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Article

Bayesian and Non-Bayesian Estimation for a New Extension of Power Topp–Leone Distribution under Ranked Set Sampling with Applications

1
Department of Mathematics and Statistics, Faculty of Science, Imam Mohammad Ibn Saud Islamic University (IMSIU), Riyadh 11432, Saudi Arabia
2
Department of Mathematics, College of Science, Jouf University, P.O. Box 848, Sakaka 72351, Saudi Arabia
3
Department of Statistics and Operations Research, College of Science, King Saud University, P.O. Box 2455, Riyadh 11451, Saudi Arabia
4
Mathematics and Computer Science Department, Faculty of Science, Beni-Suef University, Beni-Suef 62521, Egypt
5
Faculty of Business Administration, Delta University for Science and Technology, Gamasa 11152, Egypt
*
Author to whom correspondence should be addressed.
Axioms 2023, 12(8), 722; https://doi.org/10.3390/axioms12080722
Submission received: 29 May 2023 / Revised: 18 July 2023 / Accepted: 19 July 2023 / Published: 25 July 2023
(This article belongs to the Special Issue Probability, Statistics and Estimation)

Abstract

:
In this article, we intend to introduce and study a new two-parameter distribution as a new extension of the power Topp–Leone (PTL) distribution called the Kavya–Manoharan PTL (KMPTL) distribution. Several mathematical and statistical features of the KMPTL distribution, such as the quantile function, moments, generating function, and incomplete moments, are calculated. Some measures of entropy are investigated. The cumulative residual Rényi entropy (CRRE) is calculated. To estimate the parameters of the KMPTL distribution, both maximum likelihood and Bayesian estimation methods are used under simple random sample (SRS) and ranked set sampling (RSS). The simulation study was performed to be able to verify the model parameters of the KMPTL distribution using SRS and RSS to demonstrate that RSS is more efficient than SRS. We demonstrated that the KMPTL distribution has more flexibility than the PTL distribution and the other nine competitive statistical distributions: PTL, unit-Gompertz, unit-Lindley, Topp–Leone, unit generalized log Burr XII, unit exponential Pareto, Kumaraswamy, beta, Marshall-Olkin Kumaraswamy distributions employing two real-world datasets.

1. Introduction

The Topp–Leone (TL) distribution, developed by [1], is one of the most helpful of the known distributions, with support across the unit interval. It has the following distribution function (CDF) and density function (PDF):
G ( t ; δ ) = t δ 2 t δ , 0 < t < 1 , δ > 0 ,
and
g ( t ; δ ) = 2 δ t δ 1 1 t 2 t δ 1 , 0 < t < 1 , δ > 0 ,
where δ is a shape parameter.
Generalizations of the TL distribution have been shown to be beneficial in a variety of disciplines. Many notable academics have made significant attempts to suggest new generalized and developed modifications of the TL model, for example, TL inverse Weibull distribution [2], Type I half-Logistic TL distribution [3], TL geometric distribution [4], truncated Cauchy power inverted TL distribution [5], TL Nadarajah-Haghighi distribution [6], power inverted TL distribution [7], TL linear exponential distribution [8], Kumaraswamy inverted TL distribution [9], new power TL family [10], alpha power inverted TL distribution [11], half-logistic inverted TL distribution [12], type II Power TL family [13], odd log-logistic TL family [14], TL odd Fréchet distribution [15], Burr III-TL family [16], inverse TL distribution [17], exponentiated generalized TL family [18], transmuted TL power function distribution [19], transmuted TL family [20], sine TL family [21], weighted TL family [22], TL inverse Lomax distribution [23], and new weighted TL family [24], among others.
Recently, Ref. [25] used this transformation, Z = T 1 / λ , to introduce the PTL distribution as a generalization of the TL distribution, and it has the following CDF, PDF, and quantile function (qf)
G ( z ; λ , δ ) = z λ δ 2 z λ δ , 0 < z < 1 , λ , δ > 0 ,
g ( z ; λ , δ ) = 2 λ δ z λ δ 1 1 z λ 2 z λ δ 1 , 0 < z < 1 , λ , δ > 0 ,
and
Q ( q ) = 1 1 q 1 δ 0.5 1 λ ,
where λ and δ are two shape parameters and q 0 , 1 .
In recent years, many authors used the power transformation technique to obtain statistical distributions that are more flexible due to the shape parameter. Several of the potential power distributions are as follows: the power Zeghdoudi distribution [26], power modified Kies distribution [27], power Darna distribution [28], power Burr X distribution [29], power transmuted inverse Rayleigh distribution [30], power Rama distribution [31], power binomial exponential distribution [32], power Aradhana distribution [33], power Lomax distribution [34], power half logistic distribution [35], power Shanker distribution [36], power Lindley distribution [37], and power Cauchy distribution [38], among others.
Adding parameters improves versatility, but they also increase the problem of the complexity estimation parameters. In recent times, Ref. [39] created the Kavya–Manoharan (KM) class in order to acquire new parsimonious distribution families, and it has the following CDF:
F ( z ; Ω ) = e e 1 1 e G z ; Ω , z R .
The corresponding PDF and qf of the KM family are
f ( z ; Ω ) = e e 1 g z ; Ω e G z ; Ω ,
and
Q ( q ) = G 1 ln 1 q 1 e 1 ,
where G ( z ; Ω ) and g ( z ; Ω ) are the CDF and the PDF of the parent distribution.
Ranked set sampling (RSS) is an efficient and successful alternative to simple random sampling (SRS). When sampling units are expensive and difficult to quantify, this method is typically used to generate samples that are more representative of the underlying population, as well as samples that are straightforward and affordable to arrange in line with the variable of interest. Plenty of studies on RSS technique changes have been undertaken. Additional details about the RSS system may be found in, for example, [40,41,42,43]. The study of RSS-based estimates for several parametric models has lately attracted a significant amount of interest. These studies repeatedly indicate that RSS outperforms SRS and other traditional sampling strategies. Here are several instances: Ref. [44] for the Lomax distribution, Ref. [45] for the exponentiated exponential distribution, Ref. [46] for the xgamma distribution, Refs. [47,48] for exponentiated Pareto distribution, Refs. [49,50] for the Kumaraswamy distribution, Ref. [51] for the exponential-Poisson distribution, Ref. [52] for the generalized inverse Lindley distribution, Ref. [53] for the Birnbaum–Saunders distribution, Ref. [54] for the generalized quasi-Lindley distribution, Ref. [55] for the Weibull distribution, and Ref. [56] for the Zubair Lomax distribution.
Although [25] introduced a new flexible two-shape parameter distribution called the PTL distribution, the limitation of this study is that the PTL distribution does not give more fitting for different types of data. Because of this, we aim in this paper to introduce a new extension of the PTL distribution by the same number of parameters, called the KMPTL distribution. The new suggested distribution gives a better fit than the PTL distribution and some well-known distribution, and we supported that in the application section. Here, we aim to profit from the combined KM-class of distributions and the PTL distribution by investigating a new two-parameter distribution named the KMPTL distribution. The major motivations behind the KMPTL distribution are as follows:
  • The KMPTL distribution is very simple and it has more flexibility than the PTL distribution, and both distributions have two parameters.
  • We demonstrate that the KMPTL distribution may provide desirable features in both practical and theoretical terms.
  • Numerous broad statistical and mathematical aspects of the PTL distribution were studied.
  • Four different measures of entropy are calculated.
  • The cumulative residual Rényi entropy (CRRE) is calculated.
  • Classical and Bayesian approaches of estimation were utilized to compute the estimate of parameters for the KMPTL distribution, under SRS and RSS.
  • For modeling, we used two genuine datasets from economics and physics; the KMPTL distribution provides a better fit than the PTL distribution and the other nine competitive statistical distributions, the PTL, unit-Gompertz (UG), unit-Lindley (UL), TL, unit generalized log Burr XII (UGLBXII), unit exponential Pareto distribution (UEPD), Kumaraswamy (Kw), beta, and Marshall-Olkin Kumaraswamy (MOK) distributions, and we suggested this in the application section.
The following is an outline of the contents of this article. In Section 2, the formulation of the KMPTL distribution is discussed. Numerous mathematical characteristics of the KMPTL distribution are proposed in Section 3. Two Sections, Section 4 and Section 5, are devoted to four different measures of entropy and the CRRE from the KMPTL distribution. Classical and Bayesian estimation of the two shape unknown parameters from the KMPTL distribution, utilizing a thorough simulation experiment, are discussed in Section 6 and Section 7, respectively. Section 8 examines two real datasets and provides a clear comparison of nine competitive distributions. Section 9 presents a conclusion to the topic.

