265,157 research outputs found

    Solid-solid transition of the size-polydisperse hard-sphere system

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    The solid-solid coexistence of a polydisperse hard sphere system is studied by using the Monte Carlo simulation. The results show that for large enough polydispersity the solid-solid coexistence state is more stable than the single-phase solid. The two coexisting solids have different composition distributions but the same crystal structure. Moreover, there is evidence that the solid-solid transition terminates in a critical point as in the case of the fluid-fluid transition.Comment: 9 pages, 4 figure

    A Remark on Soliton Equation of Mean Curvature Flow

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    In this short note, we consider self-similar immersions F:RnRn+kF: \mathbb{R}^n \to \mathbb{R}^{n+k} of the Graphic Mean Curvature Flow of higher co-dimension. We show that the following is true: Let F(x)=(x,f(x)),xRnF(x) = (x,f(x)), x \in \mathbb{R}^{n} be a graph solution to the soliton equation Hˉ(x)+F(x)=0. \bar{H}(x) + F^{\bot}(x) = 0. Assume supRnDf(x)C0<+\sup_{\mathbb{R}^{n}}|Df(x)| \le C_{0} < + \infty. Then there exists a unique smooth function f:RnRkf_{\infty}: \mathbb{R}^{n}\to \mathbb{R}^k such that f(x)=limλfλ(x) f_{\infty}(x) = \lim_{\lambda \to \infty}f_{\lambda}(x) and f(rx)=rf(x) f_{\infty}(r x)=r f_{\infty}(x) for any real number r0r\not= 0, where fλ(x)=λ1f(λx). f_{\lambda}(x) = \lambda^{-1}f(\lambda x). Comment: 6 page
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