1,947 research outputs found

    The behavior of the NPMLE of a decreasing density near the boundaries of the support

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    We investigate the behavior of the nonparametric maximum likelihood estimator f^n\hat{f}_n for a decreasing density ff near the boundaries of the support of ff. We establish the limiting distribution of f^n(n−α)\hat{f}_n(n^{-\alpha}), where we need to distinguish between different values of 0<α<10<\alpha<1. Similar results are obtained for the upper endpoint of the support, in the case it is finite. This yields consistent estimators for the values of ff at the boundaries of the support. The limit distribution of these estimators is established and their performance is compared with the penalized maximum likelihood estimator.Comment: Published at http://dx.doi.org/10.1214/009053606000000100 in the Annals of Statistics (http://www.imstat.org/aos/) by the Institute of Mathematical Statistics (http://www.imstat.org

    Asymptotic normality of the LkL_k-error of the Grenander estimator

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    We investigate the limit behavior of the LkL_k-distance between a decreasing density ff and its nonparametric maximum likelihood estimator f^n\hat{f}_n for k≥1k\geq1. Due to the inconsistency of f^n\hat{f}_n at zero, the case k=2.5k=2.5 turns out to be a kind of transition point. We extend asymptotic normality of the L1L_1-distance to the LkL_k-distance for 1≤k<2.51\leq k<2.5, and obtain the analogous limiting result for a modification of the LkL_k-distance for k≥2.5k\geq2.5. Since the L1L_1-distance is the area between ff and f^n\hat{f}_n, which is also the area between the inverse gg of ff and the more tractable inverse UnU_n of f^n\hat{f}_n, the problem can be reduced immediately to deriving asymptotic normality of the L1L_1-distance between UnU_n and gg. Although we lose this easy correspondence for k>1k>1, we show that the LkL_k-distance between ff and f^n\hat{f}_n is asymptotically equivalent to the LkL_k-distance between UnU_n and gg.Comment: Published at http://dx.doi.org/10.1214/009053605000000462 in the Annals of Statistics (http://www.imstat.org/aos/) by the Institute of Mathematical Statistics (http://www.imstat.org

    On the upper limit of antinuclei content in cosmic rays

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    Upper limit of antinuclei content in cosmic ray

    Magnetic degeneracy and hidden metallicity of the spin density wave state in ferropnictides

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    We analyze spin density wave (SDW) order in iron-based superconductors and electronic structure in the SDW phase. We consider an itinerant model for Fe-pnictides with two hole bands centered at (0,0)(0,0) and two electron bands centered at (0,π)(0,\pi) and (π,0)(\pi,0) in the unfolded BZ. A SDW order in such a model is generally a combination of two components with momenta (0,π)(0,\pi) and (π,0)(\pi,0), both yield (π,π)(\pi,\pi) order in the folded zone. Neutron experiments, however, indicate that only one component is present. We show that (0,π)(0,\pi) or (π,0)(\pi,0) order is selected if we assume that only one hole band is involved in the SDW mixing with electron bands. A SDW order in such 3-band model is highly degenerate for a perfect nesting and hole-electron interaction only, but we show that ellipticity of electron pockets and interactions between electron bands break the degeneracy and favor the desired (0,π)(0,\pi) or (π,0)(\pi,0) order. We further show that stripe-ordered system remains a metal for arbitrary coupling. We analyze electronic structure for parameters relevant to the pnictides and argue that the resulting electronic structure is in good agreement with ARPES experiments. We discuss the differences between our model and J1−J2J_1-J_2 model of localized spins.Comment: reference list updated, typos are correcte

    Interplay between magnetism and superconductivity in Fe-pnictides

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    We consider phase transitions and potential co-existence of spin-density-wave (SDW) magnetic order and extended s-wave (s+s^+) superconducting order within a two-band itinerant model of iron pnictides, in which SDW magnetism and s+s^+ superconductivity are competing orders. We show that depending on parameters, the transition between these two states is either first order, or involves an intermediate phase in which the two orders co-exist. We demonstrate that such co-existence is possible when SDW order is incommensurate.Comment: 5 pages, 3 figure
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