2,077 research outputs found

    The decay rate of ψ(2S)\psi(2S) to Λc+ÎŁ+ˉ\Lambda_c+\bar{\Sigma^+} in SM and beyond

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    With rapid growth of the database of the BES III and the proposed super flavor factory, measurement on the rare ψ(2S)\psi(2S) decays may be feasible, especially the weak decays into baryon final states. In this work we study the decay rate of ψ(2S)\psi(2S) to Λc+ÎŁ+‟\Lambda_c+\overline{\Sigma^+} in the SM and physics beyond the SM (here we use the unparticle model as an example). The QPC model is employed to describe the creation of a pair of qqˉq\bar q from vacuum. We find that the rate of ψ(2S)→Λc+ÎŁ+‟\psi(2S)\rightarrow \Lambda_c+\overline{\Sigma^+} is at order of 10−1010^{-10} in the SM, whereas the contribution of the unparticle is too small to be substantial. Therefore if a large branching ratio is observed, it must be due to new physics beyond SM, but by no means the unparticle.Comment: 9 pages, 1 figure

    Search for Bc(ns)B_c(ns) via the Bc(ns)→Bc(ms)π+π−B_c(ns)\to B_c(ms)\pi^+\pi^- transition at LHCb and Z0Z_0 factory

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    It is interesting to study the characteristics of the whole family of BcB_c which contains two different heavy flavors. LHC and the proposed Z0Z^0 factory provide an opportunity because a large database on the BcB_c family will be achieved. BcB_c and its excited states can be identified via their decay modes. As suggested by experimentalists, Bc∗(ns)→Bc+ÎłB_c^*(ns)\to B_c+\gamma is not easy to be clearly measured, instead, the trajectories of π+\pi^+ and π−\pi^- occurring in the decay of Bc(ns)→Bc(ms)+π+π−B_c(ns)\to B_c(ms)+\pi^+\pi^- (n>mn>m) can be unambiguously identified, thus the measurement seems easier and more reliable, therefore this mode is more favorable at early running stage of LHCb and the proposed Z0Z^0 factory. In this work, we calculate the rate of Bc(ns)→Bc(ms)+π+π−B_c(ns)\to B_c(ms)+\pi^+\pi^- in terms of the QCD multipole-expansion and the numerical results indicate that the experimental measurements with the luminosity of LHC and Z0Z^0 factory are feasible.Comment: 12 pages, 1 figures and 4 tables, acceptted by SCIENCE CHINA Physics, Mechanics & Astronomy (Science in China Series G

    The signal of Z±(4430)Z^\pm(4430) in nucleon-antinucleon scattering

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    We study the production of Z±(4430)Z^\pm(4430) at a nucleon-antinucleon scattering experiment. Considering the PANDA experiment to be an ideal platform to explore the production of the charmonium and charmonim-like states, we suggest the forthcoming PANDA experiment to pay attention to the production of Z±(4430)Z^\pm(4430).Comment: 6 pages, 15 figures. Published version in EPJ

    The magnetic dipole transitions in the (cbˉ)(c\bar{b}) binding system

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    The magnetic dipole transitions between the vector mesons Bc∗B_c^* and their relevant pseudoscalar mesons BcB_c (BcB_c, Bc∗B_c^*, Bc(2S)B_c(2S), Bc∗(2S)B_c^*(2S), Bc(3S)B_c(3S) and Bc∗(3S)B_c^*(3S) etc, the binding states of (cbˉ)(c\bar{b}) system) of the BcB_c family are interesting. To see the `hyperfine' splitting due to spin-spin interaction is an important topic for understanding the spin-spin interaction and the spectrum of the the (cbˉ)(c\bar{b}) binding system. The knowledge about the magnetic dipole transitions is also very useful for identifying the vector boson Bc∗B_c^* mesons experimentally, whose masses are just slightly above the masses of their relevant pseudoscalar mesons BcB_c accordingly. Considering the possibility to observe the vector mesons via the transitions at Z0Z^0 factory and the potentially usages of the theoretical estimate on the transitions, we fucus our efforts on calculating the magnetic dipole transitions, i.e. precisely to calculate the rates for the transitions such as decays Bc∗→BcγB_c^*\to B_c\gamma and Bc∗→Bce+e−B_c^*\to B_c e^+e^-, and particularly work in the Behte-Salpeter framework. In the estimate, as a typical example, we carefully investigate the dependance of the rate Γ(Bc∗→Bcγ)\Gamma(B_c^*\to B_c\gamma) on the mass difference ΔM=MBc∗−MBc\Delta M=M_{B_c^*}-M_{B_c} as well.Comment: 10 pages, 2 figures, 1 tabl

