4,622 research outputs found

    Study of the K1(1270)βˆ’K1(1400)K_1(1270)-K_1(1400) mixing in the decays Bβ†’J/Ξ¨K1(1270),J/Ξ¨K1(1400)B\to J/\Psi K_1(1270), J/\Psi K_1(1400)

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    We studied the B meson decays Bβ†’J/Ξ¨K1(1270,1400)B\to J/\Psi K_1(1270,1400) in the pQCD approach beyond the leading order. With the vertex corrections and the NLO Wilson coefficients included, the branching ratios of the considered decays are Br(B+β†’J/Ξ¨K1(1270)+)=1.76βˆ’0.69+0.65Γ—10βˆ’3,Br(B+β†’J/Ξ¨K1(1400)+)=7.03βˆ’2.52+2.70Γ—10βˆ’4Br(B^+\to J/\Psi K_1(1270)^+)=1.76^{+0.65}_{-0.69}\times10^{-3}, Br(B^+\to J/\Psi K_1(1400)^+)=7.03^{+2.70}_{-2.52}\times10^{-4}, and Br(B0β†’J/Ξ¨K1(1270)0)=(1.63βˆ’0.64+0.60)Γ—10βˆ’3Br(B^0\to J/\Psi K_1(1270)^0)=(1.63^{+0.60}_{-0.64})\times10^{-3} with the mixing angle ΞΈK1=33∘\theta_{K_1}=33^\circ, which can agree well with the data or the present experimental upper limit within errors. So we support the opinion that ΞΈK1∼33∘\theta_{K_1}\sim33^\circ is much more favored than 58∘58^{\circ}. Furthermore, we also give the predictions for the polarization fractions, direct CP violations from the different polarization components, the relative phase angles for the considered decays with the mixing angle ΞΈK1=33∘\theta_{K_1}=33^\circ and 58∘58^\circ, respectively. The direct CP violations of the two charged decays B+β†’J/Ξ¨K1(1270,1400)+B^+\to J/\Psi K_1(1270,1400)^+ are very small (10βˆ’4∼10βˆ’5)(10^{-4}\sim10^{-5}), because there is no weak phase until up to O(Ξ»4)\mathcal{O}(\lambda^4) with the Wolfenstein parameter Ξ»=0.22537\lambda=0.22537. These results can be tested at the running LHCb and forthcoming Super-B experiments.Comment: 14 pages,3 figures,to appear in EPJ

    Associated production of the heavy charged gauge boson WH{W_{H}} and a top quark at LHC

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    In the context of topflavor seesaw model, we study the production of the heavy charged gauge boson WH{W_{H}} associated with a top quark at the LHC. Focusing on the searching channel ppβ†’tWHβ†’ttΛ‰bβ†’lΞ½jjbbbpp\rightarrow tW_H\rightarrow t\bar{t}b \rightarrow l\nu jjbbb, we carry out a full simulation of the signal and the relevant standard model backgrounds. The kinematical distributions of final states are presented. It is found that the backgrounds can be significantly suppressed by sets of kinematic cuts, and the signal of the heavy charged boson might be detected at the LHC with s=14\sqrt{s}=14 TeV. With a integrated luminosity of \LL= 100 fbβˆ’1fb^{-1}, a 8.3Οƒ8.3 \sigma signal significance can be achieved for mWH=1.6m_{W_H}=1.6 TeV.Comment: 16 pages, 6 figure

    Management of duodenal trauma

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    AbstractDuodenal trauma is uncommon but nowadays seen more and more frequently due to the increased automobile accidents and violent events. The management of duodenal trauma can be complicated, especially when massive injury to the pancreatic-duodenal-biliary complex occurs simultaneously. Even the patients receive surgeries in time, multiple postoperative complications and high mortality are common. To know and manage duodenal trauma better, we searched the recent related literature in PubMed by the keywords of duodenal trauma, therapy, diagnosis and abdomen. It shows that because the diagnosis and management are complicated and the mortality is high, duodenal trauma should be treated in time and tactfully. And application of new technology can help improve the management. In this review, we discussed the incidence, diagnosis, management, and complications as well as mortality of duodenal trauma
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