67,681 research outputs found

    Convergence of Adaptive Finite Element Approximations for Nonlinear Eigenvalue Problems

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    In this paper, we study an adaptive finite element method for a class of a nonlinear eigenvalue problems that may be of nonconvex energy functional and consider its applications to quantum chemistry. We prove the convergence of adaptive finite element approximations and present several numerical examples of micro-structure of matter calculations that support our theory.Comment: 24 pages, 12 figure

    First-principles study of native point defects in Bi2Se3

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    Using first-principles method within the framework of the density functional theory, we study the influence of native point defect on the structural and electronic properties of Bi2_2Se3_3. Se vacancy in Bi2_2Se3_3 is a double donor, and Bi vacancy is a triple acceptor. Se antisite (SeBi_{Bi}) is always an active donor in the system because its donor level (ε\varepsilon(+1/0)) enters into the conduction band. Interestingly, Bi antisite(BiSe1_{Se1}) in Bi2_2Se3_3 is an amphoteric dopant, acting as a donor when μ\mue_e<<0.119eV (the material is typical p-type) and as an acceptor when μ\mue_e>>0.251eV (the material is typical n-type). The formation energies under different growth environments (such as Bi-rich or Se-rich) indicate that under Se-rich condition, SeBi_{Bi} is the most stable native defect independent of electron chemical potential μ\mue_e. Under Bi-rich condition, Se vacancy is the most stable native defect except for under the growth window as μ\mue_e>>0.262eV (the material is typical n-type) and Δ\Deltaμ\muSe_{Se}<<-0.459eV(Bi-rich), under such growth windows one negative charged BiSe1_{Se1} is the most stable one.Comment: 7 pages, 4 figure

    Dark viscous fluid described by a unified equation of state in cosmology

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    We generalize the Λ\LambdaCDM model by introducing a unified EOS to describe the Universe contents modeled as dark viscous fluid, motivated by the fact that a single constant equation of state (EOS) p=p0p=-p_0 (p0>0p_0>0) reproduces the Λ\LambdaCDM model exactly. This EOS describes the perfect fluid term, the dissipative effect, and the cosmological constant in a unique framework and the Friedmann equations can be analytically solved. Especially, we find a relation between the EOS parameter and the renormalizable condition of a scalar field. We develop a completely numerical method to perform a χ2\chi^2 minimization to constrain the parameters in a cosmological model directly from the Friedmann equations, and employ the SNe data with the parameter A\mathcal{A} measured from the SDSS data to constrain our model. The result indicates that the dissipative effect is rather small in the late-time Universe.Comment: 4 pages, 2 figures. v2: new materials added. v3: matches the version to appear in IJMP

    CP violation in J/ψΛΛˉJ/\psi \rightarrow \Lambda \bar \Lambda

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    We study CP violation in J/ψΛΛˉJ/\psi \rightarrow \Lambda \bar{\Lambda} decay. This decay provides a good place to look for CP violation. Some observables are very sensitive to the Λ\Lambda electric dipole moment dΛd_\Lambda and therefore can be used to improve the experimental upper bound on dΛd_\Lambda. CP violations in the lepton pair decays of J/ψJ/\psi and Υ\Upsilon are also discussed.Comment: 8 pages, RevTex, UM-P-92/113, OZ-92/3

    Partially linear censored quantile regression

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    Censored regression quantile (CRQ) methods provide a powerful and flexible approach to the analysis of censored survival data when standard linear models are felt to be appropriate. In many cases however, greater flexibility is desired to go beyond the usual multiple regression paradigm. One area of common interest is that of partially linear models: one (or more) of the explanatory covariates are assumed to act on the response through a non-linear function. Here the CRQ approach of Portnoy (J Am Stat Assoc 98:1001–1012, 2003) is extended to this partially linear setting. Basic consistency results are presented. A simulation experiment and unemployment example justify the value of the partially linear approach over methods based on the Cox proportional hazards model and on methods not permitting nonlinearity
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