16,715 research outputs found

    Entanglement renormalization and integral geometry

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    We revisit the applications of integral geometry in AdS3_3 and argue that the metric of the kinematic space can be realized as the entanglement contour, which is defined as the additive entanglement density. From the renormalization of the entanglement contour, we can holographically understand the operations of disentangler and isometry in multi-scale entanglement renormalization ansatz. Furthermore, a renormalization group equation of the long-distance entanglement contour is then derived. We then generalize this integral geometric construction to higher dimensions and in particular demonstrate how it works in bulk space of homogeneity and isotropy.Comment: 40 pages, 7 figures. v2: discussions on the general measure added, typos fixed; v3: sections reorganized, various points clarified, to appear in JHE

    LFV couplings of the extra gauge boson Z' and leptonic decay and production of pseudoscalar mesons

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    Considering the constraints of the lepton flavor violating (LFV) processes ΞΌβ†’3e\mu \rightarrow 3e and Ο„β†’3ΞΌ\tau\rightarrow3\mu on the LFV couplings Zβ€²β„“iβ„“jZ'\ell_{i}\ell_{j}, in the contexts of the E6E_{6} models, the left-right (LR) models, the "alternative" left-right (ALR) models and the 331 models, we investigate the contributions of the extra gauge boson Zβ€²Z' to the decay rates of the processes β„“iβ†’β„“jΞ½β„“Ξ½β„“\ell_{i}\rightarrow\ell_{j}\nu_{\ell}\nu_{\ell}, Ο„β†’ΞΌP\tau\rightarrow\mu P and Pβ†’ΞΌeP\rightarrow \mu e with P=Ο€0,Ξ·P=\pi^{0},\eta and Ξ·β€²\eta '. Our numerical results show that the maximal values of the branching ratios for these processes are not dependent on the Zβ€²Z' mass MZβ€²M_{Z'} at leader order. The extra gauge boson ZXβ€²Z'_{X} predicted by the E6E_{6} models can make the maximum value of the branching ratio Br(Ο„β†’ΞΌΞ½β„“Ξ½β„“)Br(\tau\rightarrow\mu\nu_{\ell}\nu_{\ell}) reach 1.1Γ—10βˆ’71.1\times10^{-7}. All Zβ€²Z' models considered in this paper can produce significant contributions to the process Ο„β†’ΞΌP\tau\rightarrow\mu P. However, the value of Br(Pβ†’ΞΌe)Br(P\rightarrow\mu e) is far below its corresponding experimental upper bound.Comment: 14 pages, 2 figures; matches published versio
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