5,202 research outputs found

    Analysis on Heavy Quarkonia Transitions with Pion Emission in Terms of the QCD Multipole Expansion and Determination of Mass Spectra of Hybrids

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    One of the most important tasks in high energy physics is search for the exotic states, such as glueball, hybrid and multi-quark states. The transitions ψ(ns)ψ(ms)+ππ\psi(ns)\to \psi(ms)+\pi\pi and Υ(ns)Υ(ms)+ππ\Upsilon(ns)\to \Upsilon(ms)+\pi\pi attract great attentions because they may reveal characteristics of hybrids. In this work, we analyze those transition modes in terms of the theoretical framework established by Yan and Kuang. It is interesting to notice that the intermediate states between the two gluon-emissions are hybrids, therefore by fitting the data, we are able to determine the mass spectra of hybrids. The ground hybrid states are predicted as 4.23 GeV (for charmonium) and 10.79 GeV (for bottonium) which do not correspond to any states measured in recent experiments, thus it may imply that very possibly, hybrids mix with regular quarkonia to constitute physical states. Comprehensive comparisons of the potentials for hybrids whose parameters are obtained in this scenario with the lattice results are presented.Comment: 16 pages, 2 figur

    (3,6-Dibromo-o-phenyl­ene)dimethanol

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    The title compound, C8H8Br2O2, was synthesized from the hydrolysis of 1,4-dibromo-2,3-bis­(bromo­meth­yl)benzene. One intra­molecular O—H⋯O and two intra­molecular C—H⋯Br inter­actions occur. In the crystal, mol­ecules are linked into a chain running parallel to [010]. Adjacent chains are linked into a two-dimensional layer by a combination of inter­molecular O—H⋯O hydrogen bonds and C—H⋯π inter­actions

    Effects of Rashba spin-orbit coupling and a magnetic field on a polygonal quantum ring

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    Using standard quantum network method, we analytically investigate the effect of Rashba spin-orbit coupling (RSOC) and a magnetic field on the spin transport properties of a polygonal quantum ring. Using Landauer-Buttiker formula, we have found that the polarization direction and phase of transmitted electrons can be controlled by both the magnetic field and RSOC. A device to generate a spin-polarized conductance in a polygon with an arbitrary number of sides is discussed. This device would permit precise control of spin and selectively provide spin filtering for either spin up or spin down simply by interchanging the source and drain
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