20,360 research outputs found

    Strong decays of DsJ(2317)D_{sJ}(2317) and DsJ(2460)D_{sJ}(2460)

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    With the identification of (DsJ(2317),DsJ(2460)D_{sJ}(2317), D_{sJ}(2460)) as the (0+0^+, 1+1^+) doublet in the heavy quark effective field theory, we derive the light cone QCD sum rule for the coupling of eta meson with DsJ(2317)DsD_{sJ}(2317) D_s and DsJ(2460)Dsβˆ—D_{sJ}(2460) D_s^{*} . Through Ξ·βˆ’Ο€0\eta-\pi^0 mixing we calculate their pionic decay widths, which are consistent with the experimental values (or upper limits). Combining the radiative decay widths derived by Colangelo, Fazio and Ozpineci in the same framework, we conclude that the decay patterns of DsJ(2317,2460)D_{sJ}(2317, 2460) strongly support their interpretation as ordinary csΛ‰c \bar s mesons.Comment: Comments and suggestions welcome

    Quantum state engineering with flux-biased Josephson phase qubits by Stark-chirped rapid adiabatic passages

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    In this paper, the scheme of quantum computing based on Stark chirped rapid adiabatic passage (SCRAP) technique [L. F. Wei et al., Phys. Rev. Lett. 100, 113601 (2008)] is extensively applied to implement the quantum-state manipulations in the flux-biased Josephson phase qubits. The broken-parity symmetries of bound states in flux-biased Josephson junctions are utilized to conveniently generate the desirable Stark-shifts. Then, assisted by various transition pulses universal quantum logic gates as well as arbitrary quantum-state preparations could be implemented. Compared with the usual PI-pulses operations widely used in the experiments, the adiabatic population passage proposed here is insensitive the details of the applied pulses and thus the desirable population transfers could be satisfyingly implemented. The experimental feasibility of the proposal is also discussed.Comment: 9 pages, 4 figure
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