2. The Kavya–Manoharan Power Topp–Leone Distribution

Here, in this section, we intend to create the KMPTL distribution. Substituting Equations (3) and (4) into Equations (6) and (7) to obtain the CDF and PDF of the KMPTL distribution as below:
F ( z ; λ , δ ) = e e 1 1 e z λ δ 2 z λ δ , 0 < z < 1 , λ , δ > 0 ,
and
f ( z ; λ , δ ) = 2 λ δ e e 1 z λ δ 1 1 z λ 2 z λ δ 1 e z λ δ 2 z λ δ .
In addition, the survival function and the hazard rate function (HRF) are provided via
S ( z ; λ , δ ) = 1 e e 1 1 e z λ δ 2 z λ δ ,
and
h ( z ; λ , δ ) = 2 λ δ e z λ δ 1 1 z λ 2 z λ δ 1 e z λ δ 2 z λ δ e 1 z λ δ 2 z λ δ 1 .
The reversed and cumulative HRFs are
τ ( z ; λ , δ ) = 2 λ δ z λ δ 1 1 z λ 2 z λ δ 1 e z λ δ 2 z λ δ 1 ,
and
H ( z ; λ , δ ) = ln 1 e e 1 1 e z λ δ 2 z λ δ .
Figure 1 and Figure 2 show some curves of the PDF and the HRF for the KMPTL distribution. We can note from Figure 1 that the curves of PDF for the KMPTL distribution can be unimodal, right-skewed, left-skewed, symmetric, heavy-tailed, and decreasing, but from Figure 2 we can note that the curves of HRF for the KMPTL distribution can be increasing, J-shaped, U-shaped and, bathtub.
The HRF is complex in definition, but an asymptotic study is possible. The limit gives important information on its behavior.
When z 0 , we have h ( z ; λ , δ ) 2 δ λ δ e 1 e z λ δ 1 . As a result, when λ δ < 1 , we have h ( z ; λ , δ ) + , when λ δ = 1 , we have a constant limit: h ( z ; λ , δ ) = 2 δ λ δ e 1 e , and when λ δ > 1 , we have h ( z ; λ , δ ) 0 .
On the other hand, when z 1 , there is no parameter nuance; we have h ( z ; λ , δ ) + . This asymptotic analysis is completed by a graphic analysis in Figure 2. In addition, Figure 3 shows a monotone plot of the HRF for the KMPTL distribution to confirm the HRF has more shapes under the different values of parameter.

3. Some Basic Statistical Properties

In this part, we will look at some basic structural aspects of the KMPTL distribution.

3.1. Quantile Function

The qf, defined as Q q ; λ , δ = F 1 q ; λ , δ , is computed by inverting Equation (9) as
Q q ; λ , δ = 1 1 ln 1 q 1 e 1 1 δ 0.5 1 λ .
We derive the first, second (median), and third quantiles by inserting q = 0.25 , 0.5 , and 0.75 . Furthermore, Bowley’s skewness ( γ 1 ) and Moor’s kurtosis ( γ 2 ) are calculated using the quantiles as below
γ 1 = Q 0.75 ; λ , δ 2 Q 0.5 ; λ , δ + Q 0.25 ; λ , δ Q 0.75 ; λ , δ Q 0.25 ; λ , δ ,
and
γ 2 = Q 0.875 ; λ , δ Q 0.625 ; λ , δ Q 0.375 ; λ , δ + Q 0.125 ; λ , δ Q 0.75 ; λ , δ Q 0.25 ; λ , δ .
Table 1 shows some numerical values of Q 1 , Q 2 , Q 3 , γ 1 , and γ 2 for the KMPTL distribution with numerous numerical combinations of the two shape parameters, λ and δ .

3.2. Moments

The w t h moment of a random variable Z with the KMPTL distribution is
μ w = E Z w = 0 1 z w f ( z ; λ , δ ) d z = 2 λ δ e e 1 0 1 z w + λ δ 1 1 z λ 2 z λ δ 1 e z λ δ 2 z λ δ d z ,
by using the exponential expansion
e z λ δ 2 z λ δ = i = 0 1 i i ! z λ δ i 2 z λ δ i ,
by inserting (13) in (12), we have
μ w = 2 λ δ e e 1 i = 0 1 i i ! 0 1 z w + λ δ ( i + 1 ) 1 1 z λ 2 z λ δ ( i + 1 ) 1 d z .
Let x = z λ , then
μ w = 2 δ e e 1 i = 0 1 i i ! 0 1 x w λ + δ ( i + 1 ) 1 1 x 2 x δ ( i + 1 ) 1 d x .
Let v = 1 x , then
μ w = 2 δ e e 1 i = 0 1 i i ! 0 1 v 1 + v δ ( i + 1 ) 1 1 v w λ + δ ( i + 1 ) 1 d v .
Employing the binomial expansion
1 + v δ ( i + 1 ) 1 = j = 0 δ ( i + 1 ) 1 j v j ,
by inserting (15) in (14), we have
μ w = 2 δ e e 1 i , j = 0 1 i i ! δ ( i + 1 ) 1 j 0 1 v j + 1 1 v w λ + δ ( i + 1 ) 1 d v ,
then
μ w = 2 δ e e 1 i , j = 0 1 i i ! δ ( i + 1 ) 1 j B j + 2 , w λ + δ ( i + 1 ) .
The moment-generating function the KMPTL distribution is
M t ( z ) = w = 0 t w w ! μ w = 2 δ e e 1 i , j , w = 0 1 i t w i ! w ! δ ( i + 1 ) 1 j B j + 2 , w λ + δ ( i + 1 ) .
Table 2 shows some numerical values of moments, variance ( σ 2 ), skewness ( α 1 ), kurtosis ( α 2 ), and coefficient of variation (CV) for the KMPTL distribution. Figure 4 shows 3D Plots of moments for the KMPTL distribution. Figure 4 shows that when the value of δ increases then the values of variance, skewness, kurtosis, and CV decrease, but the values of mean and index of dispersion (ID) increase.

3.3. Incomplete Moments

The q t h lower incomplete moment of a random variable Z having the KMPTL distribution is calculated from the next equation:
ϖ q t = 2 λ δ e e 1 0 t z q + λ δ 1 1 z λ 2 z λ δ 1 e z λ δ 2 z λ δ d z .
Employing (13) in (17), we get
ϖ q t = 2 λ δ e e 1 i = 0 1 i i ! 0 t z q + λ δ ( i + 1 ) 1 1 z λ 2 z λ δ ( i + 1 ) 1 d z .
Let x = z λ , then
ϖ q t = 2 δ e e 1 i = 0 1 i i ! 0 t λ x q λ + δ ( i + 1 ) 1 1 x 2 x δ ( i + 1 ) 1 d x .
Let v = 1 x , then
ϖ q t = 2 δ e e 1 i = 0 1 i i ! 0 1 t λ v 1 + v δ ( i + 1 ) 1 1 v q λ + δ ( i + 1 ) 1 d v ,
by inserting (15) in the above equation, we have
ϖ q t = 2 δ e e 1 i , j = 0 1 i i ! δ ( i + 1 ) 1 j 0 1 t λ v j + 1 1 v q λ + δ ( i + 1 ) 1 d v ,
then,
ϖ q t = 2 δ e e 1 i , j = 0 1 i i ! δ ( i + 1 ) 1 j B 1 t λ j + 2 , q λ + δ ( i + 1 ) ,
where B z ( . , . ) is the incomplete beta function.

4. Entropy

Entropy is one of the most significant measurements of uncertainty. Many kinds of entropy can be used to determine risk and dependability.

4.1. Rényi Measure of Entropy

The Rényi entropy [57] measure is calculated from the next equation:
R ζ = 1 1 ζ log E ζ λ , δ , ζ > 0 , ζ 1 ,
where E ζ λ , δ = 0 1 f z ; λ , δ ζ d z . Now, we need to calculate E ζ λ , δ . Then,
E ζ λ , δ = 0 1 f z ; λ , δ ζ d z = 2 λ δ e e 1 ζ 0 1 z ζ λ δ 1 1 z λ ζ 2 z λ δ 1 ζ e ζ z λ δ 2 z λ δ d z .
Applying (13) in the previous equation, we obtain
E ζ λ , δ = 2 λ δ e e 1 ζ i = 0 ζ i i ! 0 1 z λ δ i + ζ ζ 1 z λ ζ 2 z λ δ i + ζ ζ d z .
Let x = z λ , then
E ζ λ , δ = 2 λ δ e e 1 ζ i = 0 ζ i λ i ! 0 1 x δ i + ζ ζ λ + 1 λ 1 1 x ζ 2 x δ i + ζ ζ d x .
Let v = 1 x , then
E ζ λ , δ = 2 λ δ e e 1 ζ i = 0 ζ i λ i ! 0 1 v ζ 1 + v δ i + ζ ζ 1 v δ i + ζ ζ λ + 1 λ 1 d v .
By employing the binomial expansion (15) in the above equation, we get
E ζ λ , δ = i , j = 0 Ψ i , j 0 1 v ζ + j 1 v δ i + ζ ζ λ + 1 λ 1 d v ,
then
E ζ λ , δ = i , j = 0 Ψ i , j B ζ + j + 1 , δ i + ζ ζ λ + 1 λ ,
where Ψ i , j = 2 λ δ e e 1 ζ ζ i λ i ! δ i + ζ ζ j .
Inserting (21) into (19), then the Rényi entropy of the KMPTL distribution is
R ζ = 1 1 ζ log i , j = 0 Ψ i , j B ζ + j + 1 , δ i + ζ ζ λ + 1 λ , ζ > 0 , ζ 1 .

4.2. Arimoto Measure of Entropy

The Arimoto entropy [58] measure is calculated from the next equation:
A ζ = ζ 1 ζ E ζ λ , δ 1 ζ 1 , ζ > 0 , ζ 1 .
Inserting (21) into (23), then the Arimoto entropy of the KMPTL distribution is
A ζ = ζ 1 ζ i , j = 0 Ψ i , j B ζ + j + 1 , δ i + ζ ζ λ + 1 λ 1 ζ 1 , ζ > 0 , ζ 1 .

