372 research outputs found

    Quantum measurements and the Abelian Stabilizer Problem

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    We present a polynomial quantum algorithm for the Abelian stabilizer problem which includes both factoring and the discrete logarithm. Thus we extend famous Shor's results. Our method is based on a procedure for measuring an eigenvalue of a unitary operator. Another application of this procedure is a polynomial quantum Fourier transform algorithm for an arbitrary finite Abelian group. The paper also contains a rather detailed introduction to the theory of quantum computation.Comment: 22 pages, LATE

    Exact results for spin dynamics and fractionization in the Kitaev Model

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    We present certain exact analytical results for dynamical spin correlation functions in the Kitaev Model. It is the first result of its kind in non-trivial quantum spin models. The result is also novel: in spite of presence of gapless propagating Majorana fermion excitations, dynamical two spin correlation functions are identically zero beyond nearest neighbor separation, showing existence of a gapless but short range spin liquid. An unusual, \emph{all energy scale fractionization}of a spin -flip quanta, into two infinitely massive π\pi-fluxes and a dynamical Majorana fermion, is shown to occur. As the Kitaev Model exemplifies topological quantum computation, our result presents new insights into qubit dynamics and generation of topological excitations.Comment: 4 pages, 2 figures. Typose corrected, figure made better, clarifying statements and references adde

    Connection Formulae for Asymptotics of Solutions of the Degenerate Third Painlev\'{e} Equation. I

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    The degenerate third Painlev\'{e} equation, u=(u)2uuτ+1τ(8ϵu2+2ab)+b2uu^{\prime \prime} = \frac{(u^{\prime})^{2}}{u} - \frac{u^{\prime}}{\tau} + \frac{1}{\tau}(-8 \epsilon u^{2} + 2ab) + \frac{b^{2}}{u}, where ϵ,bR\epsilon,b \in \mathbb{R}, and aCa \in \mathbb{C}, and the associated tau-function are studied via the Isomonodromy Deformation Method. Connection formulae for asymptotics of the general as τ±0\tau \to \pm 0 and ±i0\pm i0 solution and general regular as τ±\tau \to \pm \infty and ±i\pm i \infty solution are obtained.Comment: 40 pages, LaTeX2

    Zeta functions and Dynamical Systems

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    In this brief note we present a very simple strategy to investigate dynamical determinants for uniformly hyperbolic systems. The construction builds on the recent introduction of suitable functional spaces which allow to transform simple heuristic arguments in rigorous ones. Although the results so obtained are not exactly optimal the straightforwardness of the argument makes it noticeable.Comment: 7 pages, no figuer

    Decoherence Free Subspace and entanglement by interaction with a common squeezed bath

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    In this work we find explicitly the decoherence free subspace (DFS) for a two two-level system in a common squeezed vacuum bath. We also find an orthogonal basis for the DFS composed of a symmetrical and an antisymmetrical (under particle permutation) entangled state. For any initial symmetrical state, the master equation has one stationary state which is the symmetrical entangled decoherence free state. In this way, one can generate entanglement via common squeezed bath of the two systems. If the initial state does not have a definite parity, the stationary state depends strongly on the initial conditions of the system and it has a statistical mixture of states which belong to the DFS. We also study the effect of the coupling between the two-level systems on the DFS.Comment: 4 pages, 1 figur

    Lattice model of three-dimensional topological singlet superconductor with time-reversal symmetry

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    We study topological phases of time-reversal invariant singlet superconductors in three spatial dimensions. In these particle-hole symmetric systems the topological phases are characterized by an even-numbered winding number ν\nu. At a two-dimensional (2D) surface the topological properties of this quantum state manifest themselves through the presence of ν\nu flavors of gapless Dirac fermion surface states, which are robust against localization from random impurities. We construct a tight-binding model on the diamond lattice that realizes a topologically nontrivial phase, in which the winding number takes the value ν=±2\nu =\pm 2. Disorder corresponds to a (non-localizing) random SU(2) gauge potential for the surface Dirac fermions, leading to a power-law density of states ρ(ϵ)ϵ1/7\rho(\epsilon) \sim \epsilon^{1/7}. The bulk effective field theory is proposed to be the (3+1) dimensional SU(2) Yang-Mills theory with a theta-term at θ=π\theta=\pi.Comment: 5 pages, 3 figure

    Fault-tolerant quantum computation by anyons

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    A two-dimensional quantum system with anyonic excitations can be considered as a quantum computer. Unitary transformations can be performed by moving the excitations around each other. Measurements can be performed by joining excitations in pairs and observing the result of fusion. Such computation is fault-tolerant by its physical nature
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