Abstract
Gamma distributions are widely used in applied fields due to its flexibility of accommodating right-skewed data. Although inference methods for a single gamma mean have been well studied, research on the common mean of several gamma populations are sparse. This paper addresses the problem of confidence interval estimation of the common mean of several gamma populations using the concept of generalized inference and the method of variance estimates recovery (MOVER). Simulation studies demonstrate that several proposed approaches can provide confidence intervals with satisfying coverage probabilities even at small sample sizes. The proposed methods are illustrated using two examples.
Introduction
Due to its flexibility of accommodating right-skewed data, the standard two-parameter Gamma distribution has been widely used in many applied fields such as meteorology, reliability, medical science, engineering and quality control [1–4]. Under many circumstances, the research interest lies in making inference about the mean. There exit abundant research regarding making inference about gamma mean(s). For example, Fraser et al. [5] investigated inference methods for gamma mean based on asymptotic approximation, and Krishnamoorthy and León-Novelo [6] investigated small sample inference for gamma parameters for one-sample and two-sample problems. Recently, several fiducial methods [7–9] constructed approximate generalized pivotal quantities for a single gamma mean in different ways. Wang et al. [10] extended a fiducial approach [7] for a single gamma mean to construct a fiducial confidence interval for the difference between two independent gamma means.
There also exist some research on testing equality of several gamma means. For example, Chang et al. [11] proposed a parametric bootstrap method for comparing several gamma means, and Krishnamoorthy et al. [12] presented likelihood ratio test for comparing several gamma distributions. When testing equality of several gamma means concludes the null hypothesis (i.e. all the means are equal) can not be rejected, naturally, making inference about the common mean is of interest. Despite the fact that inference procedures about the common gamma means are of practical and theoretical importance, there has not yet been a well-developed approach for this purpose at small sample sizes except some traditional large sample methods. Therefore, the goal of this paper is to present accurate small sample inference methods for confidence interval estimation for the common gamma mean derived from several independent samples.
The rest of this paper is organized as follows. We will first present preliminaries including notations and existing methods for confidence interval estimation of single gamma mean. Then we will propose several methods for constructing confidence intervals for common gamma mean. Simulation results are presented to evaluate the performance of the proposed methods and examples are analyzed using the proposed methods. Finally, summary and discussion are given.
Preliminaries
The setting
Consider K independent gamma populations. Let be a random sample from the ith gamma population as Yij ∼ gamma(αi, βi) where αi is shape parameter and βi is rate parameter; i.e. the corresponding probability density function for Yij is
for yij > 0, αi, βi > 0. Let μi denote the population mean for ith sample. Then μi = αi/βi for i = 1, 2, …, K. We assume that μ1 = μ2 = … = μK and let μ denote the common mean. The goal of this paper is to present procedures for confidence interval estimation of μ at small to medium sample sizes.
Let and stand for the maximum likelihood estimates for αi and βi, respectively. The maximum likelihood estimate of μi is where the large sample variance for is [5]
| (1) |
and its estimate is
| (2) |
The common gamma mean can be estimated as a pooled estimate of sample means defined as
| (3) |
Using standard large sample theory, we have
asymptotically. Hence, a simple large sample solution for confidence interval estimation for common μ is
| (4) |
Of course, we also can obtain a large sample confidence interval using standard maximum likelihood theory. However, these large sample solutions do not have good performance at small sample sizes. Hence in this paper, we will present some procedures with satisfactory performance.
Existing methods for confidence interval estimation for single gamma mean
In the following, we will review several existing methods for confidence interval estimation for single gamma mean. These methods are known to have reasonable performance at small to medium sample sizes, and will be used in the following to present our new procedures for confidence interval estimation for common gamma mean.
Let Y1, Y2, …, Yn be a random sample from a gamma population gamma(α, β). The population mean μ = α/β. Let and denote the arithmetic mean and geometric mean, respectively. The maximum likelihood estimate of μ is where and are the maximum likelihood estimates for α and β, respectively.
Methods based on generalized inference
The generalized variables and generalized pivots were introduced by Tsui and Weerahandi [13] and Weerahandi [14]. More details can be found in the book by Weerahandi [15]. The concepts of generalized pivotal quantity and generalized confidence interval have been successfully applied to a variety of practical problems where standard exact solutions do not exist and it has been shown that generalized inference method generally have good performance, even at small sample sizes; see e.g. [16–21]. Recently, Hannig et al. [22] demonstrated generalized confidence intervals coincide with fiducial confidence intervals. In the following, we review three existing methods for constructing generalized pivotal quantity for single gamma mean.
Krishnamoorthy and Wang’s method: [7, 23] This method is based on the fact that (j = 1, 2, …, n) follows N(μ, σ2) approximately for gamma distribution. Let and be the observed sample mean and sample variance based on the transformed data . The generalized pivotal quantities for μ and σ2 can be obtained as [24]:
where Z ∼ N(0, 1), , and Z and U are independent. Furthermore, the generalized pivotal quantities for for α and β can be written as:
| (5) |
Chen and Ye’s method: [8, 25] Note that approximately, where ν = 2E2(V1)/var(V1), c = E(V1)/ν, E(V1) = 2nα(ψ(nα) − ψ(α) − log(n)) and var(V1) = 4n2 α2(ψ′(α)/n − ψ′(α)) with ψ and ψ′ being the digamma and trigamma functions respectively. Then and can be obtained by substituting α with its point estimate . An approximate generalized pivotal quantity (GPQ) for α is:
where , and are observed values of and . Furthermore, as , a GPQ for β can be constructed as:
| (6) |
where .
