• Journal of the Korean Statistical Society
• /
• 제20권1호
• /
• pp.67-76
• /
• 1991

The empirical Bayes version involves ″independent″ repetitions(a sequence) of the component decision problem. With the varying sample size possible, these are not identical components. However, we impose the usual assumption that the parameters sequence $\theta$=($\theta$$_1$, $\theta$$_2$, …) consists of independent G-distributed parameters where G is unknown. We assume that G $\in$ g, a known family of distributions. The sample size $N_i$ and the decisin rule $d_i$ for component i of the sequence are determined in an evolutionary way. The sample size $N_1$ and the decision rule $d_1$$\in$ $D_{N1}$ used in the first component are fixed and chosen in advance. The sample size $N_2$and the decision rule $d_2$ are functions of *see full text($\underline{X}^1$equation omitted), the observations in the first component. In general, $N_i$ is an integer-valued function of *see full text(equation omitted) and, given $N_i$, $d_i$ is a $D_{Ni}$/-valued function of *see full text(equation omitted). The action chosen in the i-th component is *(equation omitted) which hides the display of dependence on *(equation omitted). We construct an empirical Bayes decision rule for estimating normal mean and show that it is asymptotically optimal.

• 한국전기전자재료학회:학술대회논문집
• /
• 한국전기전자재료학회 2000년도 추계학술대회 논문집
• /
• pp.355-358
• /
• 2000

Magnetoresistance changes of NiFe thin films were investigated as a function of deposition temperature. DC magnetron sputtering was employed to fabricate Ta/NiFe(t)/Ta thin films on Si(001) substrates with in-situ field or with no-field. The thickness(t) of NiFe films was a range of 4 to 15nm. Substrate temperature was a range of 30 to 400$^{\circ}C$. MR measurement was carried out as a function of angle $\theta$, between external field and current direction. MR ratio increased with increasing substrate temperature, also, max. MR ratio was observed in samples deposited at 300$^{\circ}C$. With increasing upto 400$^{\circ}C$, MR ratio was rapidly decreased in the case of thinner NiFe films. In non-field deposited NiFe films, both angle $\theta$=0, 90。, there was no significant change in MR curves. However, MR curves of in-situ field deposited NiFe films were different in both angles $\theta$=0 and 90。

• Journal of the Korean Statistical Society
• /
• 제25권1호
• /
• pp.95-110
• /
• 1996

We consider the question of efficiency of the Bayes sequential procedure with respect to the optimal fixed sample size Bayes procedure in a simple vs. simple testing problem for data coming from a general nonregular density b(.theta.)h(x)l(x < .theta.). Efficiency is defined in two different ways in these caiculations. Also, the minimax sequential risk (and minimax sequential stratage) is studied as a function of the cost of sampling.

• Journal of Information Science Theory and Practice
• /
• 제1권3호
• /
• pp.6-11
• /
• 2013

A new explanation, using exponential functions, is given for the S-shaped functional relation between the mean citation score and the proportion of top 10% (and other percentages) publications for the 500 Leiden Ranking universities. With this new model we again obtain an explanation for the concave or convex relation between the proportion of top $100{\theta}%$ publications, for different fractions of ${\theta}$.

• 대한안전경영과학회지
• /
• 제2권2호
• /
• pp.71-83
• /
• 2000

This paper presents accelerated life tests for Type I censoring data under probabilistic stresses. Probabilistic stress, $S_j$, is the random variable for stress influenced by test environments, test equipments, sampling devices and use conditions. The hazard rate, ,$theta_j$, is the random variable of environments and the function of probabilistic stress. Also it is assumed that the general stress distribution is uniform, the life distribution for the given hazard rate, $\theta$, is exponential and inverse power law model holds. In this paper, we obtained maximum likelihood estimators of model parameters and the mean life in use stress condition.

• 대한수학회보
• /
• 제53권6호
• /
• pp.1831-1844
• /
• 2016

In this paper, we improve the full-Newton step infeasible interior-point algorithm proposed by Mansouri et al. [6]. The algorithm takes only one full-Newton step in a major iteration. To perform this step, the algorithm adopts the largest logical value for the barrier update parameter ${\theta}$. This value is adapted with the value of proximity function ${\delta}$ related to (x, y, s) in current iteration of the algorithm. We derive a suitable interval to change the parameter ${\theta}$ from iteration to iteration. This leads to more flexibilities in the algorithm, compared to the situation that ${\theta}$ takes a default fixed value.

• 대한수학회보
• /
• 제50권3호
• /
• pp.761-766
• /
• 2013

We derive several modular equations and present their proofs based on concise algebraic computations. In addition, we establish explicit relations and formulas for some parameterizations for the theta functions ${\varphi}$ and ${\psi}$ and show some applications of the modular equations to evaluations of the cubic continued fraction and the theta function ${\psi}$.

• Journal of the Korean Statistical Society
• /
• 제24권2호
• /
• pp.337-347
• /
• 1995

In the problem of some sequential estimation, the stopping times may be written in the form $N(c) = inf{n \geq n_0; n \geq c^2 S^2_n/\delta^2 (\bar{X}_n)}$ where ${s^2_n}$ and ${\bar{X}_n}$ are the sequences of sample variance and sample mean of the independently and identically distributed (i.i.d.) random variables with distribution $F_{\theta}(x), \theta \in \Theta$, respectively, and $\delta$ is either constant or any given positive real valued function. We obtain some asymptotic normality and asymptotic expectation of the N(c) in various limiting situations. Specially, uniform asymptotic normality and uniform asymptotic expectation of the N(c) are given.