4.3. Tsallis Measure of Entropy

The Tsallis entropy [59] measure is calculated from the next equation:
T ζ = 1 ζ 1 1 E ζ λ , δ , ζ > 0 , ζ 1 .
Inserting (21) into (25), then the Tsallis entropy of the KMPTL distribution is
T ζ = 1 ζ 1 1 i , j = 0 Ψ i , j B ζ + j + 1 , δ i + ζ ζ λ + 1 λ , ζ > 0 , ζ 1 .

4.4. Havrda and Charvat Measure of Entropy

The Havrda and Charvat entropy [60] measure is calculated from the next equation:
H C ζ = 1 2 1 ζ 1 E ζ λ , δ 1 ζ 1 , ζ > 0 , ζ 1 .
Inserting (21) into (27), then the Havrda and Charvat entropy of the KMPTL distribution is
H C ζ = 1 2 1 ζ 1 i , j = 0 Ψ i , j B ζ + j + 1 , δ i + ζ ζ λ + 1 λ 1 ζ 1 , ζ > 0 , ζ 1 .
Table 3 and Table 4 show some numerical values of R ζ , A ζ , T ζ , and H C ζ for the KMPTL distribution.

5. Cumulative Residual Rényi Entropy

Plenty of authors have become interested in alternative metrics of uncertainty for probability distributions in recent years, particularly in survival and reliability analysis investigations. As a result, Ref. [61] proposed the cumulative residual Rényi entropy as
ρ ζ = 1 1 ζ log D ζ λ , δ , ζ > 0 , ζ 1 ,
where D ζ λ , δ = 0 1 s z ; λ , δ ζ d z . Now, we need to calculate D ζ λ , δ . Then,
D ζ λ , δ = 0 1 S ( z ; λ , δ ) ζ d z = 0 1 1 e e 1 1 e z λ δ 2 z λ δ ζ d z .
By applying the binomial expansion in the previous equation two times, we get
D ζ λ , δ = i , j = 0 1 i + j ζ i i j e e 1 i 0 1 e j z λ δ 2 z λ δ d z .
By applying the exponential expansion (13) in the previous equation, we get
D ζ λ , δ = i , j , k = 0 1 i + j + k j k k ! ζ i i j e e 1 i 0 1 z k λ δ 2 z λ k δ d z .
Let x = z λ , then
D ζ λ , δ = i , j , k = 0 1 i + j + k j k λ k ! ζ i i j e e 1 i 0 1 x k δ + 1 λ 1 2 x k δ d x .
Let v = 1 x , then
D ζ λ , δ = i , j , k = 0 1 i + j + k j k λ k ! ζ i i j e e 1 i 0 1 1 v k δ + 1 λ 1 1 + v k δ d v .
By applying the binomial theory (15) in the previous equation, we get
D ζ λ , δ = i , j , k , m = 0 Φ i , j , k , m 0 1 v m 1 v k δ + 1 λ 1 d v .
Then,
D ζ λ , δ = i , j , k , m = 0 Φ i , j , k , m B m + 1 , k δ + 1 λ ,
where, Φ i , j , k , m = 1 i + j + k j k λ k ! ζ i i j k δ m e e 1 i . Inserting (30) into (29), then the cumulative residual Rényi entropy of the KMPTL distribution is
ρ ζ = 1 1 ζ log i , j , k , m = 0 Φ i , j , k , m B m + 1 , k δ + 1 λ , ζ > 0 , ζ 1 .

6. Estimation Methods Based on Sampling Approach

In this section, the MLE and Bayesian have been discussed. The procedures used to draw conclusions or make generalizations about a population parameter make up the estimate theory. Differentiating between the maximum likelihood approach and the Bayesian method of estimate is the current fashion. The Bayesian approach makes use of sample data information as well as previously acquired subjective knowledge about the probability distribution of the unknown parameters. In addition, the most popular technique for gathering data is the SRS approach. RSS approaches may be employed in these scenarios to study greater proportions of samples from the population under consideration and enhance the accuracy of statistical inference. This approach was first discussed and introduced by [62], which originally proposed the RSS approach. Numerous investigations have demonstrated that RSS statistical processes are numerically and theoretically superior to their SRS competitors.
The next step outlines the technique for choosing the samples:
  • Choose observations from an r-set, each of which contains r randomly chosen units.
  • Using an accessible auxiliary variable or individual assessment, the units are rated.
  • The lowest unit in the first set should be chosen, followed by the second-lowest unit in the second set, and so on until the fourth unit in the fourth set is chosen.
    1 . z ( 1 : r ) ( 1 ) ̲ z ( 2 : r ) ( 1 ) z ( r : r ) ( 1 ) z ( 1 ) c = z ( 1 : r ) ( 1 ) 2 . z ( 1 : r ) ( 2 ) z ( 2 : r ) ( 2 ) ̲ z ( r : r ) ( 2 ) z ( 2 ) c = z ( 2 : r ) ( 2 ) n . z ( 1 : r ) ( r ) z ( 2 : r ) ( r ) z ( r : r ) ( r ) ̲ z ( r ) c = z ( r : r ) ( r )
    where c = 1 , 2 , , m as a cycle iteration.
  • The process returns ranked set samples with an r. The operation will therefore be carried out m times in order to obtain the necessary sample n, where n = m r , c = 1 , 2 , , m , and h = 1 , 2 , , r samples. According to the foundation of flawless judgement ranking, z ( h ) c has the same distribution; see citation [63].
    g ( h ) c ( z ) = r ! ( h 1 ) ! ( r h ) ! [ F ( z ( h ) c ) ] h 1 [ 1 F ( z ( h ) c ) ] r h f ( z ( h ) c ) , 0 < z ( h ) c < .
For more information, see recent papers such as [64,65,66]. In this section, maximum likelihood (ML) and Bayesian using SRS and RSS have been discussed.

6.1. Maximum Likelihood Estimation under SRS

In this subsection, first, we need to look into the ML estimates (MLEs) of λ and δ according to SRS. Assume that Z i , where i = ( 1 , , n ) . The likelihood function (LFN) using SRS is:
L ( z ; Δ ) = 2 n λ n δ n e n ( e 1 ) n i = 1 n z i λ δ 1 1 z i λ 2 z i λ δ 1 e i = 1 n z i λ δ 2 z i λ δ .
The ln-LFN under SRS is:
( z ; Δ ) = n ln ( 2 ) + ln ( λ ) + ln ( δ ) + 1 ln ( e 1 ) + ( λ δ 1 ) i = 1 n ln ( z i ) + i = 1 n ln 1 z i λ + ( δ 1 ) i = 1 n ln 2 z i λ i = 1 n z i λ δ 2 z i λ δ .
In order to solve the non-linear log-LFNs that are produced by differentiating Equation (34) (with respect to the distribution parameters Δ = ( λ , δ ) ) and equating it to zero, Equation (34) can be explicitly maximized using the R program by a “mle2” function, which implements the NelderMead (NM) maximization procedure for MLE calculations.

6.2. Maximum Likelihood Estimation under RSS

Assume that c-cycle of RSS is z ( h ) c ; h = 1 , , r , c = 1 , 2 , , m , which has KMPTL distribution with vector parameters Δ . Equation (32) yields the next function under RSS:
g ( h ) c ( z | Δ ) = r ! ( h 1 ) ! ( r h ) ! e e 1 1 e z ( h ) c λ δ 2 z ( h ) c λ δ h 1 2 λ δ e e 1 z ( h ) c λ δ 1 1 e e 1 1 e z ( h ) c λ δ 2 z ( h ) c λ δ r h 1 z ( h ) c λ 2 z ( h ) c λ δ 1 e z ( h ) c λ δ 2 z ( h ) c λ δ .
By utilizing Equation (35), the LF under RSS is provided via
L R S S ( z | Δ ) = c = 1 m h = 1 r r ! ( h 1 ) ! ( r h ) ! e e 1 1 e z ( h ) c λ δ 2 z ( h ) c λ δ h 1 z ( h ) c λ δ 1 2 n λ n δ n e n ( e 1 ) n c = 1 m h = 1 r 1 e e 1 1 e z ( h ) c λ δ 2 z ( h ) c λ δ r h 1 z ( h ) c λ 2 z ( h ) c λ δ 1 e z ( h ) c λ δ 2 z ( h ) c λ δ .
In this case, the ln-LF of the KMPTL distribution is supplied by
R S S ( z | Δ ) = n ln ( 2 ) + ln ( λ ) + ln ( δ ) + 1 ln ( e 1 ) + c = 1 m h = 1 r ln r ! ( h 1 ) ! ( r h ) ! + c = 1 m h = 1 r ( h 1 ) ln e e 1 + c = 1 m h = 1 r ( h 1 ) ln 1 e z ( h ) c λ δ 2 z ( h ) c λ δ + ( λ δ 1 ) c = 1 m h = 1 r ln ( z ( h ) c ) + c = 1 m h = 1 r ( r h ) ln 1 e e 1 1 e z ( h ) c λ δ 2 z ( h ) c λ δ + c = 1 m h = 1 r ln 1 z ( h ) c λ + ( δ 1 ) c = 1 m h = 1 r ln 2 z ( h ) c λ c = 1 m h = 1 r z ( h ) c λ δ 2 z ( h ) c λ δ .
In order to solve the non-linear RSS of log-LFNs that are created by differentiating Equation (37) (with regards to the distribution parameters Δ ) and equating it to 0, Equation (37) can be explicitly maximized employing the R program by a “mle2” function, which implements the NM maximization procedure for MLE calculations; see [67].

