3,279 research outputs found

    Bipartite Flat-Graph Network for Nested Named Entity Recognition

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    In this paper, we propose a novel bipartite flat-graph network (BiFlaG) for nested named entity recognition (NER), which contains two subgraph modules: a flat NER module for outermost entities and a graph module for all the entities located in inner layers. Bidirectional LSTM (BiLSTM) and graph convolutional network (GCN) are adopted to jointly learn flat entities and their inner dependencies. Different from previous models, which only consider the unidirectional delivery of information from innermost layers to outer ones (or outside-to-inside), our model effectively captures the bidirectional interaction between them. We first use the entities recognized by the flat NER module to construct an entity graph, which is fed to the next graph module. The richer representation learned from graph module carries the dependencies of inner entities and can be exploited to improve outermost entity predictions. Experimental results on three standard nested NER datasets demonstrate that our BiFlaG outperforms previous state-of-the-art models.Comment: Accepted by ACL202

    Comment on "General nonlocality in quantum fields"

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    In this paper, we first incorporate the weak interaction into the theory of General Nonlocality by finding a appropriate metric for it. Accordingly, we suggest the theoretical frame of General Nonlocality as the candidate theory of unifying three microscope interactions in low energy limit. In this unifying scenario, the essential role of photon field is stressed.Comment: Only partial content published in the following reference. The part asserting the fermion mass problem now proved to be wrong, though remains in the versio

    Investigation for ZZ-boson decay into Ξbc\Xi_{bc} and Ξbb\Xi_{bb} baryon with the NRQCD factorizations approach

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    The ZZ-boson decay provides good opportunities for the research on ΞbQβ€²\Xi_{bQ'} baryon due to large quantity of ZZ events that can be collected at the high-energy colliders. We performed a completed investigation of the indirect production of the Ξbc\Xi_{bc} and Ξbb\Xi_{bb} baryon via ZZ-boson decay Zβ†’ΞžbQβ€²+bΛ‰+QΛ‰β€²Z\to \Xi_{bQ'}+\bar b +\bar Q' with Qβ€²=(c,b)Q'= (c, b) quark according to NRQCD factorizations approach. After considering the contribution of the diquark states ⟨bc⟩[3S1]3Λ‰/6\langle bc\rangle [^3S_1]_{\bar 3/6}, ⟨bc⟩[1S0]3Λ‰/6\langle bc\rangle [^1S_0]_{\bar 3/6}, ⟨bb⟩[1S0]6\langle bb\rangle [^1S_0]_{6} and ⟨bb⟩[3S1]3Λ‰\langle bb\rangle [^3S_1]_{\bar 3}, the calculated branching ratio for Zβ†’ΞžbQβ€²+XZ\to\Xi_{bQ'}+X are B(Zβ†’Ξžbc+X)=3.595Γ—10βˆ’5{\cal B}(Z\to\Xi_{bc}+X) = 3.595\times 10^{-5} and B(Zβ†’Ξžbc+X)=1.213Γ—10βˆ’6{\cal B}(Z\to\Xi_{bc}+X) = 1.213\times 10^{-6}. Moreover, the Ξbc\Xi_{bc} events produced are predicted to be of the 104(107)10^4(10^7) order at the LHC(CEPC), while the Ξbb\Xi_{bb} events produced are forecasted to be of the 103(106)10^3(10^6) order. Furthermore, we have estimated the production ratio R(ZQβ†’Ξžbc+,0){\cal R}(Z_Q\to\Xi^{+,0}_{bc}) with four ZZ-boson decay channels. The R(ZQβ†’Ξžbc+,0){\cal R}(Z_Q\to\Xi^{+,0}_{bc}) up to 10βˆ’610^{-6} for Zβ†’ccΛ‰Z\to c\bar c channel and 10βˆ’510^{-5} for Zβ†’bbΛ‰Z\to b\bar b channel, respectively. Finally, we present the differential decay widths of Ξbc(Ξbb)\Xi_{bc}(\Xi_{bb}) with respect to s23s_{23} and zz distributions, and analysis the uncertainties.Comment: 9 pages, 4 figures. Some ambiguous sentences have been modified and discussion extende

    Further study on the production of P-wave doubly heavy baryons from Z-boson decays

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    In this paper, we carried out a systematic investigation about the excited doubly heavy baryons production in ZZ-boson decays within the framework of NRQCD. Our investigation accounts for all the intermediate diquark states, including those in PP-wave such as ⟨cc⟩[1P1]3Λ‰\langle cc\rangle[^1P_1]_{\bar 3}, ⟨cc⟩[3PJ]6\langle cc\rangle[^3P_J]_{6}, ⟨bc⟩[1P1]3Λ‰/6\langle bc\rangle[^1P_1]_{\bar 3/6}, ⟨bc⟩[3PJ]3Λ‰/6\langle bc\rangle[^3P_J]_{\bar 3/6}, ⟨bb⟩[1P1]3Λ‰\langle bb\rangle[^1P_1]_{\bar 3}, and ⟨bb⟩[3PJ]6\langle bb\rangle[^3P_J]_{6} with J=(0,1,2)J = (0, 1, 2), were taken into account. The results show that the contributions of the all diquark state in PP-wave were 7%7\%, 8%8\%, and 3%3\%, respectively, when compared to SS-wave. Based on these results, we anticipate that about 0.539Γ—103(106)0.539\times 10^3(10^6) events of excited Ξcc\Xi_{cc}, 1.827Γ—103(106)1.827\times 10^3(10^6) events of excited Ξbc\Xi_{bc} and 0.036Γ—103(106)0.036\times 10^3(10^6) events of excited Ξbb\Xi_{bb} can be produced annually at the LHC (CEPC). Additionally, we plot the differential decay widths of Ξcc\Xi_{cc}, Ξbc\Xi_{bc} and Ξbb\Xi_{bb} as a function of the invariant mass s23s_{23} and energy fuction zz distributions, and analyze the theoretical uncertainties decay width arising from the mass parameters of heavy quark.Comment: 11 pages, 4 figure

    Like-sign Di-lepton Signals in Higgsless Models at the LHC

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    We study the potential LHC discovery of the Z1 KK gauge boson unitarizing longitudinal W+W- scattering amplitude. In particular, we explore the decay mode Z1->t tbar along with Z1-> W+W- without specifying the branching fractions. We propose to exploit the associated production pp-> W Z1, and select the final state of like-sign dileptons plus multijets and large missing energy. We conclude that it is possible to observe the Z1 resonance at a 5 sigma level with an integrated luminosity of 100 inverse fb at the LHC upto 650 GeV for a dominant WW channel, and 560 GeV for a dominant ttbar channel.Comment: 13 pages, 7 figure
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