336 research outputs found

    The productions of the top-pions and top-Higgs associated with the charm quark at the hadron colliders

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    In the topcolor-assistant technicolor (TC2) model, the typical physical particles, top-pions and top-Higgs, are predicted and the existence of these particles could be regarded as the robust evidence of the model. These particles are accessible at the Tevatron and LHC, and furthermore the flavor-changing(FC) feature of the TC2 model can provide us a unique chance to probe them. In this paper, we study some interesting FC production processes of top-pions and top-Higgs at the Tevatron and LHC, i.e., cΞ tβˆ’c\Pi_{t}^{-} and cΞ t0(ht0)c\Pi_{t}^{0}(h_{t}^{0}) productions. We find that the light charged top-pions are not favorable by the Tevatron experiments and the Tevatron has a little capability to probe neutral top-pion and top-Higgs via these FC production processes. At the LHC, however, the cross section can reach the level of 10∼10010\sim 100 pb for cΞ tβˆ’c\Pi_t^- production and 10∼100 10\sim 100 fb for cΞ t0(ht0)c\Pi_t^0(h_t^0) production. So one can expect that enough signals could be produced at the LHC experiments. Furthermore, the SM background should be clean due to the FC feature of the processes and the FC decay modes Ξ tβˆ’β†’bcΛ‰,Ξ t0(ht0)β†’tcΛ‰\Pi_t^-\to b\bar{c}, \Pi_t^0(h_t^0)\to t\bar{c} can provide us the typical signal to detect the top-pions and top-Higgs. Therefore, it is hopeful to find the signal of top-pions and top-Higgs with the running of the LHC via these FC processes.Comment: 12 pages, 6 figure

    RevisiΓ³n sobre mΓ©todos de preparaciΓ³n, mecanismos y aplicaciones de pΓ©ptidos antioxidantes en aceites

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    Natural antioxidants, especially those used in edible oil, are safer compared to chemically synthesized antioxidants. Therefore, research on natural antioxidants has become prevelant. Antioxidant peptides derived from food protein can effectively prevent oil oxidation. Protein hydrolyzation is widely applied for the production of antioxidant peptides in industry, and bioinformatics is employed nowadays to generate the desired peptide sequence. Furthermore, the mechanism of antioxidant peptides in the oil system is still controversial, which limits the further development of antioxidant peptides as food antioxidants. This review introduces the preparation method of antioxidant peptides and their mechanisms as well as applications in the oil. It will help to comprehensively understand the function of antioxidant peptides and promote their development in the oil field.Los antioxidantes naturales, especialmente utilizados en aceites comestibles, son mΓ‘s seguros en comparaciΓ³n con los antioxidantes sintetizados quΓ­micamente. Por lo tanto, la investigaciΓ³n sobre antioxidantes naturales se convierte en un punto de interΓ©s. Los pΓ©ptidos antioxidantes derivados de las proteΓ­nas alimentarias pueden prevenir eficazmente la oxidaciΓ³n del aceite. La hidrolizaciΓ³n de proteΓ­nas se usa ampliamente en la industria para la producciΓ³n de pΓ©ptidos antioxidantes y la bioinformΓ‘tica se emplea hoy en dΓ­a para generar la secuencia de pΓ©ptidos deseada. AdemΓ‘s, el mecanismo de los pΓ©ptidos antioxidantes en el sistema oleoso sigue siendo controvertido, lo que limita el desarrollo posterior de pΓ©ptidos antioxidantes como antioxidantes alimentarios. Esta revisiΓ³n presenta el mΓ©todo de preparaciΓ³n de pΓ©ptidos antioxidantes y su mecanismo, asΓ­ como las aplicaciones en aceite, lo que ayudarΓ‘ a comprender de manera integral la funciΓ³n de los pΓ©ptidos antioxidantes y promoverΓ‘ su desarrollo en el campo petrolero

    The rare top quark decays t→cVt\to cV in the topcolor-assisted technicolor model

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    We consider the rare top quark decays in the framework of topcolor-assisted technicolor (TC2) model. We find that the contributions of top-pions and top-Higgs predicted by the TC2 model can enhance the SM branching ratios by as much as 6-9 orders of magnitude. i.e., in the most case, the orders of magnitude of branching ratios are Br(tβ†’cg)∼10βˆ’5Br(t\to c g)\sim 10^{-5}, Br(tβ†’cZ)∼10βˆ’5Br(t\to c Z)\sim 10^{-5}, Br(tβ†’cΞ³)∼10βˆ’7Br(t\to c \gamma)\sim 10^{-7}. With the reasonable values of the parameters in TC2 model, such rare top quark decays may be testable in the future experiments. So, rare top quark decays provide us a unique way to test TC2 model.Comment: 14 pages, 4 figure

    First Report of Alternaria Black Spot Disease Caused by Alternaria alternata on the Invasive Weed Solanum rostratum in Xinjiang, China

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    Solanum rostratum is a noxious weed, native to Mexico and the USA, which has invaded Liaoning, Jilin, Hebei, Inner Mongolia, Shanxi, Xinjiang and Beijing, China (Eminniya et al., 2013). In August 2015, foliar symptoms of yellowish to black spots were observed on plants of S. rostratum nearby an agricultural plantation in Changji, Xinjiang. The following year, about 17% of the 206 plants surveyed on about 0.2 ha of deserted farmland were infected from July-September (at 19-35Β°C under 29-97% RH)