6.3. Bayesian Estimation

In many different contexts and fields, such as physics (see [68]), food chain (see [69]), epidemiology (see [70]), environmental (see [71]), COVID-19 (see [72]), and econometrics (see [73]), Bayesian approaches for parameter estimation have been successfully used. One benefit of using Bayesian approaches is that they enable model estimation when more complex models prevent standard estimation from succeeding [74].
The Bayes estimate based on ranked set sampling of the Δ function under the square error loss (SEL) function will now be covered. The posterior distributions given the data are used to construct the Bayes estimates (BEs) of the parameters in the Δ BE vector. The suggested method is described in brief below. Assume that I and K are the iterations and sample burn, respectively. The posterior mean is then used to minimize the SEL function for the presumptive prior distribution as follows:
Δ ˜ = 1 I K j = K + 1 I Δ ˜ ( j )
where Δ ˜ ( j ) is the Bayesian estimation vector for Δ at iteration ( j ) . Furthermore, using the R software’s coda and HDInterval package, developed in [75] and [76], respectively, we can determine MCMC results and the highest posterior density (HPD) credible interval for Δ , respectively.
Let z 1 , z 2 , , z n be associated observations, and z 1 , z 2 , , z n be a random sample of size n taken from a general distribution of the KMPTL distribution with unknown parameters, assumed to have independent rvs that adhere to the gamma distribution with the PDF specified by
Π ( Δ ) λ a 1 1 δ a 2 1 e b 1 λ + b 2 δ .
To determine the proper hyper-parameters for the independent joint prior, use the estimate and variance-covariance matrix of the MLE technique. By equating the gamma priors’ mean and variance, the estimated hyper-parameters can be written as follows:
a 1 = 1 L j = 1 L λ ^ j 2 1 L 1 i = 1 L λ ^ j 1 L i = 1 L λ j ^ 2 ; a 2 = 1 L j = 1 L δ ^ j 2 1 L 1 i = 1 L δ ^ j 1 L i = 1 L δ j ^ 2
b 1 = 1 L i = 1 L λ ^ j 1 L 1 i = 1 L λ j ^ 1 L i = 1 L λ ^ j 2 ; b 2 = 1 L i = 1 L δ ^ j 1 L 1 i = 1 L δ j ^ 1 L i = 1 L δ ^ j 2 .
where L denotes the quantity of MLE iterations.
The parameters’ posterior distribution can be stated as follows:
π * Δ d a t a = Π ( Δ ) L ( Δ d a t a ) 0 0 Π ( Δ ) L ( Δ d a t a ) d λ d δ .
where d a t a is the generated sample by SRS or RSS. It is possible to express the joint posterior to the proportionality as an equation, as shown in Equation (40).
π * Δ d a t a c = 1 m h = 1 r r ! ( h 1 ) ! ( r h ) ! e e 1 1 e z ( h ) c λ δ 2 z ( h ) c λ δ h 1 z ( h ) c λ δ 1 λ n + a 1 1 δ n + a 2 1 e b 1 λ + b 2 δ c = 1 m h = 1 r 1 e e 1 1 e z ( h ) c λ δ 2 z ( h ) c λ δ r h 1 z ( h ) c λ 2 z ( h ) c λ δ 1 e z ( h ) c λ δ 2 z ( h ) c λ δ .
The complete conditionals for λ and δ can be written, up to proportionality, as
π * λ δ , d a t a c = 1 m h = 1 r 1 e z ( h ) c λ δ 2 z ( h ) c λ δ h 1 z ( h ) c λ δ 1 λ n + a 1 1 e b 1 λ c = 1 m h = 1 r 1 e e 1 1 e z ( h ) c λ δ 2 z ( h ) c λ δ r h 1 z ( h ) c λ 2 z ( h ) c λ δ 1 e z ( h ) c λ δ 2 z ( h ) c λ δ . π * δ λ d a t a c = 1 m h = 1 r 1 e z ( h ) c λ δ 2 z ( h ) c λ δ h 1 z ( h ) c λ δ 1 δ n + a 2 1 e b 2 δ c = 1 m h = 1 r 1 e e 1 1 e z ( h ) c λ δ 2 z ( h ) c λ δ r h 2 z ( h ) c λ δ 1 e z ( h ) c λ δ 2 z ( h ) c λ δ .
We can use the Metropolis–Hastings algorithm (MHA) and the Gibbs sampling technique to produce samples from the posterior distributions as none of these posterior PDFs relate to a single common distribution. References [77,78,79] provide additional information on this topic. The normal distribution is the proposal distribution used by the MHA. The detailed steps are given below, taking into account the Gibbs sampling method:
  • Begin with initial values λ ( 0 ) = λ ^ , δ ( 0 ) = δ ^ ;
  • Put t = 1;
  • Utilize the MHA to create λ ( t ) ;
  • Utilize the MHA to create δ ( t ) ;
  • Set t = t + 1;
  • Repeat the procedures items I times.
Based on the SEL function, Δ ˜ can be determined for a large enough I, which make convergence of MCMC results. Furthermore, the method described in [80] can be used to generate a roughly 100 ( 1 α ) % HPD credible interval of Δ .

7. Simulation

Simulation studies has been used to produce random sampling of the proposed model. Because of some parameter factors, simulation studies are characterized by understanding the behavior of statistical approaches. This enables us to take into account technique characteristics such as bias, MSE, standard deviation, etc.; see also [81].
Using the R-4.3.0 program, a simulation research was carried out to compare the effectiveness of the ML and BE approaches under the SRS and RSS sampling strategies, as stated above for the unique KMPTL distribution. In this regard, the KMPTL distribution is used to generate M = 1000 moderate samples for each techniques, each with size n = (8,12,17). The parameter Δ = ( λ , δ ) values have been selected as:
  • In Table 5: λ = 0.5 and δ = 0.5 , 2 , 3 .
  • In Table 6: λ = 2 and δ = 0.5 , 2 , 3 .
  • In Table 7: λ = 3 and δ = 0.5 , 2 , 3 .
We utilise I = 12,000 iterations and the first 16.67% as burn-in samples for the Bayes estimation. The bias and mean square error (MSE) of the estimates are examined. The table results show the simulation findings, including the length of confidence intervals (LCI) with converge probability (CP). In LCI, the asymptotic CI (LACI) has been obtained for MLE, and credible CI (LCCI) for Bayesian has been obtained. In addition, the relative efficiency (RE) of sampling techniques were
R E 1 ( Δ ) = M S E S R S ( Δ ) M S E R S S 1 ( Δ ) × 100 % , R E 2 ( Δ ) = M S E S R S ( Δ ) M S E R S S 2 ( Δ ) × 100 % , R E 3 ( Δ ) = M S E R S S 1 ( Δ ) M S E R S S 2 ( Δ ) × 100 % .
Below, we provide a few crucial procedures for the numerical simulation:
  • Select the replication number M & I, the sample size n, and the parameter values;
  • Select the replication number cycle m, and the sample size of each cycle r;
  • Generate SRS and RSS from LMPTL by using the “rss” package in the R-4.3.0 program and qf (11) of the KMPTL distribution.
  • Using the simulated data, determine the MLEs and BEs of the KMPTL distribution’s parameters;
  • Repeat the above steps, M times;
  • Determine the mean of bias, average MSE, RE, LCI, and CP for each parameter.
From Table 5, Table 6 and Table 7, we can conclude the following:
  • In every calculation, the bias, MSE and LCI become smaller as n is increased.
  • The relevance of the Bias, MSE, and LCI for KMPL distribution parameters decreases as the number of cycles (r) in the RSS sampling rises, but the RE rises.
  • As the sample size for each cycle (m) rises in the RSS sampling, the significance of the Bias, MSE, and LCI for KMPTL distribution parameters declines, while the RE increases.
  • Comparatively speaking, Bayesian estimates are substantially more efficient than MLE for the majority of KMPTL distribution parameters.
  • Comparatively speaking, RSS techniques are substantially more efficient than SRS for the majority of KMPTL distribution parameters.
  • The CP rises when the sample size increases.
  • Comparatively speaking, credible CI of HPD is substantially more efficient than asymptotic CI for the majority of the KMPTL distribution parameters.
  • MSE increases when parameter δ increased

8. Applications

In this section, we used two real-world datasets to compare the KMPTL model to several other known competing models: power Topp–Leone (PTL), unit-Gompertz (UG), unit-Lindley (UL), Topp–Leone (TL), unit generalized log Burr XII (UGLBXII), Unit Exponential Pareto (UEPD), Kumaraswamy (Kw), Beta, and Marshall-Olkin Kumaraswamy (MOK). To estimate the parameters of the competing models, the MLE approach is employed. To choose the optimal model, different criteria have been used, such as the Akaike information criterion (AM1), correct Akaike information criterion (SM2), Bayesian information criterion (SM3), and Hannan–Quinn information criterion (SM4) values. In addition, different goodness of fit measures have been discussed, such as the Kolmogorov–Smirnov distance (KSD), Anderson–Darling (AD), and Cramer-von-Mises (CVM), for each distribution.

