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Physical Review A

Natural three-qubit interactions in one-way quantum computing (5 pages)

Mark Tame, Mauro Paternostro

Published Jan 1, 2006• 1 citation
OpenAlex

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Natural three-qubit interactions in one-way quantum computing

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The ground states of some many-body quantum systems can serve as resource states for the one-way quantum computing model, achieving the full power of quantum computation. Such resource states are found, for example, in spin-$\frac{5}{2}$ and spin-$\frac{3}{2}$ systems. It is, of course, desirable to have a natural resource state in a spin-$\frac{1}{2}$, that is, qubit system. Here, we give a negative answer to this question for frustration-free systems with two-body interactions. In fact, it is shown to be impossible for any genuinely entangled qubit state to be a nondegenerate ground state of any two-body frustration-free Hamiltonian. What is more, we also prove that every spin-$\frac{1}{2}$ frustration-free Hamiltonian with two-body interaction always has a ground state that is a product of single- or two-qubit states. In other words, there cannot be any interesting entanglement features in the ground state of such a qubit Hamiltonian.

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New Quantum Algorithms using Multi-Qubit Interaction

Information Sciences Letters•Sep 1, 2021•0 citations
We address the effects of natural three-qubit interactions on the computational power of one-way quantum computation. A benefit of using more sophisticated entanglement structures is the ability to construct compact and economic simulations of quantum algorithms with limited resources. We show that the features of our study are embodied by suitably prepared optical lattices, where effective three-spin interactions have been theoretically demonstrated. We use this to provide a compact construction for the Toffoli gate. Information flow and two-qubit interactions are also outlined, together with a brief analysis of relevant sources of imperfection.
The ground states of some many-body quantum systems can serve as resource states for the one-way quantum computing model, achieving the full power of quantum computation. Such resource states are found, for example, in spin-52\frac{5}{2}25​ and spin-32\frac{3}{2}23​ systems. It is, of course, desirable to have a natural resource state in a spin-12\frac{1}{2}21​, that is, qubit system. Here, we give a negative answer to this question for frustration-free systems with two-body interactions. In fact, it is shown to be impossible for any genuinely entangled qubit state to be a nondegenerate ground state of any two-body frustration-free Hamiltonian. What is more, we also prove that every spin-12\frac{1}{2}21​ frustration-free Hamiltonian with two-body interaction always has a ground state that is a product of single- or two-qubit states. In other words, there cannot be any interesting entanglement features in the ground state of such a qubit Hamiltonian.