33,615 research outputs found

    Optimal control of a leaking qubit

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    Physical implementations of quantum bits can contain coherent transitions to energetically close non-qubit states. In particular, for anharmonic oscillator systems such as the superconducting phase qubit and the transmon a two-level approximation is insufficient. We apply optimal control theory to the envelope of a resonant Rabi pulse in a qubit in the presence of a single, weakly off-resonant leakage level. The gate error of a spin flip operation reduces by orders of magnitude compared to simple pulse shapes. Near-perfect gates can be achieved for any pulse duration longer than an intrinsic limit given by the nonlinearity. The pulses can be understood as composite sequences that refocus the leakage transition. We also discuss ways to improve the pulse shapes.Comment: 4 pages, 2 figure

    On the energy dependence of the D^+/D^- production asymmetry

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    In this paper we discuss the origin of the asymmetry present in D meson production and its energy dependence. In particular, we have applied the meson cloud model to calculate the asymmetries in D^-/D^+ meson production in high energy p-p collisions and find a good agreement with recent LHCb data. Although small, this non-vanishing asymmetry may shed light on the role played by the charm meson cloud of the proton.Comment: 8 pages, 8 figures. arXiv admin note: text overlap with arXiv:hep-ph/000927

    Trace functions as Laplace transforms

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    We study trace functions on the form t\to\tr f(A+tB) where f f is a real function defined on the positive half-line, and A A and B B are matrices such that A A is positive definite and B B is positive semi-definite. If f f is non-negative and operator monotone decreasing, then such a trace function can be written as the Laplace transform of a positive measure. The question is related to the Bessis-Moussa-Villani conjecture. Key words: Trace functions, BMV-conjecture.Comment: Minor change of style, update of referenc

    Magic state distillation with low overhead

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    We propose a new family of error detecting stabilizer codes with an encoding rate 1/3 that permit a transversal implementation of the pi/8-rotation TT on all logical qubits. The new codes are used to construct protocols for distilling high-quality `magic' states T+>T|+> by Clifford group gates and Pauli measurements. The distillation overhead has a poly-logarithmic scaling as a function of the output accuracy, where the degree of the polynomial is log231.6\log_2{3}\approx 1.6. To construct the desired family of codes, we introduce the notion of a triorthogonal matrix --- a binary matrix in which any pair and any triple of rows have even overlap. Any triorthogonal matrix gives rise to a stabilizer code with a transversal TT-gate on all logical qubits, possibly augmented by Clifford gates. A powerful numerical method for generating triorthogonal matrices is proposed. Our techniques lead to a two-fold overhead reduction for distilling magic states with output accuracy 101210^{-12} compared with the best previously known protocol.Comment: 11 pages, 3 figure

    Study of the DρD^*\rho system using QCD sum rules

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    In this talk I present a study of the DρD^* \rho system made by using the method of QCD sum rules. Considering isospin and spin projectors, we investigate the different configurations and obtain three DD^* mesons with isospin I=1/2I=1/2, spin S=0S=0, 11, 22 and with masses 2500±672500\pm 67 MeV, 2523±602523\pm60 MeV, and 2439±1192439\pm119 MeV, respectively. The last state can be related to D2(2460)D^*_2(2460) (spin 2) listed by the Particle Data Group, while one of the first two might be associated with D(2640)D^*(2640), whose spin-parity is unknown. In the case of I=3/2I=3/2 we also find evidences of three states with spin 0, 1 and 2, respectively, with masses 2467±822467\pm82 MeV, 2420±1282420\pm128 MeV, and 2550±562550\pm56 MeV.Comment: Contribution to the proceedings of the XXXVI Reuni\~ao de Trabalho sobre F\'isica Nuclear no Brasil, Maresias, S\~ao Paulo, Brazi

    Quantum-dot-spin single-photon interface

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    Using background-free detection of spin-state-dependent resonance fluorescence from a single-electron charged quantum dot with an efficiency of 0:1%, we realize a single spin-photon interface where the detection of a scattered photon with 300 picosecond time resolution projects the quantum dot spin to a definite spin eigenstate with fidelity exceeding 99%. The bunching of resonantly scattered photons reveals information about electron spin dynamics. High-fidelity fast spin-state initialization heralded by a single photon enables the realization of quantum information processing tasks such as non-deterministic distant spin entanglement. Given that we could suppress the measurement back-action to well below the natural spin-flip rate, realization of a quantum non-demolition measurement of a single spin could be achieved by increasing the fluorescence collection efficiency by a factor exceeding 20 using a photonic nanostructure

    A study of the KNKN-KNK^*N coupled systems

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    We study the strangeness +1+1 meson-baryon systems to obtain improved KNKN and KNK^*N amplitudes and to look for a possible resonance formation by the KNKN-KNK^*N coupled interaction. We obtain amplitudes for light vector meson-baryon systems by implementing the ss-, tt-, uu- channel diagrams and a contact interaction. The pseudoscalar meson-baryon interactions are obtained by relying on the Weinberg-Tomozawa theorem. The transition amplitudes between the systems consisting of pseudoscalars and vector mesons are calculated by extending the Kroll-Ruderman term for pion photoproduction replacing the photon by a vector meson. We fix the subtraction constants required to calculate the loops by fitting our KNKN amplitudes to the data available for the isospin 0 and 1 ss-wave phase shifts. We provide the scattering lengths and the total cross sections for the KNKN and KNK^* N systems obtained in our model, which can be useful in future in-medium calculations. Our amplitudes do not correspond to formation of any resonance in none of the isospin and spin configurations.Comment: Published version, sent to avoid confusions recently noticed by author
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