8.1. Economic Growth Data

The trade share variable’s values in the famed “Determinants of Economic Growth Data” are taken into account in the first dataset, which is called the trade share dataset. Along with factors that may be associated with growth, the growth rates of up to 61 different countries are taken into consideration. The information is publicly accessible online as an addition to [82]. The trade share dataset consists of the following numbers: “0.1405 0.1566 0.1577 0.1604 0.1608 0.2215 0.2994 0.3131 0.3246 0.3247 0.3295 0.3300 0.3379 0.3397 0.3523 0.3589 0.3933 0.4176 0.4258 0.4356 0.4421 0.4444 0.4505 0.4558 0.4683 0.4733 0.4846 0.4889 0.5096 0.5177 0.5278 0.5347 0.5433 0.5442 0.5508 0.5527 0.5606 0.5607 0.5671 0.5753 0.5828 0.6030 0.6050 0.6136 0.6261 0.6395 0.6469 0.6512 0.6816 0.6994 0.7048 0.7292 0.7430 0.7455 0.7798 0.7984 0.8147 0.8230 0.8302 0.8342 0.9794”. The data were initially examined in terms of outliers by drawing a box-plot, and TTT was obtained and compared to the hazard line, and we noticed that the data did not contain outliers and also TTT is an increasing vector, and this corresponds to the hazard line; see Figure 5.
When compared to all other models used to fit the existing economic growth data, the KMPTL model has the lowest distance KS in Table 8. The fit CDF with empirical CDF and estimated PDF with histogram are displayed for KMPTL and others models in Figure 6. In addition, QQ-plot and PP-plot are displayed for KMPTL distribution in Figure 7.
Figure 8 shows the profile ln-likelihood of the estimated parameters with economic growth data. They provide evidence of the MLE’s existence and distinctiveness. Figure 9 shows the convergence line for MCMC results in a trace plot of the theses results for the KMPTL parameters with economic growth data. To confirm the normality plot of MCMC results, Figure 10 depicts the density plot of posterior MCMC results for KMPTL parameters for economic growth data.

8.2. Physics Data

The second dataset consisted of 30 measurements, which have been discussed by [83] and made by Quesenberry and Hales [84] to determine the tensile strength of polyester fibres. Theses data are as follows: 0.023, 0.032, 0.054, 0.069, 0.081, 0.094, 0.105, 0.127, 0.148, 0.169, 0.188, 0.216, 0.255, 0.277, 0.311, 0.361, 0.376, 0.395, 0.432, 0.463, 0.481, 0.519, 0.529, 0.567, 0.642, 0.674, 0.752, 0.823, 0.887, 0.926. The data were initially examined in terms of outliers by drawing a box-plot, and TTT was obtained and compared to the hazard line, and we noticed that the data did not contain outliers and also that TTT is an increasing vector, and this corresponds to the hazard line; see Figure 11.
When compared to all other models used to fit the existing physical data, the KMPTL model has the lowest value of distance KS, as seen in Table 9. The fit CDF with empirical CDF and estimated PDF with histogram are displayed for KMPTL and other models in Figure 12. In addition, QQ-plot and PP-plot are displayed for KMPTL distribution in Figure 13.
Table 10 shows the Bayesian estimation for all data, and Figure 14 shows the profile ln-likelihood of ML parameters for polyester fibers data. They both provide evidence of the MLE’s existence and distinctiveness. Figure 15 shows the convergence line of MCMC results with a trace plot of theses results for the KMPTL parameters with polyester fibers data. To confirm the normality plot for MCMC estimation, the density plot of posterior MCMC results for KMPTL parameters for polyester fibres data is shown in Figure 16.

9. Conclusions and Summary

In this article, we proposed a new two-parameter distribution called the KMPTL distribution. Several statistical and mathematical aspects of the KMPTL distribution, such as the qf, moments, generating function, and incomplete moments, are determined by calculating. Some measures of entropy are investigated. The CRRE is computed. To estimate the parameters of the KMPTL distribution, both ML and Bayesian estimation methods are used under SRS and RSS. The simulation investigation was conducted to estimate the model parameters of the KMPTL distribution utilizing SRS and RSS in order to demonstrate that RSS is better than SRS. Using two real-world datasets, we proved that the KMPTL distribution has greater flexibility than the PTL distribution and the other nine competing statistical distributions.

Author Contributions

Conceptualization, I.E.; Methodology, N.A., M.S., A.S.A.-M., M.E., E.M.A. and I.E.; Software, N.A., M.S., A.S.A.-M., M.E., E.M.A. and I.E.; Formal analysis, N.A., M.S., A.S.A.-M., M.E., E.M.A. and I.E.; Data curation, N.A., M.S., A.S.A.-M., M.E., E.M.A. and I.E.; Writing—original draft, N.A., M.S., A.S.A.-M., M.E., E.M.A. and I.E.; Supervision, N.A., M.S., A.S.A.-M., M.E., E.M.A. and I.E. All authors have read and agreed to the published version of the manuscript.

Funding

This research was funded by Imam Muhammad ibn Saud Islamic University grant number (221412039).

Data Availability Statement

Data sets are available in the application section.

Acknowledgments

The authors extend their appreciation to the Deanship of Scientific Research, Imam Mohammad Ibn Saud Islamic University (IMSIU), Saudi Arabia, for funding this research work through Grant No. (221412039).

Conflicts of Interest

The authors declare no conflict of interest.

