1,942 research outputs found

    Light axigluon and single top production at the LHC

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    The light axigluon model can explain the Tevatron tt‾t\overline{t} forward-backward asymmetry and at the same time satisfy the constraints from the electroweak precision measurement and the ATLASATLAS and CMSCMS data, which induces the flavor changing (FCFC) couplings of axigluon with the SMSM and new quarks. We investigate the effects of these FCFC couplings on the s- and t-channel single top productions at the LHCLHC and the FCFC decays Z→b‾s+bs‾Z\rightarrow \overline{b}s+b\overline{s}, t→cγt\rightarrow c\gamma and cgcg. Our numerical results show that the light axigluon can give significantly contributions to single top production and the rare top decays t→cγt\rightarrow c\gamma and cgcg.Comment: 22 pages, 8 figures; references added, contributions of new quarks to rare decay processes adde

    Bottom partner B' and Zb production at the LHC

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    Some new physics models, such as "beautiful mirrors" scenario, predict the existence of the bottom partner B′B'. Considering the constraints from the data for the Z→bbˉZ\rightarrow b\bar{b} branching ratio RbR_{b} and the FBFB asymmetry AFBbA_{FB}^{b} on the relevant free parameters, we calculate the contributions of B′B' to the cross section σ(Zb)\sigma(Zb) and the ZZ polarization asymmetry AZA_{Z} for ZbZb production at the LHCLHC. We find that the bottom partner B′B' can generate significant corrections to σ(Zb)\sigma(Zb) and AZA_{Z}, which might be detected in near future.Comment: 15 pages, 5 figures. Version published in Phys. Lett.

    Universal scheme to generate metal-insulator transition in disordered systems

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    We propose a scheme to generate metal-insulator transition in random binary layer (RBL) model, which is constructed by randomly assigning two types of layers. Based on a tight-binding Hamiltonian, the localization length is calculated for a variety of RBLs with different cross section geometries by using the transfer-matrix method. Both analytical and numerical results show that a band of extended states could appear in the RBLs and the systems behave as metals by properly tuning the model parameters, due to the existence of a completely ordered subband, leading to a metal-insulator transition in parameter space. Furthermore, the extended states are irrespective of the diagonal and off-diagonal disorder strengths. Our results can be generalized to two- and three-dimensional disordered systems with arbitrary layer structures, and may be realized in Bose-Einstein condensates.Comment: 5 ages, 4 figure

    Remote information concentration and multipartite entanglement in multilevel systems

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    Remote information concentration (RIC) in dd-level systems (qudits) is studied. It is shown that the quantum information initially distributed in three spatially separated qudits can be remotely and deterministically concentrated to a single qudit via an entangled channel without performing any global operations. The entangled channel can be different types of genuine multipartite pure entangled states which are inequivalent under local operations and classical communication. The entangled channel can also be a mixed entangled state, even a bound entangled state which has a similar form to the Smolin state, but has different features from the Smolin state. A common feature of all these pure and mixed entangled states is found, i.e., they have d2d^2 common commuting stabilizers. The differences of qudit-RIC and qubit-RIC (d=2d=2) are also analyzed.Comment: 10 pages, 3 figure

    Expression of hypoxia inducible factor-1α and vascular endothelial growth factor-C in human chronic periodontitis

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    AbstractBackground/purposeEvidence shows that there is a relationship between hypoxia and inflammatory response in periodontitis. Hypoxia-inducible factor (HIF)-1α is a major regulator of energy homeostasis and cellular adaptation to low oxygen stress. Although experimental results demonstrate an association between HIF-1α and vascular endothelial growth factor (VEGF)-C in tumor angiogenesis, the role of HIF-1α and VEGF-C in the pathogenesis of periodontitis is still ambiguous. So far, limited attention has been given to the role of hypoxia and VEGF-C in periodontitis. The present study aimed to investigate the expression and distribution of HIF-1α and VEGF-C in gingival tissue samples from patients with different stages of chronic periodontitis and healthy individuals.Materials and methodsA total of 56 samples were involved in this study, including moderate chronic periodontitis (n = 20), advanced chronic periodontitis (n = 20), and healthy control tissues (n = 16). The gingival specimens were stained with hematoxylin and eosin for histopathology. The expression of HIF-1α and VEGF-C in gingival tissues was detected by immunohistochemical staining.ResultsHIF-1α and VEGF-C were found in gingival tissues from patients with different stages of chronic periodontitis as well as healthy control tissues. HIF-1α protein was expressed mainly in the epithelial layer of gingival tissues, and VEGF-C protein was mostly located in the connective tissue papilla of gingival tissues. Compared with healthy controls, the expression of HIF-1α and VEGF-C in chronic periodontitis groups was significantly higher (P < 0.01), and the density of HIF-1α and VEGF-C in advanced chronic periodontitis group was even significantly higher than that in the moderate chronic periodontitis group (P < 0.01).ConclusionOur results suggest that the expression of HIF-1α and VEGF-C increased with severity of periodontitis. So, we conclude that HIF-1α may play an important role in the pathophysiology of human periodontitis and may be related to the function of VEGF-C during periodontitis

    ON THE EXISTENCE AND UNIQUENESS OF A LIMIT CYCLE FOR A LIENARD SYSTEM WITH A DISCONTINUITY LINE

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    In this paper, we investigate the existence and uniqueness of crossing limit cycle for a planar nonlinear Lienard system which is discontinuous along a straight line (called a discontinuity line). By using the Poincare mapping method and some analysis techniques, a criterion for the existence, uniqueness and stability of a crossing limit cycle in the discontinuous differential system is established. An application to Schnakenberg model of an autocatalytic chemical reaction is given to illustrate the effectiveness of our result. We also consider a class of discontinuous piecewise linear differential systems and give a necessary condition of the existence of crossing limit cycle, which can be used to prove the non-existence of crossing limit cycle

    Hexa-μ2-acetato-κ12 O:O′-(azido-κN)bis­(methanol-κO)-μ3-oxido-trichromium(III) methanol monosolvate

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    In the crystal structure of the title complex, [Cr3(CH3CO2)6(N3)O(CH3OH)2]·CH3OH, the trinuclear core has a central O atom; two methanol mol­ecules and an azide ion are coordinated to the CrIII atoms in the core. The three CrIII atoms form vertices of a nearly equilateral triangle. Each of the six acetate carboxyl­ate groups bridges a Cr—O—Cr fragment. In the crystal, the molecules inter­act with methanol solvent mol­ecules through O—H⋯O and O—H⋯N hydrogen bonds, forming a two-dimensional hydrogen-bonded network parallel to (100)
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