39 research outputs found

    Average Fidelity in n-Qubit systems

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    This letter generalizes the expression for the average fidelity of single qubits, as found by Bowdrey et al., to the case of n qubits. We use a simple algebraic approach with basis elements for the density-matrix expansion expressed as Kronecker products of n Pauli spin matrices. An explicit integration over initial states is avoided by invoking the invariance of the state average under unitary transformations of the initial density matrix. The results have applications to measurements of quantum information, for example in ion-trap and NMR experiments.Comment: 4 pages, no figures. Revision includes additional references and a more detailed symmetry argumen

    Compiling gate networks on an Ising quantum computer

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    Here we describe a simple mechanical procedure for compiling a quantum gate network into the natural gates (pulses and delays) for an Ising quantum computer. The aim is not necessarily to generate the most efficient pulse sequence, but rather to develop an efficient compilation algorithm that can be easily implemented in large spin systems. The key observation is that it is not always necessary to refocus all the undesired couplings in a spin system. Instead the coupling evolution can simply be tracked and then corrected at some later time. Although described within the language of NMR the algorithm is applicable to any design of quantum computer based on Ising couplings.Comment: 5 pages RevTeX4 including 4 figures. Will submit to PR

    The distribution of quantum fidelities

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    When applied to different input states, an imperfect quantum operation yields output states with varying fidelities, defined as the absolute square of their overlap with the desired states. We present an expression for the distribution of fidelities for a class of operations applied to a general qubit state, and we present general expressions for the variance and input-space averaged fidelities of arbitrary linear maps on finite dimensional Hilbert spaces.Comment: 5 pages, 1 figur

    Fidelity of quantum operations

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    We present a derivation and numerous applications of a compact explicit formula for the average fidelity of a quantum operation on a finite dimensional quantum system. The formula can be applied to averages over particularly relevant subspaces; it is easily generalized to multi-component systems, and as a special result, we show that when the same completely positive trace-preserving map is applied to a large number of qubits with one-bit fidelity F close to unity, the average fidelity of the operation on the full K-bit register scales as F3K/2F^{3K/2}.Comment: 5 pages, no figures. The text has been modified to acknowledge that our Eq.(1) has appeared already in quant-ph/0503243 and quant-ph/051221

    Minimal measurements of the gate fidelity of a qudit map

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    We obtain a simple formula for the average gate fidelity of a linear map acting on qudits. It is given in terms of minimal sets of pure state preparations alone, which may be interesting from the experimental point of view. These preparations can be seen as the outcomes of certain minimal positive operator valued measures. The connection of our results with these generalized measurements is briefly discussed

    Effect of noise on geometric logic gates for quantum computation

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    We introduce the non-adiabatic, or Aharonov-Anandan, geometric phase as a tool for quantum computation and show how it could be implemented with superconducting charge qubits. While it may circumvent many of the drawbacks related to the adiabatic (Berry) version of geometric gates, we show that the effect of fluctuations of the control parameters on non-adiabatic phase gates is more severe than for the standard dynamic gates. Similarly, fluctuations also affect to a greater extent quantum gates that use the Berry phase instead of the dynamic phase.Comment: 8 pages, 4 figures; published versio

    Single qubit gates by selective excitation with Jump and Return sequences

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    We discuss the implementation of frequency selective rotations using sequences of hard pulses and delays. These rotations are suitable for implementing single qubit gates in Nuclear Magnetic Resonance (NMR) quantum computers, but can also be used in other related implementations of quantum computing. We also derive methods for implementing hard pulses in the presence of moderate off-resonance effects, and describe a simple procedure for implementing a hard 180 degree rotation in a two spin system. Finally we show how these two approaches can be combined to produce more accurate frequency selective rotations.Comment: Revised and extended at request of referee; now in press at Physical Review A. 6 pages RevTex including 3 figure

    State transfer in dissipative and dephasing environments

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    By diagonalization of a generalized superoperator for solving the master equation, we investigated effects of dissipative and dephasing environments on quantum state transfer, as well as entanglement distribution and creation in spin networks. Our results revealed that under the condition of the same decoherence rate γ\gamma, the detrimental effects of the dissipative environment are more severe than that of the dephasing environment. Beside this, the critical time tct_c at which the transfer fidelity and the concurrence attain their maxima arrives at the asymptotic value t0=π/2λt_0=\pi/2\lambda quickly as the spin chain length NN increases. The transfer fidelity of an excitation at time t0t_0 is independent of NN when the system subjects to dissipative environment, while it decreases as NN increases when the system subjects to dephasing environment. The average fidelity displays three different patterns corresponding to N=4r+1N=4r+1, N=4r1N=4r-1 and N=2rN=2r. For each pattern, the average fidelity at time t0t_0 is independent of rr when the system subjects to dissipative environment, and decreases as rr increases when the system subjects to dephasing environment. The maximum concurrence also decreases as NN increases, and when NN\rightarrow\infty, it arrives at an asymptotic value determined by the decoherence rate γ\gamma and the structure of the spin network.Comment: 12 pages, 6 figure
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