232 research outputs found

    Zc(3900)Z_c(3900) as a DDˉ∗D\bar{D}^* molecule from the pole counting rule

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    A comprehensive study on the nature of the Zc(3900)Z_c(3900) resonant structure is carried out in this work. By constructing the pertinent effective Lagrangians and considering the important final-state-interaction effects, we first give a unified description to all the relevant experimental data available, including the J/ψπJ/\psi\pi and ππ\pi\pi invariant mass distributions from the e+e−→J/ψππe^+e^-\to J/\psi\pi\pi process, the hcπh_c\pi distribution from e+e−→hcππe^+e^-\to h_c\pi\pi and also the DDˉ∗D\bar D^{*} spectrum in the e+e−→DDˉ∗πe^+e^-\to D\bar D^{*}\pi process. After fitting the unknown parameters to the previous data, we search the pole in the complex energy plane and find only one pole in the nearby energy region in different Riemann sheets. Therefore we conclude that Zc(3900)Z_c(3900) is of DDˉ∗D\bar D^* molecular nature, according to the pole counting rule method~[Nucl.~Phys.~A543, 632 (1992); Phys.~Rev.~D 35,~1633 (1987)]. We emphasize that the conclusion based upon the pole counting method is not trivial, since both the DDˉ∗D\bar D^{*} contact interactions and the explicit ZcZ_c exchanges are introduced in our analyses and they lead to the same conclusion.Comment: 21 pages, 9 figures. To match the published version in PRD. Additional discussion on the spectral density function is include

    On leptonic width of X(4260)X(4260)

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    New measurements on cross sections in e+e−→J/ψπ+π−e^+e^-\to J/\psi\pi^+\pi^-, hcπ+π−h_c\pi^+\pi^-, D0D∗−π++c.c.D^0D^{*-}\pi^++c.c., ψ(2S)π+π−\psi(2S)\pi^+\pi^-, ωχc0\omega\chi_{c0} and J/ψηJ/\psi\eta channels have been carried out by BESIII, Belle and BABAR collaborations, and also in the Ds∗Dˉs∗D_s^*\bar D_s^* channel. We perform extensive numerical analyses by combining all these data available, together with those in DDˉ∗D\bar D^* and D∗Dˉ∗D^*\bar D^* channels. Though the latter show no evident peak around s=4.230\sqrt{s}=4.230 GeV, the missing X(4260)X(4260) is explained as that it is concealed by the interference effects of the well established charmonia ψ(4040)\psi(4040), ψ(4160)\psi(4160) and ψ(4415)\psi(4415). Our analyses reveal that the leptonic decay width of X(4260)X(4260) ranges from O(102)O(10^2) eV to O(1)O(1) keV, and hence may be explained in the conventional quark model picture. That is, the X(4260)X(4260) may well be interpreted as a mixture of 43S14^3S_1 and 33D13^3D_1 states.Comment: two small mistakes are fixed, figures redrawn, major physical outputs remain unchanged. Version published in EPJ

    Effects of Mo on the Microstructure and Hydrogen Sorption Properties of Ti-Mo Getters

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    AbstractThe effects of Mo on the microstructure evolution, porosity and hydrogen sorption properties of Ti-Mo getters are investigated in this work. The results show that the addition of Mo prolongs the densification process of Ti-Mo getters and results in a significant amount of sintered pores. With the Mo content increasing, the porosity of getters firstly increases reaching the maximum value as it attains about 7.5wt.%, and then drops. At the room temperature, the hydrogen sorption property of getters increases progressively with the Mo content increasing, but the tendency is not very clear before its content lies below 2.5wt.%. When the Mo content achieves about 7.5wt.%, the hydrogen sorption property proves to be the best. The discussion is made about the above mentioned phenomena inclusive of hydrogen sorption properties of getters under different activation conditions (from 500–750 °C)

    Upregulation of microRNA-25 associates with prognosis in hepatocellular carcinoma

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    BACKGROUND: Accumulating evidence has shown that up-regulation of microRNA-25(miR-25) is associated with the prognosis of several types of human malignant solid tumors. However, whether miR-25 expression has influence on the prognosis of hepatocellular carcinoma (HCC) is still unknown. METHODS: The differentially expressed amount of the miR-25 was validated in triplicate by quantitative reverse-transcription polymerase chain reaction (qRT-PCR). Survival rate was analyzed by log-rank test, and survival curves were plotted according to Kaplan–Meier. Multivariate analysis of the prognostic factors was performed with Cox regression model. RESULTS: The expression of miR-25 was significantly upregulated in HCC tissues when compared with adjacent normal tissues (p<0.0001). Patients who had high miR-25 expression had a shorter overall survival than patients who had low miR-25 expression (median overall survival, 31.0 months versus 42.9 months, p=0.0192). The multivariate Cox regression analysis indicated that miR-25 expression (HR=2.179; p=0.001), TNM stage (HR=1.782; p=0.014), and vein invasion (HR=1.624; p=0.020) were independent prognostic factors for overall survival. CONCLUSION: Our data suggests that the overexpression of miR-25 in HCC tissues is of predictive value on poor prognosis. VIRTUAL SLIDE: The virtual slide(s) for this article can be found here: http://www.diagnosticpathology.diagnomx.eu/vs/198961842111430

