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    UMNH:Mamm:4160

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    UMNH:Mamm:4160 Voucher specimen study ski

    Interpretations for the X(4160) observed in the double charm production at B factories

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    AbstractBelle Collaboration has recently observed a new state, the X(4160), in the process of double charm production e+e−→J/ψ+X(4160) followed by X(4160)→D∗D¯∗. We discuss possible interpretations for the X(4160) based on the NRQCD calculations and the potential model estimates for the charmonium spectrum. We first focus on the D-wave spin-singlet 2−+ charmonium D21(2D), which is estimated to have a small production rate of about 5% of that for e+e−→J/ψ+ηc(1S), and therefore is incompatible with the observed data for X(4160). We then discuss the possibility that the X(4160) is the known JPC=1−− charmonium state ψ(4160), which can be produced via two photon fragmentation, but the production rate is much smaller than observed for e+e−→J/ψ+X(4160). In contrast to above two possibilities, the ηc(4S) assignment is a likely one, which is supported by the observed relatively large production rate and non-observation of DD¯ decay of X(4160), but we have to understand why ηc(4S) has such a low mass, which deserves further studies. The P-wave excited state χc0(3P) is also an interesting candidate, if the observed broad peak around 3.8–3.9 GeV in the recoil mass of DD¯ against J/ψ in e++e−→J/ψ+DD¯ is due to the χc0(2P) state. Measurements of production angular distributions will be helpful to distinguish between ηc(4S) and χc0(3P) assignments. Production mechanisms in nonrelativistic QCD are emphasized

    Exploring the molecular scenario of X(4160)

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    Abstract In this work, we investigate the decays of meson X(4160) in the molecular frame. By using an effective lagrangian approach, we calculate the widths of X(4160)J/ψϕX(4160)\rightarrow J/\psi \phi X ( 4160 ) → J / ψ ϕ , DDˉD^*\bar{D}^* D ∗ D ¯ ∗ , DDˉD^*\bar{D} D ∗ D ¯ and DDˉD\bar{D} D D ¯ through the triangle loop mechanism in the molecular scenario. Based on the compositeness condition, the coupling between X(4160) and the DsDˉsD_s^*\bar{D}_s^* D s ∗ D ¯ s ∗ molecular state is determined. The other coupling constants used are determined phenomenologically. The calculation of the decay widths shows that the DDˉD^*\bar{D}^* D ∗ D ¯ ∗ decay mode has a larger branching ratio. These predictions can be seen as a test for the charmonium assignment of X(4160)

    Exploring the molecular scenario of X(4160)

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    In this work, we investigate the decays of meson X(4160)X(4160) in the molecular frame. By using an effective lagrangian approach, we calculate the widths of X(4160)J/ψϕX(4160)\to J/ψϕ, DDˉD^*\bar{D}^*, DDˉD^*\bar{D} and DDˉD\bar{D} through the triangle loop mechanism in the molecular scenario. Based on the compositeness condition, the coupling between X(4160)X(4160) and the DsDˉsD_s^*\bar{D}_s^* molecular state is determined. The other coupling constants used are determined phenomenologically. The calculation of the decay widths shows that the DDˉD^*\bar{D}^* decay mode has a larger branching ratio. These predictions can be seen as a test for the charmonium assignment of X(4160)X(4160).9 pages,10 figure

    Block Card 4160 Angola Road

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    This image was produced by the Auditor's Office in Lucas County, Ohio for tax assessment purposes. Associated dates are approximate. Descriptive terms related to this photograph include: Ranch houses | 4160 Angola Road (Toledo, Ohio) | Dwelling | Adams Township Area (Toledo, Ohio

    The strong decays of X(3940) and X(4160)

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    The new mesons X(3940) and X(4160) have been found by Belle Collaboration in the processes e+eJ/ψD()Dˉ()e^+e^-\rightarrow J/\psi D^{(*)}{\bar{D}}^{(*)}. Considering X(3940) and X(4160) as ηc(3S)\eta _c(3S) and ηc(4S)\eta _c(4S) states, the two-body open charm OZI-allowed strong decay of ηc(3S)\eta _c(3S) and ηc(4S)\eta _c(4S) are studied by the improved Bethe–Salpeter method combined with the 3P0^3P_0 model. The strong decay width of ηc(3S)\eta _c(3S) is Γηc(3S)=(33.515.3+18.4)\Gamma _{\eta _c(3S)}=(33.5^{+18.4}_{-15.3}) MeV, which is close to the result of X(3940); therefore, ηc(3S)\eta _c(3S) is a good candidate of X(3940). The strong decay width of ηc(4S)\eta _c(4S) is Γηc(4S)=(69.921.1+22.4)\Gamma _{\eta _c(4S)}=(69.9^{+22.4}_{-21.1}) MeV, considering the errors of the results, it is close to the lower limit of X(4160). But the ratio of the decay width Γ(DDˉ)Γ(DDˉ)\frac{\Gamma (D{\bar{D}}^*)}{\Gamma (D^*{\bar{D}}^*)} of ηc(4S)\eta _c(4S) is larger than the experimental data of X(4160). According to the above analysis, ηc(4S)\eta _c(4S) is not the candidate of X(4160), and more investigations of X(4160) is needed

    4160. Martin Lefranc, prévôt de Lausanne

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    4160. Martin Lefranc, prévôt de Lausanne. In: Molinier Auguste. Les Sources de l'histoire de France - Des origines aux guerres d'Italie (1494). IV. Les Valois, 1328-1461. Paris : A. Picard et fils, 1904. p. 260

    Cultured neuronal cells treated with SLF HO-4160 decrease production of hydrogen peroxide.

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    <p>MC65 cells were cultured in the presence (TC+) or absence (TC−) of tetracycline, a transgene suppressor of the APP fragment C99. In the absence of tetracycline, cells express the C99 fragment which is then further cleaved to form Aβ. Treatment with either the HO-4160 compound (+4160, 0.3 µM) or the antioxidant vitamin E (+Vit E, 100 µM) reduces the extracellular accumulation of hydrogen peroxide in cells expressing APP-C99. Error bars represent the SEM for N = 3. *p<0.05 TC− compared to both + Vit E and +4160.</p
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