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Figure 1. Some curves of the PDF for the KMPTL distribution.
Figure 1. Some curves of the PDF for the KMPTL distribution.
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Figure 2. Some curves of the HRF for the KMPTL distribution.
Figure 2. Some curves of the HRF for the KMPTL distribution.
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Figure 3. Monotone plot of the HRF for the KMPTL distribution.
Figure 3. Monotone plot of the HRF for the KMPTL distribution.
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Figure 4. 3D Plots of moments for the KMPTL distribution.
Figure 4. 3D Plots of moments for the KMPTL distribution.
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Figure 5. Box-plot, TTT plot, and hazard plot for KMPTL: economic growth data.
Figure 5. Box-plot, TTT plot, and hazard plot for KMPTL: economic growth data.
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Figure 6. Estimated CDF and PDF for KMPTL and other models: economic growth data.
Figure 6. Estimated CDF and PDF for KMPTL and other models: economic growth data.
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Figure 7. Estimated PP and QQ for KMPTL: economic growth data.
Figure 7. Estimated PP and QQ for KMPTL: economic growth data.
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Figure 8. Examination of the MLE maxillary value of the KMPTL distribution: economic growth data.
Figure 8. Examination of the MLE maxillary value of the KMPTL distribution: economic growth data.
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Figure 9. Examination of the Bayesian convergence measures of the KMPTL distribution: economic growth data.
Figure 9. Examination of the Bayesian convergence measures of the KMPTL distribution: economic growth data.
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Figure 10. Examination of the Bayesian frequency measures of parameters of the KMPTL distribution: economic growth data.
Figure 10. Examination of the Bayesian frequency measures of parameters of the KMPTL distribution: economic growth data.
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Figure 11. Box-plot, TTT plot, and hazard plot for KMPTL: polyester fibers data.
Figure 11. Box-plot, TTT plot, and hazard plot for KMPTL: polyester fibers data.
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Figure 12. Estimated CDF and PDF for KMPTL and other models: polyester fibers data.
Figure 12. Estimated CDF and PDF for KMPTL and other models: polyester fibers data.
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Figure 13. Estimated PP and QQ for KMPTL: polyester fibers data.
Figure 13. Estimated PP and QQ for KMPTL: polyester fibers data.
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Figure 14. Examination of the MLE maxillary value of the KMPTL distribution: polyester fibers data.
Figure 14. Examination of the MLE maxillary value of the KMPTL distribution: polyester fibers data.
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Figure 15. Examination of the Bayesian convergence measures of the KMPTL distribution: polyester fibers data.
Figure 15. Examination of the Bayesian convergence measures of the KMPTL distribution: polyester fibers data.
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Figure 16. Examination of the Bayesian frequency measures of parameters of the KMPTL distribution: polyester fibers data.
Figure 16. Examination of the Bayesian frequency measures of parameters of the KMPTL distribution: polyester fibers data.
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Table 1. Results of some numerical values of Q 1 , Q 2 , Q 3 , γ 1 , and γ 2 for the KMPTL distribution.
Table 1. Results of some numerical values of Q 1 , Q 2 , Q 3 , γ 1 , and γ 2 for the KMPTL distribution.
δ λ Q 1 Q 2 Q 3 γ 1 γ 2
1.51.80.3720.5220.6760.0151.159
2.30.4620.6010.736−0.0171.17
2.80.530.6590.778−0.0381.18
3.30.5830.7020.808−0.0521.187
3.80.6260.7350.831−0.0631.194
4.30.6610.7620.849−0.0711.199
4.80.690.7840.864−0.0781.204
5.30.7150.8020.876−0.0831.208
5.80.7360.8170.886−0.0871.211
6.30.7540.8310.894−0.0911.214
21.80.4470.5850.721−0.0051.172
2.30.5330.6570.774−0.0311.182
2.80.5960.7080.81−0.0471.19
3.30.6450.7460.836−0.0591.197
3.80.6830.7760.856−0.0671.202
4.30.7140.7990.872−0.0741.206
4.80.740.8180.884−0.0791.21
5.30.7610.8330.895−0.0831.213
5.80.7790.8470.903−0.0871.215
6.30.7950.8580.911−0.0891.218
3.51.80.5770.6870.791−0.0281.19
2.30.650.7450.832−0.0451.198
2.80.7020.7850.86−0.0561.204
3.30.7410.8150.88−0.0641.208
3.80.7710.8370.895−0.0691.211
4.30.7940.8540.906−0.0741.214
4.80.8140.8690.916−0.0771.216
5.30.830.880.923−0.081.218
5.80.8430.890.93−0.0821.22
6.30.8540.8980.935−0.0841.221
51.80.6460.7390.826−0.0361.198
2.30.710.7890.861−0.0491.204
2.80.7550.8230.884−0.0581.208
3.30.7880.8480.901−0.0641.212
3.80.8130.8670.913−0.0681.214
4.30.8330.8810.923−0.0711.216
4.80.8490.8930.931−0.0741.218
5.30.8620.9020.937−0.0761.219
5.80.8730.910.942−0.0781.22
6.30.8830.9170.947−0.0791.221
Table 2. Results of some moments, σ 2 , α 1 , α 2 , and CV for the KMPTL distribution.
Table 2. Results of some moments, σ 2 , α 1 , α 2 , and CV for the KMPTL distribution.
δ λ μ 1 μ 2 μ 3 μ 4 σ 2 α 1 α 2 CV
1.51.80.5240.3160.2090.1480.041−0.0122.2830.387
2.30.5950.3890.2710.1990.035−0.1822.4070.313
2.80.6480.4480.3270.2470.029−0.3222.5690.264
3.30.6880.4980.3750.2910.025−0.4272.7360.228
3.80.7210.540.4180.3320.021−0.5112.8940.201
4.30.7470.5760.4560.3680.018−0.5783.040.179
4.80.7690.6070.4890.4010.016−0.6343.1750.162
5.30.7870.6330.5190.4320.014−0.6823.2970.148
5.80.8030.6570.5450.4590.012−0.7223.4090.136
6.30.8160.6770.5690.4840.011−0.7573.510.126
21.80.5810.3720.2560.1850.034−0.1182.3880.319
2.30.6480.4470.3240.2440.028−0.2892.5650.257
2.80.6960.5070.3830.2980.022−0.4112.7480.215
3.30.7330.5560.4340.3460.018−0.5022.920.185
3.80.7620.5960.4770.3890.015−0.5733.0750.163
4.30.7860.630.5150.4270.013−0.633.2130.145
4.80.8050.6590.5470.4610.011−0.6773.3350.131
5.30.8210.6830.5760.4910.0096−0.7173.4450.119
5.80.8340.7050.6010.5180.0084−0.753.5430.11
6.30.8460.7230.6240.5430.0074−0.7793.6310.101
3.51.80.6790.4830.3570.2730.022−0.2992.640.22
2.30.7350.5570.4330.3440.017−0.4292.8470.175
2.80.7750.6130.4940.4050.013−0.5183.0240.146
3.30.8040.6570.5440.4560.01−0.5843.1730.125
3.80.8270.6920.5850.50.0082−0.6343.2980.109
4.30.8450.7210.620.5370.0068−0.6743.4040.097
4.80.8590.7440.6490.570.0057−0.7063.4950.087
5.30.8720.7640.6740.5980.0048−0.7333.5740.08
5.80.8820.7810.6960.6230.0041−0.7563.6420.073
6.30.890.7960.7150.6450.0036−0.7753.7020.067
51.80.7310.550.4250.3360.016−0.3732.7840.174
2.30.780.6210.5020.4120.012−0.4792.9780.138
2.80.8150.6720.5610.4740.0087−0.5513.1340.115
3.30.8390.7120.6080.5240.0068−0.6043.2590.098
3.80.8590.7430.6470.5660.0054−0.6443.3610.086
4.30.8740.7680.6780.6020.0044−0.6753.4460.076
4.80.8860.7880.7040.6320.0037−0.73.5170.068
5.30.8960.8050.7270.6580.0031−0.7213.5770.062
5.80.9040.820.7460.6810.0026−0.7393.6290.057
6.30.9110.8330.7630.7010.0023−0.7533.6750.052
Table 3. Some numerical values of R ζ , A ζ , T ζ , and H C ζ for the KMPTL distribution at ζ = 0.5 and 0.8.
Table 3. Some numerical values of R ζ , A ζ , T ζ , and H C ζ for the KMPTL distribution at ζ = 0.5 and 0.8.
δ λ ζ = 0.5 ζ = 0.8
R ζ HC ζ A ζ T ζ R ζ HC ζ A ζ T ζ
1.51.8−0.133−0.155−0.125−0.129−0.18−0.237−0.176−0.177
2.3−0.2−0.23−0.182−0.191−0.259−0.34−0.251−0.252
2.8−0.277−0.313−0.242−0.259−0.348−0.452−0.333−0.336
3.3−0.356−0.394−0.299−0.326−0.436−0.562−0.413−0.418
3.8−0.432−0.469−0.351−0.389−0.521−0.665−0.488−0.495
4.3−0.505−0.539−0.397−0.446−0.601−0.762−0.558−0.566
4.8−0.575−0.603−0.437−0.499−0.677−0.851−0.623−0.633
5.3−0.64−0.662−0.473−0.548−0.748−0.934−0.682−0.694
5.8−0.703−0.715−0.505−0.593−0.815−1.011−0.737−0.752
