4,124 research outputs found

    Cosmic e^\pm, \bar p, \gamma and neutrino rays in leptocentric dark matter models

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    Dark matter annihilation is one of the leading explanations for the recently observed eΒ±e^\pm excesses in cosmic rays by PAMELA, ATIC, FERMI-LAT and HESS. Any dark matter annihilation model proposed to explain these data must also explain the fact that PAMELA data show excesses only in eΒ±e^\pm spectrum but not in anti-proton. It is interesting to ask whether the annihilation mode into anti-proton is completely disallowed or only suppressed at low energies. Most models proposed have negligible anti-protons in all energy ranges. We show that the leptocentric U(1)Bβˆ’3LiU(1)_{B-3L_i} dark matter model can explain the eΒ±e^\pm excesses with suppressed anti-proton mode at low energies, but at higher energies there are sizable anti-proton excesses. Near future data from PAMELA and AMS can provide crucial test for this type of models. Cosmic Ξ³\gamma ray data can further rule out some of the models. We also show that this model has interesting cosmic neutrino signatures.Comment: Latex 20 pages and five figures. References adde

    Quasi-two-body decays Bβ†’Ξ·c(1S,2S)β€…β€Š[ρ(770),ρ(1450),ρ(1700)β†’]β€…β€ŠΟ€Ο€B \to \eta_c {(1S ,2S)}\;[\rho(770),\rho(1450),\rho(1700) \to ]\; \pi\pi in the perturbative QCD approach

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    In this paper, we calculated the branching ratios of the quasi-two-body decays Bβ†’Ξ·c(1S,2S)B \to \eta_c (1S ,2S) [ρ(770),ρ(1450),ρ(1700)β†’]ππ[\rho(770), \rho(1450),\rho(1700)\to ] \pi\pi by employing the perturbative QCD (PQCD) approach. The contributions from the PP-wave resonances ρ(770)\rho(770), ρ(1450)\rho(1450) and ρ(1700)\rho(1700) were taken into account. The two-pion distribution amplitude ΦππP\Phi_{\pi\pi}^{\rm P} is parameterized by the vector current time-like form factor FΟ€F_{\pi} to study the considered decay modes. We found that (a) the PQCD predictions for the branching ratios of the considered quasi-two-body decays are in the order of 10βˆ’7∼10βˆ’610^{-7} \sim 10^{-6}, while the two-body decay rates B(Bβ†’Ξ·c(1S,2S)(ρ(1450),ρ(1700))){\cal B}(B \to \eta_c{(1S,2S)} (\rho(1450),\rho(1700))) are extracted from those for the corresponding quasi-two-body decays; (b) the whole pattern of the pion form factor-squared ∣FΟ€βˆ£2|F_\pi|^2 measured by the BABAR Collaboration could be understood based on our theoretical results; (c) the general expectation based on the similarity between Bβ†’Ξ·cππB \to \eta_c \pi\pi and Bβ†’J/ΟˆΟ€Ο€B \to J/\psi \pi\pi decays are confirmed: R2(Ξ·c)β‰ˆ0.45R_2(\eta_c)\approx 0.45 is consistent with the measured R2(J/ψ)β‰ˆ0.56Β±0.09R_2(J/\psi)\approx 0.56\pm 0.09 within errors; and (d) new ratios R3(Ξ·c(1S))R_3(\eta_c(1S)) and R4(Ξ·c(2S))R_4(\eta_c(2S)) among the branching ratios of the considered decay modes are defined and could be tested by future experiments.Comment: 10 pages, 3 figure

    Quasi-two-body decays Bβ†’DKβˆ—(892)β†’DKΟ€B \to D K^*(892) \to D K \pi in the perturbative QCD approach

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    We study the quasi-two-body decays Bβ†’DKβˆ—(892)β†’DKΟ€B\to D K^*(892) \to D K\pi by employing the perturbative QCD approach. The two-meson distribution amplitudes \Phi_{K\pi}^{\text{P-wave}} are adopted to describe the final state interactions of the kaon-pion pair in the resonance region. The resonance line shape for the PP-wave KΟ€K\pi component Kβˆ—(892)K^*(892) in the time-like form factor FKΟ€(s)F_{K\pi}(s) is parameterized by the relativistic Breit-Wigner function. For most considered decay modes, the theoretical predictions for their branching ratios are consistent with currently available experimental measurements within errors. We also disscuss some ratios of the branching fractions of the concerned decay processes. More precise data from LHCb and Belle-II are expected to test our predictions.Comment: 10 pages, 3 figures and 2 tables.To be published in EPJ

    Pyrogen reaction and conversion of sustained ventricular tachycardia to sinus rhythm: two case reports

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    INTRODUCTION: Pyrogen reaction is a side effect of intravenous infusion of solution on body; sustained ventricular tachycardia is a serious arrhythmia, no relationship between them has been reported before. CASE PRESENTATION: Two patients with sustained ventricular tachycardia refractory to lidocaine happened to have pyrogen reaction. The sustained ventricular tachycardia was converted to sinus rhythm after the pyrogen reaction. CONCLUSION: The conversion of sustained ventricular tachycardia might be related to pyrogen reaction. The effects of pyrogen reaction on sustained ventricular tachycardia need further research

    Superposition coded modulation with peak-power limitation

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    We apply clipping to superposition coded modulation (SCM) systems to reduce the peak-to-average power ratio (PAPR) of the transmitted signal. The impact on performance is investigated by evaluating the mutual information driven by the induced peak-power-limited input signals. It is shown that the rate loss is marginal for moderate clipping thresholds if optimal encoding/decoding is used. This fact is confirmed in examples where capacityapproaching component codes are used together with the maximum a posteriori probability (MAP) detection. In order to reduce the detection complexity of SCM with a large number of layers, we develop a suboptimal soft compensation (SC) method that is combined with soft-input soft-output (SISO) decoding algorithms in an iterative manner. A variety of simulation results for additive white Gaussian noise (AWGN) and fading channels are presented. It is shown that with the proposed method, the effect of clipping can be efficiently compensated and a good tradeoff between PAPR and bit-error rate (BER) can be achieved. Comparisons with other coded modulation schemes demonstrate that SCM offers significant advantages for high-rate transmissions over fading channels
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