in the -layer Ising toric code
- Spectral properties for a family of two-dimensional quantum antiferromagnets