1
views
0
recommends
+1 Recommend
0 collections
    0
    shares
      • Record: found
      • Abstract: found
      • Article: found
      Is Open Access

      Hamiltonian simulation with nearly optimal dependence on spectral norm

      Preprint

      Read this article at

      Bookmark
          There is no author summary for this article yet. Authors can add summaries to their articles on ScienceOpen to make them more accessible to a non-specialist audience.

          Abstract

          We present a quantum algorithm for approximating the real time evolution \(e^{-iHt}\) of an arbitrary \(d\)-sparse Hamiltonian to error \(\epsilon\), given black-box access to the positions and \(b\)-bit values of its non-zero matrix entries. The complexity of our algorithm is \(\mathcal{O}((t\sqrt{d}\|H\|_{1 \rightarrow 2})^{1+o(1)}/\epsilon^{o(1)})\) queries and a factor \(\mathcal{O}(b)\) more gates, which is shown to be optimal up to subpolynomial factors through a matching query lower bound. This provides a polynomial speedup in sparsity for the common case where the spectral norm \(\|H\|\ge\|H\|_{1 \rightarrow 2}\) is known, and generalizes previous approaches which achieve optimal scaling, but with respect to more restrictive parameters. By exploiting knowledge of the spectral norm, our algorithm solves the black-box unitary implementation problem -- \(\mathcal{O}(d^{1/2+o(1)})\) queries suffice to approximate any \(d\)-sparse unitary in the black-box setting, which matches the quantum search lower bound of \(\Omega(\sqrt{d})\) queries and improves upon prior art [Berry and Childs, QIP 2010] of \(\tilde{\mathcal{O}}(d^{2/3})\) queries. Combined with known techniques, we also solve systems of sparse linear equations with condition number \(\kappa\) using \(\mathcal{O}((\kappa \sqrt{d})^{1+o(1)}/\epsilon^{o(1)})\) queries, which is a quadratic improvement in sparsity.

          Related collections

          Most cited references3

          • Record: found
          • Abstract: found
          • Article: not found

          Universal Quantum Simulators

          Lloyd (1996)
          Feynman's 1982 conjecture, that quantum computers can be programmed to simulate any local quantum system, is shown to be correct.
            Bookmark
            • Record: found
            • Abstract: found
            • Article: found
            Is Open Access

            On the relationship between continuous- and discrete-time quantum walk

            (2010)
            Quantum walk is one of the main tools for quantum algorithms. Defined by analogy to classical random walk, a quantum walk is a time-homogeneous quantum process on a graph. Both random and quantum walks can be defined either in continuous or discrete time. But whereas a continuous-time random walk can be obtained as the limit of a sequence of discrete-time random walks, the two types of quantum walk appear fundamentally different, owing to the need for extra degrees of freedom in the discrete-time case. In this article, I describe a precise correspondence between continuous- and discrete-time quantum walks on arbitrary graphs. Using this correspondence, I show that continuous-time quantum walk can be obtained as an appropriate limit of discrete-time quantum walks. The correspondence also leads to a new technique for simulating Hamiltonian dynamics, giving efficient simulations even in cases where the Hamiltonian is not sparse. The complexity of the simulation is linear in the total evolution time, an improvement over simulations based on high-order approximations of the Lie product formula. As applications, I describe a continuous-time quantum walk algorithm for element distinctness and show how to optimally simulate continuous-time query algorithms of a certain form in the conventional quantum query model. Finally, I discuss limitations of the method for simulating Hamiltonians with negative matrix elements, and present two problems that motivate attempting to circumvent these limitations.
              Bookmark
              • Record: found
              • Abstract: found
              • Article: found
              Is Open Access

              Simulating sparse Hamiltonians with star decompositions

              We present an efficient algorithm for simulating the time evolution due to a sparse Hamiltonian. In terms of the maximum degree d and dimension N of the space on which the Hamiltonian H acts for time t, this algorithm uses (d^2(d+log* N)||Ht||)^{1+o(1)} queries. This improves the complexity of the sparse Hamiltonian simulation algorithm of Berry, Ahokas, Cleve, and Sanders, which scales like (d^4(log* N)||Ht||)^{1+o(1)}. To achieve this, we decompose a general sparse Hamiltonian into a small sum of Hamiltonians whose graphs of non-zero entries have the property that every connected component is a star, and efficiently simulate each of these pieces.
                Bookmark

                Author and article information

                Journal
                11 July 2018
                Article
                1807.03967
                14720017-bc72-4109-a29f-b05bd0b55ec5

                http://arxiv.org/licenses/nonexclusive-distrib/1.0/

                History
                Custom metadata
                26 pages, 2 figures
                quant-ph

                Quantum physics & Field theory
                Quantum physics & Field theory

                Comments

                Comment on this article