17,481 research outputs found

    Light pseudoscalar eta and H->eta eta decay in the simplest little Higgs mode

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    The SU(3) simplest little Higgs model in its original framework without the so-called mu term inevitably involves a massless pseudoscalar boson eta, which is problematic for b-physics and cosmological axion limit. With the mu term introduced by hand, the eta boson acquires mass m_eta ~ mu, which can be lighter than half the Higgs boson mass in a large portion of the parameter space. In addition, the introduced mu term generates sizable coupling of H-eta-eta. The Higgs boson can dominantly decay into a pair of eta's especially when mH below the WW threshold. Another new decay channel of H->Z+eta can be dominant or compatible with H -> WW for mH above the Z+eta threshold. We show that the LEP bound on the Higgs boson mass is loosened to some extent due to this new H->eta eta decay channel as well as the reduced coupling of H-Z-Z. The Higgs boson mass bound falls to about 110 GeV for f=3-4 TeV. Since the eta boson decays mainly into a bb pair, H-> eta eta -> 4b and H-> Z eta -> Z bb open up other interesting search channels in the pursuit of the Higgs boson in the future experiments. We discuss on these issues.Comment: major modification considering the simplest little Higgs model with the mu ter

    Entropy and Its Quantum Thermodynamical Implication for Anomalous Spectral Systems

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    The state function entropy and its quantum thermodynamical implication for two typical dissipative systems with anomalous spectral densities are studied by investigating on their low-temperature quantum behavior. In all cases it is found that the entropy decays quickly and vanishes as the temperature approaches zero. This reveals a good conformity with the third law of thermodynamics and provides another evidence for the validity of fundamental thermodynamical laws in the quantum dissipative region.Comment: 10 pages, 3 figure

    Fluidized-bed heat treating equipment

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    Improving Whole Slide Segmentation Through Visual Context - A Systematic Study

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    While challenging, the dense segmentation of histology images is a necessary first step to assess changes in tissue architecture and cellular morphology. Although specific convolutional neural network architectures have been applied with great success to the problem, few effectively incorporate visual context information from multiple scales. With this paper, we present a systematic comparison of different architectures to assess how including multi-scale information affects segmentation performance. A publicly available breast cancer and a locally collected prostate cancer datasets are being utilised for this study. The results support our hypothesis that visual context and scale play a crucial role in histology image classification problems

    A protocol for Agrobacterium-mediated transformation of Kalanchoë blossfeldiana with a flavonoid 3',5' hydroxylase (F3'5'H) gene

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    In the present investigation, explants from Kalanchoë blossfeldiana were used for gene transformation. The young leaves were inoculated with Agrobacterium tumefaciens LBA4404 strain with a binary vector plasmid pArtblue containing F3'5'H gene under control of CaMV35S promoter and nptII selectable marker gene. After inoculation, the explants were transferred to the co-cultivation medium. They were then transferred to the selection medium containing kanamycin and were sub-cultured every two weeks. Leaves of the putative transgenic shoots that survived in the selection medium were used in reverse transcription polymerase chain reaction (RT-PCR) analysis to detect gene expression. The RT-PCR analysis showed the presence of 550 bp F3'5'H amplification products and had an expression of F3'5'H gene. Plants with the introduced F3'5'H gene produced totally pale red flowers.Key words: Kalanchoë blossfeldiana, Agrobacterium-mediated transformation, young leaf, F3'5'H gene, reverse transcription-polymerase chain reaction (RT-PCR)

    One-dimensional vertical dust strings in a glass box

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    The oscillation spectrum of a one-dimensional vertical dust string formed inside a glass box on top of the lower electrode in a GEC reference cell was studied. A mechanism for creating a single vertical dust string is described. It is shown that the oscillation amplitudes, resonance frequencies, damping coefficients, and oscillation phases of the dust particles separate into two distinct groups. One group exhibits low damping coefficients, increasing amplitudes and decreasing resonance frequencies for dust particles closer to the lower electrode. The other group shows high damping coefficients but anomalous resonance frequencies and amplitudes. At low oscillation frequencies, the two groups are also separated by a {\pi}-phase difference. One possible cause for the difference in behavior between the two groups is discussed