Wang and Wu’s method [9]: This method is based on Cornish-Fisher approximation. Let and F(.) be the c.d.f. of T. Note that U = F(T)∼U(0, 1). Using the Cornish-Fisher expansion, the Uth percentile of T can be approximated by g1(α) + [g2(α)]1/2 Q(α, U), where gi(α) is the ith cumulant of T and Q(α, U) is a function of gi(α)’s. Detailed formula can be found in [9]. Let t denote the observed value of T. Solving t = g1(α) + [g2(α)]1/2Q(α, U) for α, we obtain the approximate Rα. The GPQ for β can be obtained similarly as in (6):
| (7) |
where . This method improves Chen and Ye’s method and can work well even when the shape parameter α is small.
The three aforementioned methods for generating Rα and Rβ lead to three generalized pivots of a single gamma mean:
| (8) |
Via simulation, we can obtain an array of Rμ’s and the estimated confidence interval for μ is (Rμ(α/2), Rμ(1 − α/2)) where Rμ(α) is the 100αth percentile of Rμ’s.
A parametric bootstrap method [6]
Krishnamoorthy and León-Novelo [6] presented a method based on parametric bootstrapping for confidence interval estimation using the following pivotal quantity:
| (9) |
where and are based on a bootstrap sample from distribution. A two-sided 100(1 − p)% confidence interval (l, u) for μ is:
| (10) |
where Qp as the 100pth percentile of Q defined in (9).
The proposed methods for confidence interval estimation of common gamma mean
The methods based on generalized inference
For the ith (i = 1, 2, …, K) sample, we can obtain the generalized pivotal quantities using one of the three methods reviewed above (i.e. Krishnamoorthy and Wang’s method [7, 23] Chen and Ye’s method [8, 25], and Wang and Wu’s method [9]). Replacing μi and αi with and in (1), the generalized pivotal quantity for can be written as
| (11) |
The generalized pivotal quantity we propose for the common gamma mean μ is a weighted average of the generalized pivot ’s based on K individual samples, i.e.
| (12) |
where .
It is easy to see that Rμ satisfies the two conditions to be an approximate bona fide generalized pivotal quantity: 1) the distributions of Rμ is independent of any unknown parameters; and 2) the observed value of Rμ equals to the common gamma μ approximately. This way of constructing generalized pivots for common mean has been widely used in literature. For example, Krishnamoorthy and Lu [17] studied inferences on the common mean of several normal populations based on the generalized variable method; and Tian and Wu [26] studied common mean of several log-normal populations.
Computing algorithms
Consider a given data set Yij’s (i = 1, 2, …, K, j = 1, 2, …, ni) where the ith sample is from gamma(αi, βi). We assume μi = μ for all i = 1, 2, …, K. The generalize confidence intervals for the common mean μ can be computed by the following steps:
-
1
Using one of the three methods presented above, generate and , then calculate generalized pivot for μi following (12) for i = 1, 2, …, K.
-
2
Repeat steps 1, generate and and calculate . Using and , calculate following (11) for i = 1, 2, …, K.
-
3
Using obtained in step 1 and in step 2 for i = 1, 2, …, K, calculate the generalized pivot of the common mean Rμ from (12).
-
4
Repeat Steps 1-3 a total B (B = 2000) times and obtain an array of Rμ’s.
-
5
Rank this array of Rμ’s from small to large.
The 100αth percentile of Rμ’s, Rμ(α), is an estimate of the lower bound of the one-sided 100(1 − α)% confidence interval and (Rμ(α/2), Rθ(1 − α/2)) is a two-sided 100(1 − α)% confidence interval.
Remark 2.1: In computing algorithm, we used different sets of random variables for and . Our simulation shows that the generalized pivotal quantity based on the same set of random variables for and produces confidence intervals which are too liberal. Similar conclusions have been stated in [17, 26].
We refer these three methods based on the generalized pivots of common gamma mean as GVK, GVC, GVW, corresponding to the methods used for confidence interval estimation of a single gamma mean, i.e. Krishnamoorthy and Wang’s method [7, 23] Chen and Ye’s method [8, 25], and Wang and Wu’s method [9].
The MOVER-type methods
The method of variance estimates recovery (MOVER) is a useful technique for obtaining a closed-form approximate confidence interval for a linear combination of parameters based on the confidence intervals of the individual parameters [27, 28]. In this section, using the methods for estimating confidence intervals for a single gamma mean reviewed above, the MOVER method is applied for confidence interval estimation of the common gamma mean.
Let li and ui be the lower and upper limits of an approximate two-sided 100(1 − p)% confidence interval (li, ui) for the gamma mean based only on ith sample. A MOVER 100(1 − p)% confidence interval (L, U) of the common gamma mean is given by [27, 28]:
| (13) |
where , is defined in (2), and and are the maximum likelihood estimates for αi and μi, respectively.
For calculating confidence intervals (lk, uk) for the single gamma mean μi (i = 1, …, K), we will use the three generalized inference methods (i.e. Krishnamoorthy and Wang’s method [7, 23], Chen and Ye’s method [8, 25], and Wang and Wu’s method [9]) as well as the parametric bootstrap method by Krishnamoorthy and León-Novelo [6] reviewed above. Each method provides an approximate confidence interval (li, ui) for the ith single gamma mean μi (i = 1, 2, …K).
