34,786 research outputs found

    New Physics Searches with Higgs-photon associated production at the Higgs Factory

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    The Higgs factory is designed for precise measurement of Higgs characters and search for new physics. In this paper we propose that e+eβˆ’β†’Ξ³he^+e^- \to \gamma h process could be a useful channel for new physics, which is normally expressed model independently by effective field theory. We calculate the cross section in both the Standard Model and effective field theory approach, and find that the new physics effects of Ξ³h\gamma h have only two degrees of freedom, much fewer than the Higgsstrahlung process. This point could be used to reduce the degeneracies of Wilson coefficients. We also calculated for the first time the 2Οƒ\sigma bounds of Ξ³h\gamma h at the Higgs factory, and prove that Ξ³h\gamma h is more sensitive to some dimension-6 operators than the current experimental data. In the optimistic scenario new physics effects may be observed at the CEPC or FCC-ee after the first couple of years of their run.Comment: 5 pages, 3 figures, submitted to Chinese Physics

    Minimax Estimation of Large Precision Matrices with Bandable Cholesky Factor

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    Last decade witnesses significant methodological and theoretical advances in estimating large precision matrices. In particular, there are scientific applications such as longitudinal data, meteorology and spectroscopy in which the ordering of the variables can be interpreted through a bandable structure on the Cholesky factor of the precision matrix. However, the minimax theory has still been largely unknown, as opposed to the well established minimax results over the corresponding bandable covariance matrices. In this paper, we focus on two commonly used types of parameter spaces, and develop the optimal rates of convergence under both the operator norm and the Frobenius norm. A striking phenomenon is found: two types of parameter spaces are fundamentally different under the operator norm but enjoy the same rate optimality under the Frobenius norm, which is in sharp contrast to the equivalence of corresponding two types of bandable covariance matrices under both norms. This fundamental difference is established by carefully constructing the corresponding minimax lower bounds. Two new estimation procedures are developed: for the operator norm, our optimal procedure is based on a novel local cropping estimator targeting on all principle submatrices of the precision matrix while for the Frobenius norm, our optimal procedure relies on a delicate regression-based thresholding rule. Lepski's method is considered to achieve optimal adaptation. We further establish rate optimality in the nonparanormal model. Numerical studies are carried out to confirm our theoretical findings

    SU(2) x SU(2) x U(1) Interpretation on the 750 GeV Diphoton Excess

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    We propose that the SU(2) x SU(2) x U(1) (aka G221) models could provide us a 750 GeV scalar resonance that may account for the diphoton excess observed at the LHC while satisfying present collider constraints. The neutral component of the SU(2)RSU(2)_R scalar multiplet can be identified as the 750 GeV scalar. In the lepto-phobic and fermio-phobic G221 models the new charged gauge boson W' could be light, and we find that the diphoton decay width could be dominated by the loop contribution from the Wβ€²W'. To initiate gluon fusion production, it is necessary to extend the G221 symmetry to the Pati-Salam and SO(10) symmetry. We investigate the possibilities that the light colored scalars or vectorlike fermions survive in the SO(10) theory and provide large gluon fusion rate for the diphoton signature. It is possible to test the G221 interpretation by direct searches of W' using the multi-gauge boson production channel at the Run 2 LHC.Comment: 26 pages, 3 figures, 2 table

    Space-Distribution PDEs for Path Independent Additive Functionals of McKean-Vlasov SDEs

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    Let P2(Rd) be the space of probability measures on Rd with finite second moment. The path independence of additive functionals of McKean-Vlasov SDEs is characterized by PDEs on the product space Rd*P2(Rd) equipped with the usual derivative in space variable and Lions derivative in distribution. These PDEs are solved by using probabilis- tic arguments developed from [2]. In particular, the path independence of the Girsanov transformation killing the drift term is identified with a nonlinear PDE on Rd*P2(Rd), which includes corresponding results derived earlier for the classical SDEs as special situations.Comment: 17 PAGE

    Model-independent Probe of anomalous heavy neutral Higgs bosons at the LHC

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    We first formulate, in the framework of effective Lagrangian, the general form of the effective interactions of the lightest Higgs boson h and a heavier neutral Higgs boson H in a multi-Higgs system taking account of Higgs mixing effect. We regard h as the discovered Higgs boson which has been shown to be consistent with the standard model (SM) Higgs boson. The obtained effective interactions contain extra parameters reflecting the Higgs mixing effect. Next, We study the constraints on the anomalous coupling constants of H from both the requirement of the unitarity of the S matrix and the exclusion bounds on the SM Higgs boson obtained from the experimental data at the 7--8 TeV LHC. From this we obtain the available range of the anomalous coupling constants of H, with which H is not excluded by the yet known theoretical and experimental constraints. We then study the signatures of H at the 14 TeV LHC. In this paper, we suggest taking weak-boson scattering and pp to VH* to VVV as sensitive processes for probing H model independently at the 14 TeV LHC. We take several examples with the anomalous HVV coupling constants in the available ranges to do the numerical study. a full tree-level calculation at the hadron level is given with signals and backgrounds carefully calculated. We impose a series of proper kinematic cuts to effectively suppress the backgrounds. It is shown that, in both the VV scattering and the pp to VH* to VVV processes, H boson can be discovered from the invariant mass distributions of the final state particles with reasonable integrated luminosity. Especially, in the pp to VH* to VVV process, the invariant mass distribution of the final state jets can show a clear resonance peak of H. Finally, we propose several physical observables from which the values of the anomalous coupling constants f_W and f_{WW} can be measured experimentally.Comment: revtex4, 25pages, with 21 eps files for 21 figures. Tp appear in Phys. Rev. D 90 (2014