6.3−0.762−0.765−0.533−0.634−0.878−1.083−0.788−0.805
21.8−0.201−0.231−0.182−0.191−0.26−0.34−0.251−0.253
2.3−0.297−0.333−0.257−0.276−0.368−0.478−0.352−0.355
2.8−0.394−0.431−0.325−0.357−0.477−0.611−0.449−0.455
3.3−0.487−0.522−0.386−0.432−0.579−0.735−0.539−0.547
3.8−0.575−0.603−0.437−0.5−0.674−0.848−0.62−0.63
4.3−0.657−0.676−0.482−0.56−0.762−0.951−0.694−0.707
4.8−0.734−0.741−0.52−0.614−0.844−1.045−0.761−0.777
5.3−0.806−0.801−0.553−0.663−0.92−1.13−0.822−0.84
5.8−0.873−0.854−0.582−0.708−0.991−1.21−0.878−0.899
6.3−0.937−0.903−0.608−0.748−1.058−1.283−0.93−0.954
3.51.8−0.392−0.429−0.324−0.356−0.471−0.605−0.445−0.45
2.3−0.531−0.563−0.412−0.466−0.622−0.787−0.576−0.585
2.8−0.658−0.677−0.482−0.561−0.758−0.946−0.69−0.703
3.3−0.774−0.774−0.539−0.642−0.88−1.085−0.79−0.807
3.8−0.878−0.858−0.584−0.711−0.989−1.207−0.876−0.897
4.3−0.973−0.93−0.622−0.771−1.089−1.316−0.953−0.978
4.8−1.061−0.994−0.654−0.823−1.179−1.413−1.021−1.051
5.3−1.142−1.05−0.681−0.87−1.263−1.501−1.083−1.116
5.8−1.216−1.1−0.704−0.911−1.34−1.581−1.139−1.175
6.3−1.286−1.145−0.724−0.949−1.412−1.654−1.19−1.23
51.8−0.541−0.572−0.418−0.474−0.63−0.797−0.583−0.592
2.3−0.702−0.714−0.504−0.592−0.801−0.995−0.726−0.74
2.8−0.843−0.831−0.57−0.688−0.949−1.162−0.845−0.864
3.3−0.969−0.927−0.62−0.768−1.079−1.306−0.946−0.971
3.8−1.081−1.008−0.661−0.835−1.195−1.43−1.033−1.063
4.3−1.182−1.077−0.693−0.892−1.3−1.539−1.11−1.145
4.8−1.274−1.137−0.72−0.942−1.394−1.637−1.177−1.217
5.3−1.359−1.19−0.743−0.986−1.481−1.724−1.238−1.282
5.8−1.437−1.237−0.762−1.025−1.561−1.803−1.292−1.341
6.3−1.509−1.279−0.779−1.06−1.635−1.876−1.342−1.395
Table 4. Some numerical values of R ζ , A ζ , T ζ , and H C ζ for the KMPTL distribution at ζ = 1.2 and 2.0.
Table 4. Some numerical values of R ζ , A ζ , T ζ , and H C ζ for the KMPTL distribution at ζ = 1.2 and 2.0.
δ λ ζ = 1.2 ζ = 2
R ζ HC ζ A ζ T ζ R ζ HC ζ A ζ T ζ
1.51.8−0.225−0.355−0.229−0.23−0.284−0.656−0.305−0.328
2.3−0.312−0.498−0.321−0.322−0.378−0.92−0.417−0.46
2.8−0.409−0.658−0.423−0.426−0.481−1.237−0.544−0.618
3.3−0.503−0.818−0.525−0.53−0.582−1.578−0.675−0.789
3.8−0.593−0.974−0.624−0.63−0.676−1.932−0.804−0.966
4.3−0.678−1.122−0.718−0.726−0.764−2.295−0.931−1.148
4.8−0.757−1.263−0.807−0.818−0.847−2.663−1.054−1.332
5.3−0.831−1.397−0.892−0.905−0.923−3.035−1.173−1.518
5.8−0.901−1.525−0.972−0.987−0.995−3.41−1.289−1.705
6.3−0.966−1.647−1.048−1.066−1.062−3.786−1.402−1.893
21.8−0.313−0.499−0.321−0.323−0.38−0.924−0.418−0.462
2.3−0.43−0.694−0.446−0.449−0.504−1.31−0.573−0.655
2.8−0.545−0.89−0.571−0.576−0.625−1.735−0.733−0.868
3.3−0.653−1.078−0.69−0.697−0.737−2.179−0.891−1.089
3.8−0.752−1.254−0.802−0.812−0.84−2.632−1.044−1.316
4.3−0.844−1.421−0.906−0.92−0.935−3.092−1.191−1.546
4.8−0.929−1.577−1.005−1.021−1.022−3.556−1.334−1.778
5.3−1.008−1.725−1.097−1.116−1.103−4.023−1.471−2.012
5.8−1.081−1.865−1.185−1.207−1.178−4.493−1.603−2.246
6.3−1.15−1.997−1.267−1.292−1.247−4.963−1.732−2.482
3.51.8−0.538−0.877−0.563−0.568−0.616−1.702−0.721−0.851
2.3−0.695−1.153−0.737−0.746−0.779−2.358−0.952−1.179
2.8−0.836−1.406−0.897−0.91−0.924−3.036−1.174−1.518
3.3−0.962−1.638−1.043−1.06−1.052−3.726−1.384−1.863
3.8−1.074−1.851−1.176−1.198−1.167−4.422−1.584−2.211
4.3−1.176−2.048−1.299−1.326−1.27−5.123−1.774−2.561
4.8−1.268−2.231−1.413−1.444−1.364−5.826−1.956−2.913
5.3−1.354−2.402−1.518−1.554−1.451−6.531−2.131−3.266
5.8−1.432−2.562−1.617−1.658−1.53−7.238−2.298−3.619
6.3−1.505−2.713−1.711−1.756−1.604−7.945−2.46−3.973
51.8−0.703−1.166−0.746−0.755−0.785−2.387−0.962−1.193
2.3−0.878−1.483−0.946−0.96−0.965−3.251−1.241−1.625
2.8−1.03−1.768−1.124−1.144−1.12−4.132−1.502−2.066
3.3−1.164−2.024−1.284−1.31−1.256−5.022−1.747−2.511
3.8−1.282−2.258−1.429−1.461−1.376−5.917−1.979−2.959
4.3−1.388−2.472−1.562−1.6−1.483−6.815−2.199−3.408
4.8−1.484−2.67−1.684−1.728−1.581−7.716−2.408−3.858
5.3−1.572−2.854−1.797−1.847−1.669−8.618−2.608−4.309
5.8−1.653−3.027−1.903−1.959−1.751−9.521−2.8−4.761
6.3−1.728−3.189−2.002−2.064−1.827−10.425−2.985−5.213
Table 5. MLE and Bayesian at λ = 0.5.
Table 5. MLE and Bayesian at λ = 0.5.
λ = 0.5 PointConfidanceRE
SRSRSS c = 1RSS c = 3SRSRSS c = 1RSS c = 3
δ n BiasMSEBiasMSEBiasMSELCICPLCICPLCICPRE1RE2RE3
MLE0.58 λ 0.08550.24430.02810.08980.02410.06741.910394.00%1.170895.20%1.005595.40%272%363%133%
δ 0.35270.44380.15230.13460.08590.09852.217597.20%1.309998.20%1.184897.40%330%450%137%
12 λ 0.04200.17520.02410.08890.02010.02801.634293.80%1.190497.00%0.651497.60%197%627%318%
δ 0.30560.35240.09750.08850.04710.05062.472097.40%1.102998.00%0.863497.60%398%696%175%
17 λ 0.02510.12860.03240.0514−0.00950.01871.404093.80%0.880896.00%0.535598.00%250%687%275%
δ 0.28120.30660.06710.07180.05290.03131.871897.40%1.017898.00%0.662397.40%427%980%229%
28 λ 0.18130.36900.02210.04680.01190.01162.274892.80%0.844396.80%0.419697.80%789%3188%404%
δ 0.17941.03040.06470.2270−0.00540.05923.920496.40%1.852393.20%0.954796.80%454%1740%383%
12 λ 0.16280.28730.02420.0456−0.00820.00162.004092.00%0.913395.40%0.158695.80%630%17,571%2788%
δ 0.08850.7759−0.00630.21980.02430.04183.438891.40%2.140994.40%0.796995.40%353%1855%525%
17 λ 0.10300.17480.02140.04110.00720.00161.589893.00%0.791198.60%0.539499.40%425%10,996%2586%
δ 0.06750.55260.00610.08590.01000.03362.904991.00%1.149696.80%0.718496.60%644%1644%255%
38 λ 0.13370.32230.00290.02090.00450.00552.165194.80%0.567699.00%0.290199.00%1540%5874%381%
δ 0.08770.85530.04940.1465−0.00410.03303.612692.20%1.489295.00%0.713197.20%584%2589%443%
12 λ 0.07930.12690.01420.0127−0.00160.00071.362895.40%0.439296.80%0.103396.40%997%18,240%1829%
δ 0.04120.9558−0.00080.12810.01670.03113.832992.80%2.079795.20%0.688698.20%746%3076%412%
17 λ 0.05640.09920.00240.0026−0.00100.00051.215795.80%0.200799.40%0.090797.40%3783%18,510%489%
δ 0.02300.44470.00390.04720.00620.01572.615393.20%0.852895.60%0.490696.40%941%2838%302%
Bayesian0.58 λ 0.10830.08410.05170.01590.05170.00150.913093.86%0.646598.57%0.252389.00%528%5498%1041%
δ 0.14450.14790.02760.01140.02760.00011.040892.29%0.678199.43%0.204282.57%1303%224,969%17272%
12 λ 0.08320.04560.02970.00430.02970.00070.818995.71%0.4811100.00%0.173190.29%1054%6853%650%
δ 0.11390.09020.01140.00320.01140.00000.961495.00%0.5228100.00%0.145186.71%2793%334,035%11959%
17 λ 0.06550.02960.01860.00220.01860.00030.750198.29%0.3906100.00%0.131491.80%1352%9137%676%
δ 0.08540.05770.00990.00160.00990.00000.876894.71%0.4388100.00%0.117286.00%3585%356,028%9930%
28 λ 0.07330.02920.01160.00310.01160.00110.749198.14%0.326499.29%0.165790.57%956%2773%290%
δ 0.07280.14860.00460.00100.00460.00002.869599.57%0.9168100.00%0.208699.71%14,194%632,266%4454%
12 λ 0.04580.01150.00270.00120.00270.00050.604399.57%0.2217100.00%0.111989.71%959%2347%245%
δ 0.04520.04400.00280.00040.00280.00002.2306100.00%0.6511100.00%0.1449100.00%10,682%276,372%2587%
17 λ 0.02920.00650.00340.00070.00340.00030.497499.71%0.164899.71%0.078889.00%992%2525%255%
δ 0.03290.02020.00120.00020.00120.00001.8829100.00%0.5275100.00%0.1164100.00%8281%141,788%1712%
38 λ 0.05690.01850.01220.00260.01220.00100.656798.71%0.293299.57%0.153887.71%704%1800%256%
δ 0.05990.07720.00350.00060.00350.00003.2656100.00%0.9224100.00%0.2064100.00%12,553%275,087%2191%
12 λ 0.03530.01030.00490.00130.00490.00040.515299.29%0.199499.86%0.104184.43%816%2291%281%
δ 0.03260.01900.00220.00020.00220.00002.4116100.00%0.6532100.00%0.1430100.00%8331%79,911%959%
17 λ 0.02270.00560.00120.00060.00120.00030.430099.43%0.1442100.00%0.073185.00%885%2252%255%
δ 0.01480.00980.00100.00020.00100.00001.9831100.00%0.5311100.00%0.1137100.00%5910%42,117%713%
Table 6. MLE and Bayesian at λ = 2.0.
Table 6. MLE and Bayesian at λ = 2.0.
λ = 2 PointConfidanceRE
SRSRSS c = 1RSS c = 3SRSRSS c = 1RSS c = 3
δ n BiasMSEBiasMSEBiasMSELCICPLCICPLCICPRE1RE2RE3
MLE0.58 λ −0.32281.3168−0.27690.5790−0.16960.41834.321196.20%2.781097.40%2.449297.20%227%315%138%
δ 0.78461.60610.35010.45040.22610.28003.905297.20%2.246695.20%1.877393.80%357%574%161%