Substituting (lk, uk) in (13), we obtain confidence interval estimation of common mean μ. We refer these MOVER-type methods as MOVERK, MOVERC, MOVERW, MOVERboot corresponding to the methods used for single gamma mean, i.e. Krishnamoorthy and Wang’s method [7, 23] Chen and Ye’s method [8, 25], Wang and Wu’s method [9], and the parametric bootstrap method by Krishnamoorthy and León-Novelo’s method [6], respectively.
Simulation studies
In previous section, we presented several methods for confidence interval estimation of common gamma mean: three methods based on the generalized pivots (i.e. GVK, GVC, GVW); and four MOVER-type methods (i.e. MOVERK, MOVERC, MOVERW, MOVERboot).
Simulation studies are carried out to evaluate the performances of proposed methods in terms of coverage probabilities and average lengths of proposed confidence intervals. The number of samples K is set as 2 and 5, and a variety of sample sizes from small (5) to large (50) including balanced and unbalanced settings are used. The parameter settings are as follows: 1) common mean μ is set as 1 and 5; 2) shape parameter for each sample varies from 0.5 or 1 to 5 or 10, and the differences among K shape parameters varies from small to large. For each parameter setting, 2,000 random samples are generated. For the confidence interval based on generalized pivots (i.e. GVK, GVC, GVW), MOVERK, MOVERC, MOVERW), 2000 values of generalized pivots are obtained for each random sample. For the confidence interval based on parametric bootstrapping (MOVERboot), 2000 bootstrap samples are generated for each random sample. The performances of each method is assessed by coverage probability and average lengths of proposed confidence intervals. The simulation results are presented in Tables 1 and 2.
Table 1. Coverage probabilities (CP) and length of confidence interval (CI) of proposed 95% confidence intervals for the common gamma mean (2000 simulations) with two independent samples (K = 2).
| (α1, α2) | Sizes* | GVK | GVC | GVW | MOVERK | MOVERC | MOVERW | MOVERboot | |||||||
|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
| CP | CI | CP | CI | CP | CI | CP | CI | CP | CI | CP | CI | CP | CI | ||
| μ = 1 | |||||||||||||||
| (0.5,1) | I | 0.947 | 3.798 | 0.977 | 31.948 | 0.962 | 9.138 | 0.910 | 2.927 | 0.950 | 28.028 | 0.927 | 8.921 | 0.903 | 2.670 |
| II | 0.952 | 2.131 | 0.976 | 10.748 | 0.966 | 4.693 | 0.917 | 2.411 | 0.952 | 35.248 | 0.941 | 9.745 | 0.917 | 2.443 | |
| III | 0.955 | 1.458 | 0.969 | 1.896 | 0.964 | 1.722 | 0.916 | 1.260 | 0.940 | 1.628 | 0.936 | 1.496 | 0.927 | 1.337 | |
| IV | 0.947 | 0.827 | 0.961 | 0.933 | 0.959 | 0.909 | 0.921 | 0.756 | 0.941 | 0.847 | 0.936 | 0.828 | 0.935 | 0.813 | |
| V | 0.941 | 0.465 | 0.954 | 0.505 | 0.951 | 0.499 | 0.922 | 0.446 | 0.942 | 0.482 | 0.939 | 0.479 | 0.943 | 0.477 | |
| (1,2) | I | 0.965 | 2.274 | 0.974 | 4.504 | 0.966 | 2.656 | 0.927 | 1.804 | 0.942 | 3.353 | 0.930 | 2.126 | 0.917 | 1.441 |
| II | 0.957 | 1.319 | 0.969 | 2.027 | 0.960 | 1.483 | 0.931 | 1.464 | 0.948 | 2.957 | 0.936 | 1.810 | 0.922 | 1.202 | |
| III | 0.958 | 0.971 | 0.966 | 1.050 | 0.960 | 0.992 | 0.926 | 0.860 | 0.933 | 0.922 | 0.931 | 0.879 | 0.924 | 0.839 | |
| IV | 0.954 | 0.584 | 0.960 | 0.605 | 0.959 | 0.593 | 0.934 | 0.545 | 0.945 | 0.562 | 0.941 | 0.554 | 0.941 | 0.549 | |
| V | 0.945 | 0.333 | 0.948 | 0.341 | 0.948 | 0.338 | 0.933 | 0.323 | 0.940 | 0.330 | 0.939 | 0.329 | 0.938 | 0.328 | |
| (1,10) | I | 0.959 | 1.035 | 0.964 | 1.532 | 0.960 | 1.108 | 0.933 | 0.825 | 0.946 | 1.326 | 0.932 | 0.927 | 0.911 | 0.725 |