    An Investigation of Willingness to Pay for Geopark Management and Conservation: A Case Study of Geotourists in the Greater China Region

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    Willingness to pay (WTP) for geological protection is essential for market-based geopark conservation tactic formulations. Whether geotourists are willing to pay and how much they prefer to pay might be influenced by different determinants. The present study aims to (1) investigate the probability of paying and the payment amount for geopark conservation and (2) examine how factors influence the intention and amount to pay for the upkeep of geoparks. The results suggest that geotourists would contribute financially to geological conservation and geopark management. The findings also revealed that geotourists’ intentions and payment for conservation were associated with educational background and monthly income level. In addition, geotourist attachment and satisfaction concerning visiting geoparks positively affected intention and payment. This study might provide empirical references for geopark management and conservation in the Greater China Region

    Understanding the Determinants of Geologically Responsible Behaviour among Geotourists: A Multi-Destination Analysis

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    This study explores the drivers of geologically responsible behaviour among geotourists in three geoparks in the Greater China region: Danxiashan UNESCO Global Geopark in southern China, Hong Kong UNESCO Global Geopark, and Yehliu Geopark in northern Taiwan. On-site questionnaire surveys were conducted, collecting over 800 respondents in these geoparks, and structural equation modelling was applied for our analysis. The findings reveal that geologically responsible behaviour is positively associated with environmentally responsible attitudes, in line with some previous research. Notably, place attachment and visitor satisfaction were not directly related to geologically responsible behaviour but were positively correlated with environmentally responsible attitudes. This suggests that emotional connections to geoparks and visitor satisfaction indirectly nurture environmentally responsible attitudes, subsequently leading to geologically responsible behaviour. These results offer practical implications for geopark management practices. Providing informative guided tours and quality informational materials can enhance visitors’ geological knowledge and foster environmentally responsible attitudes. The improvement of the visitor experience, combined with the dissemination of accurate environmental knowledge and conservation messaging, can enhance visitor satisfaction, deepen attachment to geoparks, and, ultimately, encourage more geologically responsible behaviours. Understanding these relationships can assist geotourism destinations in promoting geological resources’ conservation while enhancing the visitor experience

    D-branes with Lorentzian signature in the Nappi-Witten model

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    Lorentzian signature D-branes of all dimensions for the Nappi-Witten string are constructed. This is done by rewriting the gluing condition J+=FJ−J_+=FJ_- for the model chiral currents on the brane as a well posed first order differential problem and by solving it for Lie algebra isometries FF other than Lie algebra automorphisms. By construction, these D-branes are not twined conjugacy classes. Metrically degenerate D-branes are also obtained.Comment: 22 page

    Infinitely many N=2 SCFT with ADE flavor symmetry

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    We present evidence that for each ADE Lie group G there is an infinite tower of 4D N = 2 SCFTs, which we label as D(G, s) with s 08 \u2115, having (at least) flavor symmetry G. For G = SU(2), D(SU(2),s) coincides with the Argyres-Douglas model of type D8+1, while for larger flavor groups the models are new (but for a few previously known examples). When its flavor symmetry G is gauged, D(G,s) contributes to the Yang-Mills beta-function as 8/2(+1) adjoint hypermultiplets. The argument is based on a combination of Type IIB geometric engineering and the categorical deconstruction of arXiv: 1203.6743. One first engineers a class of N = 2 models which, trough the analysis of their category of quiver representations, are identified as asymptotically-free gauge theories with gauge group G coupled to some conformal matter system. Taking the limit gYM \u2192 0 one isolates the matter SCFT which is our D(G, s). \ua9 SISSA 2013

    Geometric construction of D-branes in WZW models

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    The geometric description of D-branes in WZW models is pushed forward. Our starting point is a gluing condition\, J+=FJ−J_{+}=FJ_- that matches the model's chiral currents at the worldsheet boundary through a linear map FF acting on the WZW Lie algebra. The equivalence of boundary and gluing conditions of this type is studied in detail. The analysis involves a thorough discussion of Frobenius integrability, shows that FF must be an isometry, and applies to both metrically degenerate and nondegenerate D-branes. The isometry FF need not be a Lie algebra automorphism nor constantly defined over the brane. This approach, when applied to isometries of the form F=RF=R with RR a constant Lie algebra automorphism, validates metrically degenerate RR-twined conjugacy classes as D-branes. It also shows that no D-branes exist in semisimple WZW models for constant\, F=−RF=-R.Comment: 23 pages, discussion of limitations of the gluing condition approach adde
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