    Further Investigation on Model-Independent Probe of Heavy Neutral Higgs Bosons at the LHC Run 2

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    In our previous paper, we provided general effective Higgs interactions for the lightest Higgs boson hh (SM-like) and a heavier neutral Higgs boson HH based on the effective Lagrangian formulation up to the dim-6 interactions, and then proposed two sensitive processes for probing HH. We showed in several examples that the resonance peak of HH and its dim-6 effective coupling constants (ECC) can be detected at the LHC Run 2 with reasonable integrated luminosity. In this paper, we further perform a more thorough study of the most sensitive process, ppβ†’VHβˆ—β†’VVVpp\to VH^\ast\to VVV, on the information about the relations between the 1Οƒ, 3Οƒ, 5Οƒ1\sigma,\,3\sigma,\,5\sigma statistical significance and the corresponding ranges of the Higgs ECC for an integrated luminosity of 100 fbβˆ’1^{-1}. These results have two useful applications in the LHC Run 2: (A) realizing the experimental determination of the ECC in the dim-6 interactions if HH is found and, (B) obtaining the theoretical exclusion bounds if HH is not found. Some alternative processes sensitive for certain ranges of the ECC are also analyzed.Comment: 10 pages, 12 figures, to be submitted to Chinese Physics

    Fermions tunnelling with quantum gravity correction

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    Quantum gravity correction is truly important to study tunnelling process of black hole. Base on the generalized uncertainty principle, we investigate the influence of quantum gravity and the result tell us that the quantum gravity correction accelerates the evaporation of black hole. Using corrected Dirac equation in curved spacetime and Hamilton-Jacobi method, we address the tunnelling of fermions in a 4-dimensional Schwarzschild spacetime. After solving the equation of motion of the spin 1/2 field, we obtain the corrected Hawking temperature. It turns out that the correction depends not only on the mass of black hole but aslo on the mass of emitted fermions. In our calculation, the quantum gravity correction accelerates the increasing of Hawking temperature during the radiation explicitly. This correction leads to the increasing of the evaporation of black hole.Comment: 5page

    3D Contouring for Breast Tumor in Sonography

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    Malignant and benign breast tumors present differently in their shape and size on sonography. Morphological information provided by tumor contours are important in clinical diagnosis. However, ultrasound images contain noises and tissue texture; clinical diagnosis thus highly depends on the experience of physicians. The manual way to sketch three-dimensional (3D) contours of breast tumor is a time-consuming and complicate task. If automatic contouring could provide a precise breast tumor contour that might assist physicians in making an accurate diagnosis. This study presents an efficient method for automatically contouring breast tumors in 3D sonography. The proposed method utilizes an efficient segmentation procedure, i.e. level-set method (LSM), to automatic detect contours of breast tumors. This study evaluates 20 cases comprising ten benign and ten malignant tumors. The results of computer simulation reveal that the proposed 3D segmentation method provides robust contouring for breast tumor on ultrasound images. This approach consistently obtains contours similar to those obtained by manual contouring of the breast tumor and can save much of the time required to sketch precise contours.Comment: 18 pages, 1 table and 5 figure

    Distance and distance signless Laplacian spread of connected graphs

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    For a connected graph GG on nn vertices, recall that the distance signless Laplacian matrix of GG is defined to be Q(G)=Tr(G)+D(G)\mathcal{Q}(G)=Tr(G)+\mathcal{D}(G), where D(G)\mathcal{D}(G) is the distance matrix, Tr(G)=diag(D1,D2,…,Dn)Tr(G)=diag(D_1, D_2, \ldots, D_n) and DiD_{i} is the row sum of D(G)\mathcal{D}(G) corresponding to vertex viv_{i}. Denote by ρD(G),\rho^{\mathcal{D}}(G), ρminD(G)\rho_{min}^{\mathcal{D}}(G) the largest eigenvalue and the least eigenvalue of D(G)\mathcal{D}(G), respectively. And denote by qD(G)q^{\mathcal{D}}(G), qminD(G)q_{min}^{\mathcal{D}}(G) the largest eigenvalue and the least eigenvalue of Q(G)\mathcal{Q}(G), respectively. The distance spread of a graph GG is defined as SD(G)=ρD(G)βˆ’ΟminD(G)S_{\mathcal{D}}(G)=\rho^{\mathcal{D}}(G)- \rho_{min}^{\mathcal{D}}(G), and the distance signless Laplacian spread of a graph GG is defined as SQ(G)=qD(G)βˆ’qminD(G)S_{\mathcal{Q}}(G)=q^{\mathcal{D}}(G)-q_{min}^{\mathcal{D}}(G). In this paper, we point out an error in the result of Theorem 2.4 in "Distance spectral spread of a graph" [G.L. Yu, et al, Discrete Applied Mathematics. 160 (2012) 2474--2478] and rectify it. As well, we obtain some lower bounds on ddistance signless Laplacian spread of a graph

    Noise and chaotic disturbance on self-similar set

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    The effect of noise on self-similar set is studied. The iteratie procedure used to generate the self-similar set is moidified by adding a stochastic variable to the diameter of generating sets at each iteration. The noise may causes the generating set to collapse to a point. Distribution functions are found describing the probability that any generating set collapse. The effect of chaotic disturbance on the iteration of self-similar set is studied. It is shown that the iterative procedure which describes the self-similar set is truncated under the influence of disturbance generated by the tent map. Conditions which lead to truncation of any chaotic map are also obtained.Comment: 9 pages with no figure
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