| II | 0.967 | 0.579 | 0.971 | 0.798 | 0.969 | 0.629 | 0.948 | 0.643 | 0.954 | 1.187 | 0.946 | 0.771 | 0.934 | 0.551 | |
| III | 0.957 | 0.478 | 0.962 | 0.494 | 0.961 | 0.481 | 0.941 | 0.434 | 0.945 | 0.445 | 0.941 | 0.436 | 0.940 | 0.427 | |
| IV | 0.956 | 0.293 | 0.959 | 0.296 | 0.959 | 0.294 | 0.947 | 0.281 | 0.946 | 0.283 | 0.947 | 0.282 | 0.947 | 0.281 | |
| V | 0.948 | 0.172 | 0.951 | 0.172 | 0.950 | 0.172 | 0.946 | 0.169 | 0.947 | 0.170 | 0.946 | 0.170 | 0.946 | 0.170 | |
| (2,10) | I | 0.960 | 0.891 | 0.963 | 1.023 | 0.953 | 0.862 | 0.931 | 0.727 | 0.933 | 0.812 | 0.927 | 0.709 | 0.917 | 0.647 |
| II | 0.954 | 0.526 | 0.957 | 0.576 | 0.953 | 0.525 | 0.933 | 0.562 | 0.940 | 0.653 | 0.934 | 0.560 | 0.921 | 0.491 | |
| III | 0.964 | 0.446 | 0.964 | 0.453 | 0.961 | 0.444 | 0.943 | 0.408 | 0.939 | 0.411 | 0.943 | 0.405 | 0.935 | 0.400 | |
| IV | 0.949 | 0.279 | 0.949 | 0.280 | 0.949 | 0.278 | 0.940 | 0.267 | 0.938 | 0.268 | 0.939 | 0.267 | 0.935 | 0.266 | |
| V | 0.952 | 0.166 | 0.953 | 0.167 | 0.953 | 0.166 | 0.950 | 0.164 | 0.947 | 0.164 | 0.950 | 0.164 | 0.949 | 0.164 | |
| (5,10) | I | 0.964 | 0.732 | 0.969 | 0.762 | 0.961 | 0.690 | 0.932 | 0.612 | 0.931 | 0.626 | 0.925 | 0.586 | 0.920 | 0.561 |
| II | 0.960 | 0.478 | 0.963 | 0.489 | 0.960 | 0.467 | 0.944 | 0.497 | 0.946 | 0.510 | 0.936 | 0.480 | 0.935 | 0.456 | |
| III | 0.956 | 0.390 | 0.956 | 0.392 | 0.957 | 0.387 | 0.934 | 0.358 | 0.936 | 0.358 | 0.934 | 0.355 | 0.936 | 0.352 | |
| IV | 0.945 | 0.246 | 0.949 | 0.246 | 0.945 | 0.245 | 0.929 | 0.235 | 0.931 | 0.235 | 0.927 | 0.235 | 0.932 | 0.234 | |
| V | 0.957 | 0.148 | 0.955 | 0.148 | 0.957 | 0.148 | 0.949 | 0.145 | 0.949 | 0.145 | 0.949 | 0.145 | 0.948 | 0.145 | |
| μ = 5 | |||||||||||||||
| (0.5,1) | I | 0.956 | 18.934 | 0.977 | 152.736 | 0.965 | 46.391 | 0.923 | 14.473 | 0.953 | 163.612 | 0.936 | 46.134 | 0.907 | 13.224 |
| II | 0.958 | 10.803 | 0.977 | 49.275 | 0.969 | 22.734 | 0.924 | 12.269 | 0.952 | 184.086 | 0.936 | 46.080 | 0.924 | 12.116 | |
| III | 0.956 | 7.174 | 0.974 | 9.363 | 0.966 | 8.501 | 0.917 | 6.177 | 0.941 | 8.038 | 0.931 | 7.393 | 0.927 | 6.588 | |
| IV | 0.932 | 4.122 | 0.950 | 4.651 | 0.948 | 4.523 | 0.906 | 3.782 | 0.928 | 4.226 | 0.925 | 4.133 | 0.923 | 4.059 | |
| V | 0.944 | 2.304 | 0.963 | 2.498 | 0.961 | 2.473 | 0.928 | 2.210 | 0.950 | 2.385 | 0.948 | 2.369 | 0.946 | 2.363 | |
| (1,2) | I | 0.957 | 11.242 | 0.975 | 21.977 | 0.961 | 13.098 | 0.921 | 8.943 | 0.942 | 16.556 | 0.925 | 10.592 | 0.912 | 7.177 |
| II | 0.961 | 6.637 | 0.976 | 10.351 | 0.966 | 7.517 | 0.938 | 7.429 | 0.954 | 15.540 | 0.944 | 9.356 | 0.924 | 6.099 | |
| III | 0.965 | 4.859 | 0.975 | 5.258 | 0.967 | 4.971 | 0.934 | 4.306 | 0.943 | 4.618 | 0.936 | 4.407 | 0.930 | 4.198 | |
| IV | 0.946 | 2.896 | 0.955 | 2.999 | 0.949 | 2.940 | 0.928 | 2.702 | 0.934 | 2.787 | 0.936 | 2.747 | 0.934 | 2.724 | |
| V | 0.952 | 1.673 | 0.953 | 1.710 | 0.956 | 1.699 | 0.945 | 1.624 | 0.950 | 1.660 | 0.950 | 1.651 | 0.948 | 1.650 | |
| (1,10) | I | 0.963 | 5.098 | 0.969 | 7.328 | 0.967 | 5.373 | 0.935 | 4.086 | 0.947 | 6.156 | 0.933 | 4.451 | 0.919 | 3.588 |
| II | 0.969 | 2.857 | 0.976 | 3.868 | 0.969 | 3.095 | 0.955 | 3.201 | 0.963 | 5.952 | 0.952 | 3.868 | 0.939 | 2.746 | |
| III | 0.958 | 2.398 | 0.960 | 2.482 | 0.956 | 2.411 | 0.938 | 2.170 | 0.940 | 2.229 | 0.940 | 2.183 | 0.933 | 2.138 | |
| IV | 0.952 | 1.455 | 0.954 | 1.470 | 0.951 | 1.458 | 0.940 | 1.393 | 0.945 | 1.405 | 0.948 | 1.397 | 0.946 | 1.393 | |