• 한국토양비료학회지
• /
• 제23권1호
• /
• pp.8-14
• /
• 1990

토양수분함량(土壤水分含量)이 다른 조건(條件)에서 물이 이동(移動)할 때 동반(同伴)되는 용질(溶質)의 이동특성(移動特性)을 결정(決定)하는 지연계수(遲延係數)와 수리동적(水理動的) 분산계수(分散係數)를 수학적(數學的)으로 해석(解析)하고 일차원수평계(一次元水平系)의 사양토(砂壤土)에서 실험적(實驗的)으로 측정(測定)하였다. 용적밀도(容積密度)를 $1,350{\pm}50kg/m^3$인 사양토(砂壤土) 토양(土壤)에 수평(水平)으로 침투(浸透)되는 0.05% $CaSO_4$ 용액(溶液)의 수분전진(水分前進)을 Boltzman transform으로 나타내고 이를 표준(標準)으로 하였을 때 0.5% KCl, $CaCl_2$ 및 $KH_2PO_4$ 용액(溶液)의 용질전진(溶質前進)을 비농도(比濃度)로 표시(表示)하여 비교(比較)하였다. 용질농도(溶質濃度)의 분포(分布)와 수분분포(水分分布)로 부터 Laryea법(法)에 의하여 수리동적(水理動的) 분산계수(分散係數)를 계산(計算)하였다. 토양(土壤)-용액계(溶液系)에서 비반응성(比反應性) 용질(溶質)인 $Cl^-$의 전진(前進)은 물의 전진(前進)보다 늦었으며, 음(陰)ion 배제효과(排除效果)는 무시(無視)되었고 지연(遲延)은 초기수분함량(初期水分含量) ${\theta}_n$의 함수(函數)로 ${\theta}/({\theta}-{\theta}_n)$로 해석(解析)되었다. 토양입자(土壤粒子)에 의하여 흡착(吸着)이 일어나는 $K^+$, $Ca^{{+}{+}}$, $H_2PO^-_4$의 전진(前進)은 초기수분함량(初期水分含量)과 지연계수(遲延係數) R의 함수(函數)로 $\frac{1}{1+R}{\cdot}\frac{{\theta}}{{\theta}-{\theta}_n}$으로 해석(解析)되며 R치(値)는 $Cl^-$를 1.0으로 보았을 때 $K^+$는 0.64, 0.80 및 2.6이었다. Langmuir 등온흡착식(等溫吸着式)을 이용(利用)한 지연계수(遲延係數) 계산(計算)은 다소의 차이(差異)가 있었으나 적용가능성(適用可能性)이 있었다. 수분분포곡선(水分分布曲線)으로부터 산출(算出)된 물의 확산계수(擴散係數) $D({\theta})$는 초기수분함량(初期水分含量)에 관계(關係)없이 토양수분함량(土壤水分含量)과 단일지수함수관계(單一指數函數關係)로 표시(表示)되었다. $$log\;D({\theta})=13.448{\theta}-9.288$$ $Cl^-$의 수리동적분포계수(水理動的分布係數)는 수분함량(水分含量) 0.36 이상(以上)에서는 물의 확산계수(擴散係數)와 비슷하였고 그 이하(以下)에서는 급격히(急激)히 감소(減少)하여 수분함량(水分含量) 0.2부근에서 자기확산계수(自己擴散係數)와 비슷한 값을 보였다. $K^+$, $Ca^{{+}{+}}$ 및 $H_2PO^-_4$의 수리동적분산계수(水理動的分散係數)는 수분함량(水分含量) 0.38에서 각각(各各) $5.5{\times}10^{-6}$, $2.4{\times}10^{-6}$ 및 $7.1{\times}10^{-7}m^2/sec$의 값을 보였고 0.36% 이하(以下)의 수분함량(水分含量)에서 급격(急激)히 감소(減少)하였으며 감소(減少) 경향(傾向)은 $H_2PO^-_4$가 가장 심(甚)하였다.

• Journal of Ecology and Environment
• /
• 제33권2호
• /
• pp.165-173
• /
• 2010

Soil respiration ($R_S$) is a critical component of the annual carbon balance of forests, but few studies thus far have attempted to evaluate empirical regression models in $R_S$. The principal objectives of this study were to evaluate the relationship between $R_S$ rates and soil temperature (ST) and soil water content (SWC) in soil from a cool-temperate deciduous broad-leaved forest, and to evaluate empirical regression models for the prediction of $R_S$ using ST and SWC. We have been measuring $R_S$, using an open-flow gas-exchange system with an infrared gas analyzer during the snowfree season from 1999 to 2001 at the Takayama Forest, Japan. To evaluate the empirical regression models used for the prediction of $R_S$, we compared a simple exponential regression (flux = $ae^{bt}$Eq. [1]) and two polynomial multiple-regression models (flux = $ae^{bt}{\times}({\theta}{\nu}-c){\times}(d-{\theta}{\nu})^f:$ Eq. [2] and flux = $ae^{bt}{\times}(1-(1-({\theta}{\nu}/c))^2)$: Eq. [3]) that included two variables (ST: t and SWC: ${\theta}{\nu}$) and that utilized hourly data for $R_S$. In general, daily mean $R_S$ rates were positively well-correlated with ST, but no significant correlations were observed with any significant frequency between the ST and $R_S$ rates on periods of a day based on the hourly $R_S$ data. Eq. (2) has many more site-specific parameters than Eq. (3) and resulted in some significant underestimation. The empirical regression, Eq. (3) was best explained by temporal variations, as it provided a more unbiased fit to the data compared to Eq. (2). The Eq. (3) (ST $\times$ SWC function) also increased the predictive ability as compared to Eq. (1) (only ST exponential function), increasing the $R^2$ from 0.71 to 0.78.