2004/07/28 by Gavin K. Brennen, Dianne P. O'Leary, Dianne P. O’Leary +1 · 87 citations
Computer Science · Mathematics · Physics and Astronomy · #Combinatorics #Discrete mathematics #Hamiltonian (control theory) #Hilbert space #Laser-Matter Interactions and Applications #Mathematical physics #Mathematics #Omega #Physics #Quantum Computing Algorithms and Architecture #Quantum Information and Cryptography #Quantum mechanics #Universality (dynamical systems) #quant-ph
paper · pdf · doi:10.1103/physreva.71.052318
published in Physical Review A 71(5) (American Physical Society) · 7 pages, 1 figure
arxiv created 2004/07/28 · openalex publication_date 2005/05/16 · arxiv updated 2009/12/01 · openalex created_date 2025/10/10 · openalex updated_date 2026/08/05
We describe criteria for implementation of quantum computation in qudits. A qudit is a -dimensional system whose Hilbert space is spanned by states \ensuremath|0⟩, \ensuremath|1⟩, …, . An important earlier work [] describes how to exactly simulate an arbitrary unitary on multiple qudits using a parameter family of single qudit and two qudit gates. That technique is based on the spectral decomposition of unitaries. Here we generalize this argument to show that exact universality follows given a discrete set of single qudit Hamiltonians and one two-qudit Hamiltonian. The technique is related to the -matrix decomposition of numerical linear algebra. We consider a generic physical system in which the single qudit Hamiltonians are a small collection of and . A coupling graph results taking nodes 0, …, and edges are allowed Hamiltonians. One qudit exact universality follows iff this graph is connected, and complete universality results if the two-qudit Hamiltonian is also allowed. We discuss implementation in the eight dimensional ground electronic states of and construct an optimal gate sequence using Raman laser pulses.