| V | 0.947 | 0.866 | 0.949 | 0.870 | 0.948 | 0.869 | 0.943 | 0.854 | 0.946 | 0.858 | 0.943 | 0.857 | 0.943 | 0.857 | |
| (2,10) | I | 0.960 | 4.540 | 0.965 | 5.190 | 0.956 | 4.367 | 0.926 | 3.701 | 0.931 | 4.105 | 0.923 | 3.602 | 0.917 | 3.287 |
| II | 0.954 | 2.639 | 0.957 | 2.890 | 0.953 | 2.635 | 0.935 | 2.822 | 0.937 | 3.278 | 0.934 | 2.815 | 0.925 | 2.471 | |
| III | 0.961 | 2.215 | 0.963 | 2.246 | 0.959 | 2.199 | 0.945 | 2.025 | 0.948 | 2.043 | 0.946 | 2.012 | 0.943 | 1.986 | |
| IV | 0.952 | 1.396 | 0.955 | 1.403 | 0.954 | 1.394 | 0.946 | 1.339 | 0.944 | 1.343 | 0.946 | 1.338 | 0.946 | 1.334 | |
| V | 0.946 | 0.829 | 0.949 | 0.831 | 0.949 | 0.829 | 0.945 | 0.815 | 0.945 | 0.817 | 0.945 | 0.817 | 0.946 | 0.816 | |
| (5,10) | I | 0.951 | 3.645 | 0.960 | 3.794 | 0.953 | 3.439 | 0.911 | 3.054 | 0.919 | 3.123 | 0.909 | 2.923 | 0.910 | 2.798 |
| II | 0.962 | 2.383 | 0.966 | 2.432 | 0.961 | 2.319 | 0.942 | 2.473 | 0.944 | 2.536 | 0.934 | 2.385 | 0.936 | 2.267 | |
| III | 0.963 | 1.962 | 0.963 | 1.971 | 0.960 | 1.944 | 0.943 | 1.801 | 0.943 | 1.804 | 0.942 | 1.787 | 0.942 | 1.772 | |
| IV | 0.951 | 1.245 | 0.952 | 1.247 | 0.953 | 1.240 | 0.944 | 1.190 | 0.943 | 1.190 | 0.944 | 1.187 | 0.943 | 1.185 | |
| V | 0.942 | 0.737 | 0.942 | 0.738 | 0.945 | 0.736 | 0.942 | 0.723 | 0.941 | 0.724 | 0.941 | 0.723 | 0.941 | 0.723 | |
* I:(5,5), II:(5,10), III:(10,10), IV:(20,20), V: (50,50)
Table 2. Coverage probabilities (CP) and length of confidence interval (CI) of proposed 95% confidence intervals for the common gamma mean (2000 simulations) with two independent samples (K = 5).
| (α1, α2) | Sizes* | GVK | GVC | GVW | MOVERK | MOVERC | MOVERW | MOVERboot | |||||||
|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
| CP | CI | CP | CI | CP | CI | CP | CI | CP | CI | CP | CI | CP | CI | ||
| μ = 1 | |||||||||||||||
| (0.5,0.5,0.75,0.75,1) | VI | 0.962 | 2.618 | 0.995 | 89.847 | 0.979 | 8.961 | 0.879 | 1.590 | 0.959 | 19.057 | 0.926 | 5.422 | 0.830 | 1.471 |
| VII | 0.955 | 0.978 | 0.980 | 1.316 | 0.966 | 1.165 | 0.857 | 0.741 | 0.922 | 0.959 | 0.901 | 0.877 | 0.869 | 0.785 | |
| VIII | 0.931 | 0.561 | 0.961 | 0.639 | 0.956 | 0.620 | 0.874 | 0.475 | 0.913 | 0.533 | 0.908 | 0.520 | 0.898 | 0.510 | |
| IX | 0.959 | 0.687 | 0.984 | 2.241 | 0.975 | 1.184 | 0.927 | 1.196 | 0.966 | 15.958 | 0.949 | 4.277 | 0.913 | 1.213 | |
| X | 0.923 | 0.309 | 0.955 | 0.338 | 0.951 | 0.335 | 0.901 | 0.287 | 0.930 | 0.311 | 0.927 | 0.309 | 0.927 | 0.308 | |
| (0.5,1,2,5,10) | VI | 0.970 | 0.903 | 0.987 | 3.417 | 0.976 | 1.300 | 0.901 | 0.609 | 0.944 | 2.858 | 0.922 | 1.146 | 0.863 | 0.551 |
| VII | 0.961 | 0.396 | 0.969 | 0.425 | 0.964 | 0.407 | 0.906 | 0.322 | 0.924 | 0.346 | 0.916 | 0.335 | 0.899 | 0.322 | |
| VIII | 0.950 | 0.235 | 0.952 | 0.240 | 0.949 | 0.236 | 0.922 | 0.213 | 0.925 | 0.217 | 0.926 | 0.215 | 0.919 | 0.214 | |
| IX | 0.966 | 0.210 | 0.978 | 0.427 | 0.970 | 0.276 | 0.946 | 0.420 | 0.969 | 4.520 | 0.958 | 1.434 | 0.919 | 0.412 | |
| X | 0.956 | 0.135 | 0.960 | 0.137 | 0.957 | 0.136 | 0.947 | 0.130 | 0.950 | 0.132 | 0.948 | 0.132 | 0.947 | 0.131 | |
| (0.5,2,2,5,5) | VI | 0.966 | 0.977 | 0.983 | 3.781 | 0.972 | 1.435 | 0.895 | 0.670 | 0.936 | 5.867 | 0.911 | 1.594 | 0.864 | 0.609 |
| VII | 0.962 | 0.443 | 0.973 | 0.474 | 0.965 | 0.453 | 0.905 | 0.363 | 0.923 | 0.389 | 0.916 | 0.375 | 0.900 | 0.361 | |
| VIII | 0.945 | 0.268 | 0.951 | 0.274 | 0.950 | 0.270 | 0.916 | 0.241 | 0.923 | 0.246 | 0.922 | 0.244 | 0.917 | 0.243 | |
