173,835 research outputs found

    First Principles Modeling of the Initial Stages of Organic Solvent Decomposition on Li(x)Mn(2)O(4) (100) Surfaces

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    Density functional theory and ab initio molecular dynamics simulations are applied to investigate the initial steps of ethylene carbonate (EC) decomposition on spinel Li(0.6)Mn(2)O(4) (100) surfaces. EC is a key component of the electrolyte used in lithium ion batteries. We predict an slightly exothermic EC bond breaking event on this oxide facet, which facilitates subsequent EC oxidation and proton transfer to the oxide surface. Both the proton and the partially decomposed EC fragment weaken the Mn-O ionic bonding network. Implications for interfacial film made of decomposed electrolyte on cathode surfaces, and Li(x)Mn(2)O(4) dissolution during power cycling, are discussed.Comment: 29 pages preprint format, 7 figure

    Constant threshold correction to electrically charged dilatonic black holes

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    We investigate the effect of a constant threshold correction to a general non-extreme, static, spherically symmetric, electrically charged black hole solution of the dilatonic Einstein-Maxwell Lagrangian, with an arbitrary coupling β\beta between the electromagnetic tensor and the dilaton field. For a small β\beta, an exact analytical solution is obtained. For an arbitrary β\beta, a close form solution, up to first order in the threshold correction, of the metric and the dilaton are presented. In the extremal limit, the close form solution is reduced to an exact analytical form.Comment: LaTex with RevTex, 8 page

    Purely non-atomic weak L^p spaces

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    Let \msp be a purely non-atomic measure space, and let 1<p<1 < p < \infty. If \weakLp\msp is isomorphic, as a Banach space, to \weakLp\mspp for some purely atomic measure space \mspp, then there is a measurable partition Ω=Ω1Ω2\Omega = \Omega_1\cup\Omega_2 such that (Ω1,ΣΩ1,μΣΩ1)(\Omega_1,\Sigma\cap\Omega_1,\mu_{|\Sigma\cap\Omega_1}) is countably generated and σ\sigma-finite, and that μ(σ)=0\mu(\sigma) = 0 or \infty for every measurable σΩ2\sigma \subseteq \Omega_2. In particular, \weakLp\msp is isomorphic to p,\ell^{p,\infty}
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