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Optimal-order bounds on the rate of convergence to normality in the multivariate delta method

机译:多元delta方法中收敛至正态率的最优阶界

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Uniform and nonuniform Berry–Esseen (BE) bounds of optimal orders on the rate of convergence to normality in the delta method for vector statistics are obtained. The results are applicable almost as widely as the delta method itself – except that, quite naturally, the order of the moments needed to be finite is generally $3/2$ times as large as that for the corresponding central limit theorems. Our BE bounds appear new even for the one-dimensional delta method, that is, for smooth functions of the sample mean of univariate random variables. Specific applications to Pearson’s, noncentral Student’s and Hotelling’s statistics, sphericity test statistics, a regularized canonical correlation, and maximum likelihood estimators (MLEs) are given; all these uniform and nonuniform BE bounds appear to be the first known results of these kinds, except for uniform BE bounds for MLEs. The new method allows one to obtain bounds with explicit and rather moderate-size constants. For instance, one has the uniform BE bound $3.61mathbb{E}(Y_{1}^{6}+Z_{1}^{6}),(1+sigma^{-3})/sqrt{n}$ for the Pearson sample correlation coefficient based on independent identically distributed random pairs $(Y_{1},Z_{1}),dots,(Y_{n},Z_{n})$ with $mathbb{E} Y_{1}=mathbb{E}Z_{1}=mathbb{E}Y_{1}Z_{1}=0$ and $mathbb{E}Y_{1}^{2}=mathbb{E}Z_{1}^{2}=1$, where $sigma:=sqrt{mathbb{E}Y_{1}^{2}Z_{1}^{2}}$.
机译:在用于矢量统计的增量方法中,获得了关于最优收敛阶收敛于正态速率的最优阶的一致和不一致Berry-Esseen(BE)界。结果的适用范围几乎与delta方法本身一样广泛-除非自然而然,所需的有限阶数通常是相应中心极限定理的3/2美元乘以。即使对于一维delta方法,即对于单变量随机变量的样本均值的平滑函数,我们的BE边界也显得很新。给出了Pearson,非中心学生和Hotelling统计,球形测试统计,正则规范相关和最大似然估计(MLE)的特定应用;除了MLE的统一BE边界外,所有这些统一的和非统一的BE边界似乎都是此类的第一个已知结果。新方法允许人们获得带有显式且大小适中的常数的边界。例如,某人的统一BE绑定为$ 3.61 mathbb {E}(Y_ {1} ^ {6} + Z_ {1} ^ {6}),(1+ sigma ^ {-3})/ sqrt {n} $用于基于独立的相同分布的随机对$(Y_ {1},Z_ {1}), dots,(Y_ {n},Z_ {n})$和$ mathbb { E} Y_ {1} = mathbb {E} Z_ {1} = mathbb {E} Y_ {1} Z_ {1} = 0 $和$ mathbb {E} Y_ {1} ^ {2} = mathbb {E} Z_ {1} ^ {2} = 1 $,其中$ sigma:= sqrt { mathbb {E} Y_ {1} ^ {2} Z_ {1} ^ {2}} $。

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