| IX | 0.957 | 0.276 | 0.976 | 0.602 | 0.965 | 0.368 | 0.944 | 0.504 | 0.966 | 5.257 | 0.954 | 1.571 | 0.922 | 0.495 | |
| X | 0.955 | 0.153 | 0.959 | 0.155 | 0.958 | 0.154 | 0.943 | 0.147 | 0.943 | 0.149 | 0.942 | 0.148 | 0.944 | 0.148 | |
| (1,2,2,5,5) | VI | 0.971 | 0.916 | 0.983 | 1.551 | 0.972 | 0.954 | 0.904 | 0.629 | 0.924 | 0.887 | 0.901 | 0.654 | 0.864 | 0.537 |
| VII | 0.960 | 0.426 | 0.966 | 0.442 | 0.958 | 0.425 | 0.915 | 0.354 | 0.918 | 0.363 | 0.911 | 0.354 | 0.901 | 0.346 | |
| VIII | 0.955 | 0.260 | 0.962 | 0.264 | 0.958 | 0.260 | 0.932 | 0.236 | 0.933 | 0.239 | 0.929 | 0.237 | 0.929 | 0.236 | |
| IX | 0.964 | 0.252 | 0.972 | 0.299 | 0.965 | 0.263 | 0.945 | 0.444 | 0.954 | 0.796 | 0.949 | 0.522 | 0.920 | 0.377 | |
| X | 0.945 | 0.151 | 0.948 | 0.152 | 0.945 | 0.151 | 0.939 | 0.145 | 0.941 | 0.146 | 0.938 | 0.146 | 0.940 | 0.146 | |
| (2,2,5,5,10) | VI | 0.968 | 0.654 | 0.979 | 0.820 | 0.970 | 0.633 | 0.898 | 0.465 | 0.908 | 0.513 | 0.892 | 0.452 | 0.864 | 0.413 |
| VII | 0.961 | 0.325 | 0.961 | 0.330 | 0.959 | 0.322 | 0.914 | 0.276 | 0.916 | 0.278 | 0.910 | 0.274 | 0.902 | 0.271 | |
| VIII | 0.966 | 0.202 | 0.967 | 0.204 | 0.964 | 0.202 | 0.941 | 0.186 | 0.940 | 0.187 | 0.941 | 0.186 | 0.936 | 0.186 | |
| IX | 0.961 | 0.180 | 0.967 | 0.188 | 0.959 | 0.180 | 0.936 | 0.302 | 0.948 | 0.345 | 0.932 | 0.300 | 0.915 | 0.267 | |
| X | 0.964 | 0.118 | 0.958 | 0.119 | 0.961 | 0.118 | 0.954 | 0.114 | 0.953 | 0.115 | 0.953 | 0.114 | 0.953 | 0.114 | |
| μ = 5 | |||||||||||||||
| (0.5,0.5,0.75,0.75,1) | VI | 0.968 | 12.835 | 0.994 | 396.747 | 0.982 | 43.412 | 0.882 | 7.805 | 0.964 | 126.406 | 0.924 | 32.435 | 0.835 | 7.311 |
| VII | 0.953 | 4.907 | 0.979 | 6.617 | 0.973 | 5.857 | 0.860 | 3.728 | 0.924 | 4.794 | 0.903 | 4.393 | 0.867 | 3.940 | |
| VIII | 0.947 | 2.813 | 0.975 | 3.203 | 0.970 | 3.107 | 0.881 | 2.384 | 0.920 | 2.676 | 0.910 | 2.615 | 0.905 | 2.563 | |
| IX | 0.957 | 3.430 | 0.985 | 10.460 | 0.976 | 5.677 | 0.918 | 5.834 | 0.962 | 63.516 | 0.947 | 20.451 | 0.906 | 5.913 | |
| X | 0.928 | 1.552 | 0.961 | 1.695 | 0.960 | 1.679 | 0.899 | 1.437 | 0.930 | 1.557 | 0.931 | 1.546 | 0.928 | 1.542 | |
| (0.5,1,2,5,10) | VI | 0.972 | 4.566 | 0.987 | 19.559 | 0.979 | 7.006 | 0.897 | 3.095 | 0.946 | 18.131 | 0.917 | 6.738 | 0.858 | 2.842 |
| VII | 0.965 | 1.971 | 0.973 | 2.117 | 0.967 | 2.025 | 0.915 | 1.611 | 0.934 | 1.730 | 0.926 | 1.670 | 0.907 | 1.609 | |
| VIII | 0.949 | 1.177 | 0.954 | 1.202 | 0.953 | 1.188 | 0.923 | 1.067 | 0.927 | 1.089 | 0.926 | 1.080 | 0.928 | 1.074 | |
| IX | 0.957 | 1.047 | 0.976 | 2.291 | 0.968 | 1.384 | 0.939 | 2.091 | 0.959 | 24.026 | 0.949 | 7.508 | 0.919 | 2.071 | |
| X | 0.950 | 0.675 | 0.953 | 0.681 | 0.950 | 0.679 | 0.939 | 0.650 | 0.945 | 0.657 | 0.944 | 0.656 | 0.944 | 0.656 | |
| (0.5,2,2,5,5) | VI | 0.966 | 4.907 | 0.984 | 16.560 | 0.974 | 6.850 | 0.894 | 3.356 | 0.936 | 19.666 | 0.912 | 6.848 | 0.860 | 3.047 |
| VII | 0.960 | 2.229 | 0.973 | 2.381 | 0.968 | 2.276 | 0.897 | 1.822 | 0.918 | 1.953 | 0.906 | 1.882 | 0.892 | 1.812 | |
| VIII | 0.948 | 1.337 | 0.952 | 1.364 | 0.950 | 1.345 | 0.911 | 1.200 | 0.919 | 1.225 | 0.912 | 1.213 | 0.911 | 1.208 | |
| IX | 0.959 | 1.391 | 0.973 | 3.026 | 0.968 | 1.882 | 0.934 | 2.512 | 0.959 | 25.382 | 0.947 | 8.083 | 0.913 | 2.437 | |
| X | 0.952 | 0.766 | 0.952 | 0.775 | 0.949 | 0.772 | 0.939 | 0.735 | 0.943 | 0.744 | 0.942 | 0.742 | 0.943 | 0.741 | |
| (1,2,2,5,5) | VI | 0.966 | 4.606 | 0.979 | 7.967 | 0.966 | 4.825 | 0.901 | 3.162 | 0.923 | 4.510 | 0.897 | 3.319 | 0.858 | 2.697 |