    New Results for Diffusion in Lorentz Lattice Gas Cellular Automata

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    New calculations to over ten million time steps have revealed a more complex diffusive behavior than previously reported, of a point particle on a square and triangular lattice randomly occupied by mirror or rotator scatterers. For the square lattice fully occupied by mirrors where extended closed particle orbits occur, anomalous diffusion was still found. However, for a not fully occupied lattice the super diffusion, first noticed by Owczarek and Prellberg for a particular concentration, obtains for all concentrations. For the square lattice occupied by rotators and the triangular lattice occupied by mirrors or rotators, an absence of diffusion (trapping) was found for all concentrations, except on critical lines, where anomalous diffusion (extended closed orbits) occurs and hyperscaling holds for all closed orbits with {\em universal} exponents df=74{\displaystyle{d_f = \frac{7}{4}}} and Ï„=157{\displaystyle{\tau = \frac{15}{7}}}. Only one point on these critical lines can be related to a corresponding percolation problem. The questions arise therefore whether the other critical points can be mapped onto a new percolation-like problem, and of the dynamical significance of hyperscaling.Comment: 52 pages, including 18 figures on the last 22 pages, email: [email protected]

    Evolution equations of curvature tensors along the hyperbolic geometric flow

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    We consider the hyperbolic geometric flow ∂2∂t2g(t)=−2Ricg(t)\frac{\partial^2}{\partial t^2}g(t)=-2Ric_{g(t)} introduced by Kong and Liu [KL]. When the Riemannian metric evolve, then so does its curvature. Using the techniques and ideas of S.Brendle [Br,BS], we derive evolution equations for the Levi-Civita connection and the curvature tensors along the hyperbolic geometric flow. The method and results are computed and written in global tensor form, different from the local normal coordinate method in [DKL1]. In addition, we further show that any solution to the hyperbolic geometric flow that develops a singularity in finite time has unbounded Ricci curvature.Comment: 15 page

    Intersections of homogeneous Cantor sets and beta-expansions

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    Let Γβ,N\Gamma_{\beta,N} be the NN-part homogeneous Cantor set with β∈(1/(2N−1),1/N)\beta\in(1/(2N-1),1/N). Any string (jℓ)ℓ=1N(j_\ell)_{\ell=1}^\N with jℓ∈{0,±1,...,±(N−1)}j_\ell\in\{0,\pm 1,...,\pm(N-1)\} such that t=∑ℓ=1Njℓβℓ−1(1−β)/(N−1)t=\sum_{\ell=1}^\N j_\ell\beta^{\ell-1}(1-\beta)/(N-1) is called a code of tt. Let Uβ,±N\mathcal{U}_{\beta,\pm N} be the set of t∈[−1,1]t\in[-1,1] having a unique code, and let Sβ,±N\mathcal{S}_{\beta,\pm N} be the set of t∈Uβ,±Nt\in\mathcal{U}_{\beta,\pm N} which make the intersection Γβ,N∩(Γβ,N+t)\Gamma_{\beta,N}\cap(\Gamma_{\beta,N}+t) a self-similar set. We characterize the set Uβ,±N\mathcal{U}_{\beta,\pm N} in a geometrical and algebraical way, and give a sufficient and necessary condition for t∈Sβ,±Nt\in\mathcal{S}_{\beta,\pm N}. Using techniques from beta-expansions, we show that there is a critical point βc∈(1/(2N−1),1/N)\beta_c\in(1/(2N-1),1/N), which is a transcendental number, such that Uβ,±N\mathcal{U}_{\beta,\pm N} has positive Hausdorff dimension if β∈(1/(2N−1),βc)\beta\in(1/(2N-1),\beta_c), and contains countably infinite many elements if β∈(βc,1/N)\beta\in(\beta_c,1/N). Moreover, there exists a second critical point αc=[N+1−(N−1)(N+3) ]/2∈(1/(2N−1),βc)\alpha_c=\big[N+1-\sqrt{(N-1)(N+3)}\,\big]/2\in(1/(2N-1),\beta_c) such that Sβ,±N\mathcal{S}_{\beta,\pm N} has positive Hausdorff dimension if β∈(1/(2N−1),αc)\beta\in(1/(2N-1),\alpha_c), and contains countably infinite many elements if β∈[αc,1/N)\beta\in[\alpha_c,1/N).Comment: 23 pages, 4 figure
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