30,102 research outputs found

    Multiquark Hadrons - A New Facet of QCD

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    I review some selected aspects of the phenomenology of multiquark states discovered in high energy experiments. They have four valence quarks (called tetraquarks) and two of them are found to have five valence quarks (called pentaquarks), extending the conventional hadron spectrum which consists of quark-antiquark (qqˉ)(q\bar{q}) mesons and qqqqqq baryons. Multiquark states represent a new facet of QCD and their dynamics is both challenging and currently poorly understood. I discuss various approaches put forward to accommodate them, with emphasis on the diquark model.Comment: 27 pages, 8 figures, 6 tables, to be published in the proceedings of the 14th. Regional Conference on Mathematical Physics, Nov. 9-14, 2015, Quaid-i-Azam University, Islamabad, Pakista

    CKM Phenomenology and B-Meson Physics - Present Status and Current Issues

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    We review the status of the Cabibbo-Kobayashi-Maskawa (CKM) matrix elements and the CP-violating phases in the CKM-unitarity triangle. The emphasis in these lecture notes is on BB-meson physics, though we also review the current status and issues in the light quark sector of this matrix. Selected applications of theoretical methods in QCD used in the interpretation of data are given and some of the issues restricting theoretical precision on the CKM matrix elements discussed. The overall consistency of the CKM theory with the available data in flavour physics is impressive and we quantify this consistency. Current data also show some anomalies which, however, are not yet statistically significant. They are discussed briefly. Some benchmark measurements that remain to be done in experiments at the BB-factories and hadron colliders are listed. Together with the already achieved results, they will provide unprecedented tests of the CKM theory and by the same token may lead to the discovery of new physics.Comment: 66 pages, 13 figures, uses pr-imfp03-new.cls (enclosed); Lectures given at the International Meeting on Fundamental Physics, Soto de Cangas (Asturias), Spain, February 23 - 28, 2003 (to appear in the proceedings.

    Hair histology as a tool for forensic identification of some domestic animal species

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    Animal hair examination at a criminal scene may provide valuable information in forensic investigations. However, local reference databases for animal hair identification are rare. In the present study, we provide differential histological analysis of hair of some domestic animals in Upper Egypt. For this purpose, guard hair of large ruminants (buffalo, camel and cow), small ruminants (sheep and goat), equine (horse and donkey) and canine (dog and cat) were collected and comparative analysis was performed by light microscopy. Based on the hair cuticle scale pattern, type and diameter of the medulla, and the pigmentation, characteristic differential features of each animal species were identified. The cuticle scale pattern was imbricate in all tested animals except in donkey, in which coronal scales were identified. The cuticle scale margin type, shape and the distance in between were characteristic for each animal species. The hair medulla was continuous in most of the tested animal species with the exception of sheep, in which fragmental medulla was detected. The diameter of the hair medulla and the margins differ according to the animal species. Hair shaft pigmentation were not detected in all tested animals with the exception of camel and buffalo, in which granules and streak-like pigmentation were detected. In conclusion, the present study provides a first-step towards preparation of a complete local reference database for animal hair identification that can be used in forensic investigations.Comment: 8 pages, 3 Figure

    Emergence of Cosmic Space and Minimal Length in Quantum Gravity

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    An emergence of cosmic space has been suggested by Padmanabhan in [arXiv:1206.4916]. This new interesting approach argues that the expansion of the universe is due to the difference between the number of degrees of freedom on a holographic surface and the one in the emerged bulk. In this paper, we derive, using emergence of cosmic space framework, the general dynamical equation of FRW universe filled with a perfect fluid by considering a generic form of the entropy as a function of area. Our derivation is considered as a generalization of emergence of cosmic space with a general form of entropy. We apply our equation with higher dimensional spacetime and derive modified Friedmann equation in Gauss-Bonnet gravity. We then apply our derived equation with the corrected entropy-area law that follows from Generalized Uncertainty Principle (GUP) and derive a modified Friedmann equations due to the GUP. We then derive the modified Raychaudhuri equation due to GUP in emergence of cosmic space framework and investigate it using fixed point method. Studying this modified Raychaudhuri equation leads to non-singular solutions which may resolve singularities in FRW universe.Comment: 10 pages, revtex4, 1 figure, to match published version in PL

    Production of the Exotic 1−−1^{--} Hadrons ϕ(2170)\phi(2170), X(4260) and Yb(10890)Y_b(10890) at the LHC and Tevatron via the Drell-Yan Mechanism

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    We calculate the Drell-Yan production cross sections and differential distributions in the transverse momentum and rapidity of the JPC=1−−J^{PC}=1^{--} exotic hadrons ϕ(2170)\phi(2170), X(4260) and Yb(10890)Y_b(10890) at the hadron colliders LHC and the Tevatron. These hadrons are tetraquark (four-quark) candidates, with a hidden ssˉs\bar{s}, ccˉc\bar{c} and bbˉb\bar{b} quark pair, respectively. In deriving the distributions and cross sections, we include the order αs\alpha_s QCD corrections, resum the large logarithms in the small transverse momentum region in the impact-parameter formalism, and use the state of the art parton distribution functions. Taking into account the data on the production and decays of these vector hadrons from the e+e−e^+e^- experiments, we present the production rates for the processes pp(pˉ)→ϕ(2170)(→ϕ(1020)π+π−→K+K−π+π−)+...pp(\bar{p}) \to \phi(2170)(\to \phi(1020) \pi^+\pi^- \to K^+K^- \pi^+\pi^-)+..., pp(pˉ)→X(4260)(→J/ψπ+π−→μ+μ−π+π−)+...pp(\bar{p}) \to X(4260)(\to J/\psi \pi^+\pi^- \to \mu^+\mu^-\pi^+\pi^-)+..., and pp(pˉ)→Yb(10890)(→(Υ(1S),Υ(2S),Υ(3S))π+π−→μ+μ−π+π−)+...pp(\bar{p}) \to Y_b(10890)(\to (\Upsilon(1S), \Upsilon(2S), \Upsilon(3S)) \pi^+\pi^- \to \mu^+\mu^-\pi^+\pi^-)+.... Their measurements at the hadron colliders will provide new experimental avenues to explore the underlying dynamics of these hadrons.Comment: 4 pages, 2 Tables, 2 Figures; submitted to Physical Review Letter
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