| VII | 0.968 | 2.151 | 0.971 | 2.234 | 0.965 | 2.148 | 0.916 | 1.791 | 0.920 | 1.837 | 0.914 | 1.788 | 0.901 | 1.746 | |
| VIII | 0.969 | 1.304 | 0.972 | 1.322 | 0.967 | 1.305 | 0.941 | 1.186 | 0.941 | 1.197 | 0.940 | 1.187 | 0.935 | 1.183 | |
| IX | 0.956 | 1.267 | 0.972 | 1.499 | 0.961 | 1.321 | 0.933 | 2.208 | 0.948 | 4.063 | 0.936 | 2.631 | 0.913 | 1.882 | |
| X | 0.958 | 0.751 | 0.955 | 0.757 | 0.952 | 0.753 | 0.946 | 0.722 | 0.947 | 0.727 | 0.945 | 0.725 | 0.946 | 0.725 | |
| (2,2,5,5,10) | VI | 0.965 | 3.276 | 0.970 | 4.063 | 0.960 | 3.143 | 0.901 | 2.312 | 0.912 | 2.527 | 0.891 | 2.243 | 0.870 | 2.063 |
| VII | 0.964 | 1.626 | 0.964 | 1.648 | 0.960 | 1.610 | 0.923 | 1.379 | 0.922 | 1.389 | 0.919 | 1.368 | 0.916 | 1.351 | |
| VIII | 0.949 | 1.007 | 0.952 | 1.014 | 0.947 | 1.004 | 0.928 | 0.927 | 0.927 | 0.930 | 0.927 | 0.925 | 0.925 | 0.923 | |
| IX | 0.958 | 0.896 | 0.964 | 0.937 | 0.956 | 0.899 | 0.939 | 1.514 | 0.947 | 1.740 | 0.938 | 1.506 | 0.922 | 1.337 | |
| X | 0.951 | 0.591 | 0.953 | 0.593 | 0.950 | 0.591 | 0.941 | 0.572 | 0.942 | 0.573 | 0.942 | 0.572 | 0.941 | 0.573 | |
* Sizes are VI:(5,5,5,5,5), VII:(10,10,10,10,10), VIII:(20,20,20,20,20), IX: (5,10,10,20,50), X: (50,50,50,50,50)
Table 1 presents simulated coverage probabilities (CP) and confidence interval lengths (CI) for K = 2. Overall speaking, three methods based on the generalized pivots (i.e. GVK, GVC, GVW) maintains satisfactory coverage probabilities for all settings except that they might be slightly conservative at small sizes and GVK was slightly liberal when (α1, α2) = (1, 2) at sample sizes (50, 50) and (α1, α2) = (0.5, 1) at sample sizes (20, 20). Among MOVER-type methods (i.e. MOVERK, MOVERC, MOVERW, MOVERboot), MOVERC performs the best while all of them are generally liberal when sample sizes are from (5, 5) to (20, 20). When sample sizes reach 50, all the proposed methods perform satisfactorily. The GVK method provides shortest confidence intervals among three generalized pivots based methods, followed by GVW. As sample sizes reach 20, all three methods (i.e. GVK, GVC, GVW) are generally comparable. MOVERK and MOVERboot provides shortest confidence intervals among MOVER-type methods. As sample sizes reach 20, all MOVER-type methods (i.e. MOVERK, MOVERC, MOVERW, MOVERboot) are comparable in terms of length. When sample sizes reach 50, all the proposed methods generate confidence intervals with comparable length.
Table 2 presents simulated coverage probabilities (CP) and confidence interval lengths (CI) for K = 5. The three generalized pivots based methods methods generally maintains satisfactory coverage probabilities for all settings except that they tend to be slightly conservative at small sizes and GVK is liberal at (α1, …, α5) = (0.5, 0.5, 0.75, 0.75, 1) with sizes (50, 50, 50, 50, 50). Among MOVER-type methods (i.e. MOVERK, MOVERC, MOVERW, MOVERboot), MOVERC performs the best while they are generally liberal when sample sizes are from (5, 5, 5, 5, 5) to (20, 20, 20, 20). When sample sizes reach 50, all methods perform satisfactorily. The GVK method provides shortest confidence intervals among three generalized pivots based methods, followed by GVW. As sample sizes reach 20, all three methods (i.e. GVK, GVC, GVW) are comparable. MOVERK provides shortest confidence intervals among three MOVER-type methods, followed by MOVERb oot. As sample sizes reach 20, all four methods (i.e. MOVERK, MOVERC, MOVERW, MOVERboot) are comparable. When sample sizes reach 50, all methods are generally comparable in terms of length.