    Transforming Multidisciplinary Customer Requirements to Product Design Specifications

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    With the increasing of complexity of complex mechatronic products, it is necessary to involve multidisciplinary design teams, thus, the traditional customer requirements modeling for a single discipline team becomes difficult to be applied in a multidisciplinary team and project since team members with various disciplinary backgrounds may have different interpretations of the customers’ requirements. A new synthesized multidisciplinary customer requirements modeling method is provided for obtaining and describing the common understanding of customer requirements (CRs) and more importantly transferring them into a detailed and accurate product design specifications (PDS) to interact with different team members effectively. A case study of designing a high speed train verifies the rationality and feasibility of the proposed multidisciplinary requirement modeling method for complex mechatronic product development. This proposed research offersthe instruction to realize the customer-driven personalized customization of complex mechatronic product

    Investigating a Global Collapsing Hub-Filament Cloud G326.611+0.811

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    We present the dynamics study toward the G326.611+0.811 (G326) hub-filament-system (HFS) cloud using the new APEX observations of both 13^{13}CO and C18^{18}O (J = 2-1). The G326 HFS cloud constitutes a central hub and at least four hub-composing filaments that are divided into a major branch of filaments (F1, and F2) and a side branch (F3-F5). The cloud holds ongoing high-mass star formation as characterised by three massive dense clumps (i.e., 370-1100 M⊙M_{\odot} and 0.14-0.16 g cm−2^{-2} for C1-C3) with the high clump-averaged mass infalling rates (>10−3>10^{-3} M⊙M_{\odot} yr−1^{-1}) within in the major filament branch, and the associated point sources bright at 70 μ\mum typical of young protostars. Along the five filaments, the velocity gradients are found in both 13^{13}CO and C18^{18}O (J = 2-1) emission, suggesting that the filament-aligned gravitational collapse toward the central hub (i.e., C2) is being at work for high-mass star formation therein. Moreover, a periodic velocity oscillation along the major filament branch is revealed in both 13^{13}CO and C18^{18}O (J = 2-1) emission with a characteristic wavelength of ∼\sim3.5 pc and an amplitude of ∼\sim0.31-0.38 km s−1^{-1}. We suggest that this pattern of velocity oscillation in G326 could arise from the clump-forming gas motions induced by gravitational instability. Taking into account the prevalent velocity gradients, the fragmentation of the major branch of filaments, and the ongoing collapse of the three massive dense clumps, it is indicative that G326 is a HFS undergoing global collapse.Comment: 21 pages, 13 figures, 2 tables, Accepted for publication in Ap

    A possible 250-second X-ray quasi-periodicity in the fast blue optical transient AT2018cow

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    The fast blue optical transients (FBOTs) are a new population of extragalactic transients of unclear physical origin. A variety of mechanisms have been proposed including failed supernova explosion, shock interaction with a dense medium, young magnetar, accretion onto a compact object, and stellar tidal disruption event, but none is conclusive. Here we report the discovery of a possible X-ray quasi-periodicity signal with a period of ∼\sim250 second (at a significance level of 99.76%) in the brightest FBOT AT2018cow through the analysis of XMM-Newton/PN data. The signal is independently detected at the same frequency in the average power density spectrum from data taken from the Swift telescope, with observations covering from 6 to 37 days after the optical discovery, though the significance level is lower (94.26%). This suggests that the QPO frequency may be stable over at least 1.1×\times 104^{4} cycles. Assuming the ∼\sim250 second QPO to be a scaled-down analogue of that typically seen in stellar mass black holes, a black hole mass of ∼103−105\sim10^{3}-10^{5} solar masses could be inferred. The overall X-ray luminosity evolution could be modeled with the stellar tidal disruption by a black hole of ∼104\sim10^4 solar masses, providing a viable mechanism to produce AT2018cow. Our findings suggest that other bright FBOTs may also harbor intermediate-mass black holes.Comment: 18 pages, 10 figures. Accepted for publication in Research in Astronomy and Astrophysic

    A simulation study on the measurement of D0-D0bar mixing parameter y at BES-III

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    We established a method on measuring the \dzdzb mixing parameter yy for BESIII experiment at the BEPCII e+e−e^+e^- collider. In this method, the doubly tagged ψ(3770)→D0D0‾\psi(3770) \to D^0 \overline{D^0} events, with one DD decays to CP-eigenstates and the other DD decays semileptonically, are used to reconstruct the signals. Since this analysis requires good e/πe/\pi separation, a likelihood approach, which combines the dE/dxdE/dx, time of flight and the electromagnetic shower detectors information, is used for particle identification. We estimate the sensitivity of the measurement of yy to be 0.007 based on a 20fb−120fb^{-1} fully simulated MC sample.Comment: 6 pages, 7 figure
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