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      Unparticle-Induced Lepton Flavor Violating Decays \tau^- ->l^- (V^0, ~P^0)

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          Abstract

          We make an evaluation of the lepton flavor violating (LFV) decays \(\tau \to \ell (V^0, P^0)\), where \(\ell=e\) or \(\mu\) and \(V^0(P^0)\) is a neutral vector (pseudo-scalar) meson, in the context of unparticle physics. The constraints are investigated systematically on the related coupling parameters from all the available experimental data, and the parameter values are specified appropriately. The results show that whereas over the whole parameter space allowed by experiments all the \(\tau \to \ell P^0\) modes have a branching ratio too small to be measurable experimentally, in a large subspace as observed all of the \(\tau \to \ell V^0\) modes get simultaneously a branching ratio as high as \({\cal O}(10^{-10}-10^{-8})\), which is reachable at the LHC and super B factory. The important implications are drawn.

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          Most cited references9

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          Collider signals in unparticle physics

          Phenomenology of the notion of an unparticle U, recently perceived by Georgi, to describe a scale invariant sector with a non-trivial infrared fixed point at a higher energy scale is explored in details. Behaving like a collection of d_U (the scale dimension of the unparticle operator O_U) invisible massless particles, this unparticle can be unveiled by measurements of various energy distributions for the processes Z to fermion pair + U and e-e+ to gamma U at e-e+ colliders, as well as mono-jet production at hadron colliders. We also study the propagator effects of the unparticle through the Drell-Yan tree level process and the one-loop muon anomaly.
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            Long-range Electron Spin-spin Interactions from Unparticle Exchange

            Unparticles as suggested by Georgi are identities that are not constrained by dispersion relations but are governed by their scaling dimension, d. Their coupling to particles can result in macroscopic interactions between matter, that are generally an inverse nonintegral power of distance. This is totally different from known macroscopic forces. We use the precisely measured long-ranged spin-spin interaction of electrons to constrain unparticle couplings to the electron. For 1
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              Bounds on Unparticles Couplings to Electrons: from Electron g-2 to Positronium Decays

              Yi Liao (2007)
              Unparticles as suggested recently by Georgi have surprising phenomenological implications, distinctive from any other new physics that we know of. But they must interact very feebly with ordinary matter to have avoided detection thus far. We determine how feebly they can interact with the electron, using the precisely measured quantities in QED: the electron g-2 and the bounds on invisible and exotic positronium decays. The most stringent bound comes from invisible ortho-positronium decays: the effective energy scale entering the vector unparticle-electron interaction must exceed 4 x 10^5 TeV for a scaling dimension 3/2 of the vector unparticle. The lower bounds on scales for other unparticles range from a few tens to a few hundreds TeV. This makes the detection of unparticles challenging in low energy electron systems.
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                Author and article information

                Journal
                21 January 2009
                2009-06-03
                Article
                10.1016/j.physletb.2009.05.032
                0901.3266
                1cc77460-4f14-436a-86c4-190c4a788d0c

                http://arxiv.org/licenses/nonexclusive-distrib/1.0/

                History
                Custom metadata
                Phys.Lett.B677:150-156,2009
                18 pages, 3 figures, Version appeared in PLB with many new discussions and more references
                hep-ph

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