In summary, generally we recommend GVK, GVC, GVW methods over MOVER-type methods due to the fact that they can generate confidence intervals with satisfactory coverage probabilities even at smaller sizes. The MOVER-type methods are not recommended unless sample sizes are greater than or equal to 50. The large sample approach in (4) can severely underestimate the coverage probabilities, hence its results are not presented.
Data examples
In this section, we illustrate the proposed methods using two examples. Both datasets was analyzed in [11] for testing equality of gamma means, and it was concluded that the null hypothesis (equality of gamma means) can not be rejected. Therefore, in this paper, we use these two datasets to illustrate our proposed methods for estimating confidence intervals of the common gamma mean.
Example 1. Wright [29] reported ground water yield from two types of wells in southwestern Virginia. Table 3 presents this dataset which includes ground water yield data from 12 wells from valley underlain by unfractured rocks, and 13 wells by fractured rocks. It has been argued that gamma distribution is appropriate to fit the data in each sample, and the test for equality of means [11] concluded that the means of water yields from two types of wells are the same. The estimated parameters are: α1 = 0.4342, , α2 = 1.1854, . The estimated 95% confidence intervals for the common gamma mean by all the proposed methods are presented in Table 4. Our simulation study demonstrate that MOVER-type methods could be liberal at sample sizes (10, 10). Give the sample sizes as 12 and 13 in this application, the confidence intervals by GVK, GVC, GVW methods are recommended, and among them the GVK method has the shortest length.
Table 3. Virginia ground water well yields data (in gal/min/ft) [29].
| Without fractures | with fractures |
|---|---|
| 0.001, 0.003, 0.007, 0.020 | 0.020, 0.031, 0.085, 0.013 |
| 0.030, 0.040, 0.041, 0.077 | 0.160, 0.160, 0.180, 0.300 |
| 0.100, 0.454, 0.490, 1.020 | 0.400, 0.440, 0.510, 0.720, 0.950 |
Table 4. Estimated confidence interval for Virginia ground water well yields data (in gal/min/ft).
| method | lower | upper | LCI |
|---|---|---|---|
| GV K | 0.140 | 0.491 | 0.351 |
| GV C | 0.159 | 0.576 | 0.417 |
| GV W | 0.153 | 0.574 | 0.421 |
| MOVER K | 0.169 | 0.459 | 0.289 |
| MOVER C | 0.178 | 0.548 | 0.370 |
| MOVER W | 0.175 | 0.530 | 0.355 |
| MOVER boot | 0.175 | 0.490 | 0.314 |
Example 2. Table 5 presents a dataset of chloride concentration in spring water samples from two types of rocks in Sierra Nevada, California and Nevada [30]. It has been argued that gamma distribution is appropriate to fit the data in each sample, and testing equality of means [11] concluded that the means of chloride concentration from two types of rocks are the same. The estimated parameters are: α1 = 0.7594, , α2 = 1.1359, . The estimated 95% confidence intervals for the common gamma mean by all the proposed methods are presented in Table 6. Given sample sizes 18 and 17 and parameter estimates, the confidence interval estimated by GVK is most recommenced in practice.
Table 5. Chloride concentration (in mg/litre) in water data. [30].
| Granodiorite | Quartz Monzonite |
|---|---|
| 6.0, 0.5, 0.4, 0.7, 0.8, 6.0, 5.0, 0.6, 1.2 | 1.0, 0.2, 1.2, 1.0, 0.3, 0.1, 0.1, 0.4, 3.2 |
| 1.0, 0.2, 1.2, 1.0, 0.3, 0.1, 0.1, 0.4, 3.2 | 0.3, 0.4, 1.8, 0.9, 0.1, 0.2, 0.3, 0.5 |
Table 6. Estimated confidence intervals and lengths for the common mean for Chloride concentration (in mg/litre) in water.
| method | lower | upper | length |
|---|---|---|---|
| GV K | 0.524 | 1.366 | 0.842 |
| GV C | 0.555 | 1.482 | 0.928 |
| GV W | 0.547 | 1.455 | 0.908 |
| MOVER K | 0.543 | 1.251 | 0.707 |
| MOVER C | 0.569 | 1.317 | 0.749 |
| MOVER W | 0.571 | 1.317 | 0.746 |
| MOVER boot | 0.567 | 1.310 | 0.743 |
Summary and discussion
Gamma distribution plays an important role in practice. When the result of testing equality of several gamma means is not significant, it is customary that we need to make inference about the common gamma mean. While the standard large sample methods exist, small sample inference for the common gamma mean has not been explored. In this article, we focus on accurate confidence interval estimation for the common gamma mean based on several independent gamma samples using the concepts of generalized pivots and the method of MOVER. Via a comprehensive simulation study, we discovered that the proposed methods based on generalized pivots can generally provide satisfactory confidence intervals with consistent performance despite parameter settings and sample sizes. The MOVER-type methods can be liberal for certain scenarios, especially when sample sizes are small.
The proposed methods are easy to implement. The R program is available at li.yan@roswellpark.org.
Due to the popularity of gamma distribution in applied fields, we expect the proposed methods have wide applicability in practice where right-skewed data are often observed.
Data Availability
All relevant data are within the paper.
Funding Statement
The author(s) received no specific funding for this work.
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