    The flavor-changing bottom-strange quark production in the littlest Higgs model with T parity at the ILC

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    In the littlest Higgs model with T-parity (LHT) the mirror quarks induce the special flavor structures and some new flavor-changing (FC) couplings which could greatly enhance the production rates of the FC processes. We in this paper study some bottom and anti-strange production processes in the LHT model at the International Linear Collider (ILC), i.e., e+eβˆ’β†’bsΛ‰e^+e^-\rightarrow b\bar{s} and Ξ³Ξ³β†’bsΛ‰\gamma\gamma\rightarrow b\bar{s}. The results show that the production rates of these processes are sizeable for the favorable values of the parameters. Therefore, it is quite possible to test the LHT model or make some constrains on the relevant parameters of the LHT through the detection of these processes at the ILC.Comment: 12 pages, 8 figure

    Transgenic and Knockout Mice Models to Reveal the Functions of Tumor Suppressor Genes

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    Cancer is caused by multiple genetic alterations leading to uncontrolled cell proliferation through multiple pathways. Malignant cells arise from a variety of genetic factors, such as mutations in tumor suppressor genes (TSGs) that are involved in regulating the cell cycle, apoptosis, or cell differentiation, or maintenance of genomic integrity. Tumor suppressor mouse models are the most frequently used animal models in cancer research. The anti-tumorigenic functions of TSGs, and their role in development and differentiation, and inhibition of oncogenes are discussed. In this review, we summarize some of the important transgenic and knockout mouse models for TSGs, including Rb, p53, Ink4a/Arf, Brca1/2, and their related genes

    Probing Topcolor-Assisted Technicolor from Top-Charm Associated Production at LHC

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    We propose to probe the topcolor-assisted technicolor (TC2) model from the top-charm associated productions at the LHC, which are highly suppressed in the Standard Model. Due to the flavor-changing couplings of the top quark with the scalars (top-pions and top-Higgs) in TC2 model, the top-charm associated productions can occur via both the s-channel and t-channel parton processes by exchanging a scalar field at the LHC. We examined these processes through Monte Carlo simulation and found that they can reach the observable level at the LHC in quite a large part of the parameter space of the TC2 model.Comment: Version to appear in PRD (Rapid Communication

    Partial wave analysis of J/\psi \to \gamma \phi \phi

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    Using 5.8Γ—107J/ψ5.8 \times 10^7 J/\psi events collected in the BESII detector, the radiative decay J/Οˆβ†’Ξ³Ο•Ο•β†’Ξ³K+Kβˆ’KS0KL0J/\psi \to \gamma \phi \phi \to \gamma K^+ K^- K^0_S K^0_L is studied. The ϕϕ\phi\phi invariant mass distribution exhibits a near-threshold enhancement that peaks around 2.24 GeV/c2c^{2}. A partial wave analysis shows that the structure is dominated by a 0βˆ’+0^{-+} state (Ξ·(2225)\eta(2225)) with a mass of 2.24βˆ’0.02+0.03βˆ’0.02+0.032.24^{+0.03}_{-0.02}{}^{+0.03}_{-0.02} GeV/c2c^{2} and a width of 0.19Β±0.03βˆ’0.04+0.060.19 \pm 0.03^{+0.06}_{-0.04} GeV/c2c^{2}. The product branching fraction is: Br(J/Οˆβ†’Ξ³Ξ·(2225))β‹…Br(Ξ·(2225)→ϕϕ)=(4.4Β±0.4Β±0.8)Γ—10βˆ’4Br(J/\psi \to \gamma \eta(2225))\cdot Br(\eta(2225)\to \phi\phi) = (4.4 \pm 0.4 \pm 0.8)\times 10^{-4}.Comment: 11 pages, 4 figures. corrected proof for journa

    Measurements of the observed cross sections for e+eβˆ’β†’e^+e^-\to exclusive light hadrons containing Ο€0Ο€0\pi^0\pi^0 at s=3.773\sqrt s= 3.773, 3.650 and 3.6648 GeV

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    By analyzing the data sets of 17.3, 6.5 and 1.0 pbβˆ’1^{-1} taken, respectively, at s=3.773\sqrt s= 3.773, 3.650 and 3.6648 GeV with the BES-II detector at the BEPC collider, we measure the observed cross sections for e+eβˆ’β†’Ο€+Ο€βˆ’Ο€0Ο€0e^+e^-\to \pi^+\pi^-\pi^0\pi^0, K+Kβˆ’Ο€0Ο€0K^+K^-\pi^0\pi^0, 2(Ο€+Ο€βˆ’Ο€0)2(\pi^+\pi^-\pi^0), K+Kβˆ’Ο€+Ο€βˆ’Ο€0Ο€0K^+K^-\pi^+\pi^-\pi^0\pi^0 and 3(Ο€+Ο€βˆ’)Ο€0Ο€03(\pi^+\pi^-)\pi^0\pi^0 at the three energy points. Based on these cross sections we set the upper limits on the observed cross sections and the branching fractions for ψ(3770)\psi(3770) decay into these final states at 90% C.L..Comment: 7 pages, 2 figure
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