162 research outputs found

    Asymptotics for the number of n-quasigroups of order 4

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    The asymptotic form of the number of n-quasigroups of order 4 is 3n+122n+1(1+o(1))3^{n+1} 2^{2^n +1} (1+o(1)). Keywords: n-quasigroups, MDS codes, decomposability, reducibility.Comment: 15 p., 3 fi

    On the volumes and affine types of trades

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    A [t][t]-trade is a pair T=(T+,T−)T=(T_+, T_-) of disjoint collections of subsets (blocks) of a vv-set VV such that for every 0≤i≤t0\le i\le t, any ii-subset of VV is included in the same number of blocks of T+T_+ and of T−T_-. It follows that ∣T+∣=∣T−∣|T_+| = |T_-| and this common value is called the volume of TT. If we restrict all the blocks to have the same size, we obtain the classical tt-trades as a special case of [t][t]-trades. It is known that the minimum volume of a nonempty [t][t]-trade is 2t2^t. Simple [t][t]-trades (i.e., those with no repeated blocks) correspond to a Boolean function of degree at most v−t−1v-t-1. From the characterization of Kasami--Tokura of such functions with small number of ones, it is known that any simple [t][t]-trade of volume at most 2⋅2t2\cdot2^t belongs to one of two affine types, called Type\,(A) and Type\,(B) where Type\,(A) [t][t]-trades are known to exist. By considering the affine rank, we prove that [t][t]-trades of Type\,(B) do not exist. Further, we derive the spectrum of volumes of simple trades up to 2.5⋅2t2.5\cdot 2^t, extending the known result for volumes less than 2⋅2t2\cdot 2^t. We also give a characterization of "small" [t][t]-trades for t=1,2t=1,2. Finally, an algorithm to produce [t][t]-trades for specified tt, vv is given. The result of the implementation of the algorithm for t≤4t\le4, v≤7v\le7 is reported.Comment: 30 pages, final version, to appear in Electron. J. Combi

    Smooth optimal control with Floquet theory

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    This paper describes an approach to construct temporally shaped control pulses that drive a quantum system towards desired properties. A parametrization in terms of periodic functions with pre-defined frequencies permits to realize a smooth, typically simple shape of the pulses; their optimization can be performed based on a variational analysis with Floquet theory. As we show with selected specific examples, this approach permits to control the dynamics of interacting spins, such that gate operations and entanglement dynamics can be implemented with very high accuracy

    Robust optimal quantum gates for Josephson charge qubits

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    Quantum optimal control theory allows to design accurate quantum gates. We employ it to design high-fidelity two-bit gates for Josephson charge qubits in the presence of both leakage and noise. Our protocol considerably increases the fidelity of the gate and, more important, it is quite robust in the disruptive presence of 1/f noise. The improvement in the gate performances discussed in this work (errors of the order of 10^{-3}-10^{-4} in realistic cases) allows to cross the fault tolerance threshold.Comment: 4 pages, 4 figure

    Implementation of Fault-tolerant Quantum Logic Gates via Optimal Control

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    The implementation of fault-tolerant quantum gates on encoded logic qubits is considered. It is shown that transversal implementation of logic gates based on simple geometric control ideas is problematic for realistic physical systems suffering from imperfections such as qubit inhomogeneity or uncontrollable interactions between qubits. However, this problem can be overcome by formulating the task as an optimal control problem and designing efficient algorithms to solve it. In particular, we can find solutions that implement all of the elementary logic gates in a fixed amount of time with limited control resources for the five-qubit stabilizer code. Most importantly, logic gates that are extremely difficult to implement using conventional techniques even for ideal systems, such as the T-gate for the five-qubit stabilizer code, do not appear to pose a problem for optimal control.Comment: 18 pages, ioptex, many figure

    Errors in quantum optimal control and strategy for the search of easily implementable control pulses

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    We introduce a new approach to assess the error of control problems we aim to optimize. The method offers a strategy to define new control pulses that are not necessarily optimal but still able to yield an error not larger than some fixed a priori threshold, and therefore provide control pulses that might be more amenable for an experimental implementation. The formalism is applied to an exactly solvable model and to the Landau-Zener model, whose optimal control problem is solvable only numerically. The presented method is of importance for applications where a high degree of controllability of the dynamics of quantum systems is required.Comment: 13 pages, 3 figure

    Photon storage in Lambda-type optically dense atomic media. II. Free-space model

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    In a recent paper [Gorshkov et al., Phys. Rev. Lett. 98, 123601 (2007)], we presented a universal physical picture for describing a wide range of techniques for storage and retrieval of photon wave packets in Lambda-type atomic media in free space, including the adiabatic reduction of the photon group velocity, pulse-propagation control via off-resonant Raman techniques, and photon-echo based techniques. This universal picture produced an optimal control strategy for photon storage and retrieval applicable to all approaches and yielded identical maximum efficiencies for all of them. In the present paper, we present the full details of this analysis as well some of its extensions, including the discussion of the effects of non-degeneracy of the two lower levels of the Lambda system. The analysis in the present paper is based on the intuition obtained from the study of photon storage in the cavity model in the preceding paper [Gorshkov et al., Phys. Rev. A 76, 033804 (2007)].Comment: 26 pages, 8 figures. V2: significant changes in presentation, new references, higher resolution of figure

    On Pure Spinor Superfield Formalism

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    We show that a certain superfield formalism can be used to find an off-shell supersymmetric description for some supersymmetric field theories where conventional superfield formalism does not work. This "new" formalism contains even auxiliary variables in addition to conventional odd super-coordinates. The idea of this construction is similar to the pure spinor formalism developed by N.Berkovits. It is demonstrated that using this formalism it is possible to prove that the certain Chern-Simons-like (Witten's OSFT-like) theory can be considered as an off-shell version for some on-shell supersymmetric field theories. We use the simplest non-trivial model found in [2] to illustrate the power of this pure spinor superfield formalism. Then we redo all the calculations for the case of 10-dimensional Super-Yang-Mills theory. The construction of off-shell description for this theory is more subtle in comparison with the model of [2] and requires additional Z_2 projection. We discover experimentally (through a direct explicit calculation) a non-trivial Z_2 duality at the level of Feynman diagrams. The nature of this duality requires a better investigation

    Optimal control of atom transport for quantum gates in optical lattices

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    By means of optimal control techniques we model and optimize the manipulation of the external quantum state (center-of-mass motion) of atoms trapped in adjustable optical potentials. We consider in detail the cases of both non interacting and interacting atoms moving between neighboring sites in a lattice of a double-well optical potentials. Such a lattice can perform interaction-mediated entanglement of atom pairs and can realize two-qubit quantum gates. The optimized control sequences for the optical potential allow transport faster and with significantly larger fidelity than is possible with processes based on adiabatic transport.Comment: revised version: minor changes, 2 references added, published versio

    Quantum control theory for coupled 2-electron dynamics in quantum dots

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    We investigate optimal control strategies for state to state transitions in a model of a quantum dot molecule containing two active strongly interacting electrons. The Schrodinger equation is solved nonperturbatively in conjunction with several quantum control strategies. This results in optimized electric pulses in the THz regime which can populate combinations of states with very short transition times. The speedup compared to intuitively constructed pulses is an order of magnitude. We furthermore make use of optimized pulse control in the simulation of an experimental preparation of the molecular quantum dot system. It is shown that exclusive population of certain excited states leads to a complete suppression of spin dephasing, as was indicated in Nepstad et al. [Phys. Rev. B 77, 125315 (2008)].Comment: 24 pages, 9 figure
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