5,388 research outputs found

    Possibility of observing MSSM charged Higgs in association with a W boson at LHC

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    Possibility of observing associated production of charged Higgs and W boson in the framework of MSSM at LHC is studied. Both leptonic and hadronic decays of W boson are studied while the charged Higgs boson is considered to decay to a τ\tau lepton and a neutrino. Therefore two search categories are defined based on the leptonic and hadronic final states, i.e. ℓτ+ETmiss\ell \tau+E^{miss}_{T} and jjτ+ETmissjj \tau+E^{miss}_{T} where ℓ=e\ell=e or μ\mu and jj is a light jet from WW decay. The discovery chance of the two categories is evaluated at an integrated luminosity of 300 \invfb at LHC. It is shown that both leptonic and hadronic final states have the chance of discovery at high \tanb. Finally 5σ5\sigma and 3σ3\sigma contours are provided for both search categories.Comment: 20 pages, 19 figure

    Coherent control of multipartite entanglement

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    Quantum entanglement between an arbitrary number of remote qubits is examined analytically. We show that there is a non-probabilistic way to address in one context the management of entanglement of an arbitrary number of mixed-state qubits by engaging quantitative measures of entanglement and a specific external control mechanism. Both all-party entanglement and weak inseparability are considered. We show that for N≥4N\ge4, the death of all-party entanglement is permanent after an initial collapse. In contrast, weak inseparability can be deterministically managed for an arbitrarily large number of qubits almost indefinitely. Our result suggests a picture of the path that the system traverses in the Hilbert space

    Bounding the entanglement of N qubits with only four measurements

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    We introduce a new measure for the genuinely N-partite (all-party) entanglement of N-qubit states using the trace distance metric, and find an algebraic formula for the GHZ-diagonal states. We then use this formula to show how the all-party entanglement of experimentally produced GHZ states of an arbitrary number of qubits may be bounded with only four measurements
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