12 λ −0.35331.1530−0.12010.4148−0.06590.14853.978896.80%2.483096.20%1.490194.00%278%776%279%
δ 0.67641.28640.17900.19090.09780.18913.572395.20%1.564095.40%1.662696.20%674%680%101%
17 λ −0.37750.9961−0.10370.2216−0.05930.13543.625397.00%1.801994.60%1.493294.40%449%736%164%
δ 0.62901.09580.10700.09430.08120.13253.283496.00%1.129494.40%2.187197.80%1162%827%71%
28 λ 0.21202.32710.14440.96700.12470.52755.926194.86%3.815892.71%2.806895.71%241%441%183%
δ 1.17414.66540.32961.11300.20550.87997.111998.86%3.931498.86%3.590498.29%419%530%126%
12 λ 0.13581.83380.08840.69920.04290.23915.285493.43%3.261893.43%1.910794.14%262%767%292%
δ 0.99463.53930.30761.01250.09670.33636.264498.29%4.137898.14%2.243296.43%350%1052%301%
17 λ 0.14971.38200.04070.42630.00930.18064.574094.71%2.556295.00%1.666595.00%324%765%236%
δ 0.67442.44890.22040.66740.09130.31565.539498.43%3.085997.00%2.282695.86%367%776%212%
38 λ 0.35852.40850.29251.21060.17770.62305.923393.00%4.160892.43%3.016792.71%199%387%194%
δ 0.86854.36510.12121.72430.13721.38967.454199.43%5.129299.00%4.592997.86%253%314%124%
12 λ 0.29742.22410.09360.51350.04780.16165.732791.57%2.787093.14%1.566095.71%433%1376%318%
δ 0.80934.07650.27411.37760.03740.42127.746198.43%4.476995.57%2.541895.00%296%968%327%
17 λ 0.29081.65590.11290.38770.02810.11144.917393.14%2.402292.29%1.304795.71%427%1486%348%
δ 0.55673.27660.11601.01420.04750.35226.756698.86%3.924396.00%2.320494.43%323%930%288%
Bayesian0.58 λ 0.02450.03990.01780.01060.01780.00571.9912100.00%1.3898100.00%0.705899.71%375%703%187%
δ 0.11440.06970.02620.00490.02620.00020.915796.71%0.5223100.00%0.183184.71%1422%44,461%3126%
12 λ 0.01370.01200.00720.00380.00720.00301.4957100.00%0.9943100.00%0.4938100.00%316%398%126%
δ 0.07370.03190.01310.00190.01310.00010.751697.86%0.3680100.00%0.129187.86%1716%43,486%2534%
17 λ 0.00600.00540.00110.00210.00110.00151.2491100.00%0.8081100.00%0.3874100.00%260%359%138%
δ 0.05050.01660.00900.00100.00900.00000.647498.86%0.2921100.00%0.103490.29%1657%39,855%2405%
28 λ 0.05250.03350.02160.01940.02160.00821.8112100.00%1.021699.86%0.550195.29%172%410%238%
δ 0.16250.14040.01020.00190.01020.00002.662699.86%0.8821100.00%0.207698.14%7545%439,806%5829%
12 λ 0.03410.01390.00590.00830.00590.00381.3486100.00%0.7071100.00%0.371896.14%166%363%218%
δ 0.09610.06150.00360.00070.00360.00002.0205100.00%0.6228100.00%0.143399.43%8775%280,496%3196%
17 λ 0.02350.00830.00640.00480.00640.00231.1121100.00%0.5422100.00%0.271994.43%174%357%206%
δ 0.06770.03290.00360.00040.00360.00001.6737100.00%0.5035100.00%0.114499.86%8102%188,280%2324%
38 λ 0.05250.03350.02160.01940.02160.00821.8112100.00%1.021699.86%0.550195.29%172%410%238%
δ 0.16250.14040.01020.00190.01020.00002.662699.86%0.8821100.00%0.207698.14%7545%439,806%5829%
12 λ 0.03410.01390.00590.00830.00590.00381.3486100.00%0.7071100.00%0.371896.14%166%363%218%
δ 0.09610.06150.00360.00070.00360.00002.0205100.00%0.6228100.00%0.143399.43%8775%280,496%3196%
17 λ 0.02350.00830.00640.00480.00640.00231.1121100.00%0.5422100.00%0.271994.43%174%357%206%
δ 0.06770.03290.00360.00040.00360.00001.6737100.00%0.5035100.00%0.114499.86%8102%188,280%2324%
Table 7. MLE and Bayesian at λ = 3.0.
Table 7. MLE and Bayesian at λ = 3.0.
λ = 3 PointConfidanceRE
SRSRSS c = 1RSS c = 3SRSRSS c = 1RSS c = 3
Methods δ n BiasMSEBiasMSEBiasMSELCICPLCICPLCICPRE1RE2RE3
MLE0.38 λ −0.51901.6445−0.09260.2282−0.03310.05464.600198.43%1.838695.14%0.907296.00%720%3013%418%
δ 0.49070.99700.03890.03460.01000.00413.411192.29%0.714098.00%0.249498.86%2878%24,059%836%
12 λ −0.37850.9832−0.03570.0950−0.03080.04793.595291.43%1.201094.29%1.095694.86%1035%2053%198%
δ 0.26850.44800.01650.01010.00630.00142.405092.14%0.389897.43%0.147095.43%4415%31,043%703%
17 λ −0.19410.5198−0.02800.0331−0.00900.00482.723891.86%0.705194.57%0.268197.71%1571%10939%696%
δ 0.13320.21350.00560.00110.00040.00031.735694.43%0.129795.71%0.068595.43%18,971%69,994%369%
0.58 λ −0.60232.7349−0.30430.8875−0.15340.54736.041998.14%3.497695.43%2.839094.14%308%500%162%
δ 0.92702.32890.27890.47700.11220.10484.755596.57%2.478692.00%1.191493.86%488%2221%455%
12 λ −0.53641.8947−0.12630.3544−0.04010.07474.972797.43%2.282194.71%1.060696.29%535%2536%474%
δ 0.64961.40600.08060.06950.01550.00873.891294.43%0.984697.00%0.360398.14%2023%16,212%801%
17 λ −0.44181.5273−0.16400.3172−0.03290.06724.527598.14%2.113492.14%1.008496.29%482%2274%472%
δ 0.47180.86820.07570.06020.01550.00733.151993.14%1.066095.86%0.630899.57%1443%11,957%829%
28 λ 0.02593.4728−0.03311.70280.04381.11197.309694.29%5.117395.29%4.133096.14%204%312%153%
δ 1.44846.01300.72502.39080.43861.58677.761999.43%5.357498.43%4.632096.43%252%379%151%
12 λ −0.02963.1821−0.00651.0169−0.02950.63576.996793.86%3.955894.29%3.125594.86%313%501%160%
δ 1.36665.53620.40861.10140.31010.94777.513598.71%3.791998.43%3.620096.43%503%584%116%
17 λ −0.04062.3864−0.12510.7429−0.02540.26376.057895.00%3.345396.14%2.011895.43%321%905%282%
δ 1.14294.74240.38260.91960.12640.27757.271797.86%3.849498.00%2.006196.00%516%1709%331%
Bayesian0.38 λ 0.00810.0231−0.00010.0062−0.00010.00252.1588100.00%1.5521100.00%0.8862100.00%375%936%249%
δ 0.06120.02010.02180.00300.02180.00030.522396.43%0.303299.57%0.138384.57%675%6813%1009%
12 λ 0.00310.0054−0.00130.0019−0.00130.00121.5645100.00%1.1041100.00%0.6220100.00%289%462%160%
δ 0.03720.00960.00560.00100.00560.00010.422897.14%0.205599.71%0.095687.29%924%7430%804%
17 λ 0.00170.0024−0.00200.0011−0.00200.00071.2878100.00%0.9026100.00%0.5028100.00%220%347%158%
δ 0.02940.00660.00530.00050.00530.00010.362398.43%0.1577100.00%0.074691.71%1379%7877%571%
0.58 λ −0.00110.02020.00540.00690.00540.00482.1389100.00%1.5040100.00%0.8219100.00%294%420%143%
δ 0.11230.05690.02270.00480.02270.00030.869297.00%0.4606100.00%0.174683.57%1194%22,408%1877%
12 λ 0.00150.0062−0.00020.0023−0.00020.00221.5528100.00%1.0743100.00%0.5750100.00%266%287%108%
δ 0.06380.02590.00990.00200.00990.00010.695797.29%0.3243100.00%0.121784.57%1322%23,434%1772%
17 λ 0.00340.00270.00190.00140.00190.00141.2806100.00%0.8677100.00%0.4551100.00%193%187%97%
δ 0.03840.01410.00770.00120.00770.00010.581798.43%0.2480100.00%0.096584.14%1132%20,160%1782%
28 λ 0.04140.02490.02850.01860.02850.00982.0417100.00%1.2539100.00%0.690399.57%133%253%190%
δ 0.13420.13540.01440.00270.01440.00002.516499.86%0.8586100.00%0.205496.29%5066%314,626%6211%
12 λ 0.02240.00940.01230.00870.01230.00441.4773100.00%0.8766100.00%0.470398.86%109%215%197%
δ 0.08910.06330.00670.00130.00670.00001.9433100.00%0.6057100.00%0.142095.71%4939%227,059%4597%
17 λ 0.01090.00530.00280.00520.00280.00251.2093100.00%0.6824100.00%0.353899.14%102%212%209%
δ 0.05230.03410.00250.00080.00250.00001.5961100.00%0.4880100.00%0.113096.57%4428%147,107%3322%
Table 8. MLE and different measures for KMPTL and comparative method: economic growth data.
Table 8. MLE and different measures for KMPTL and comparative method: economic growth data.
EstimatesSEKSDSM1SM2SM3SM4CVMAD
KMPTL λ 1.16720.77310.0568−24.8680−20.6462−24.6611−23.21350.04560.3864
δ 2.75322.6813
PTL λ 0.46010.40460.0569−24.8276−20.6059−24.6207−23.17310.04930.4091
δ 9.41773.8950
Betaa2.79400.48800.0618−23.9056−19.6838−23.6987−22.25100.04910.3867
b2.60370.4519
Kwa2.32890.30550.0689−23.2431−19.0213−23.0362−21.58860.05280.4009
b2.76240.5550
MOK α 0.29840.29740.0583−22.6334−16.3007−22.2123−20.15160.04920.4149
β 3.06320.6398
θ 1.94470.9469
UG α 0.61570.26600.1098−17.7512−13.5295−17.5443−16.09670.15861.1548
β 1.09270.2473
UL θ 0.72480.06870.248733.191835.302733.259634.01910.61533.7898
TL θ 2.73940.35070.0860−23.8362−20.2725−23.7684−23.00900.04590.3974
UGLBXII α 4.89117.09710.0569−22.9393−16.6067−22.5183−20.45750.04600.3947
β 0.97870.1834
λ 1.75291.7128
UEPD α 0.81170.06470.1670214.7548221.0874215.1758217.23660.34472.2041
β 1.30710.6696
λ 0.764141.1245
Table 9. MLE and different measures for KMPTL and comparative method: polyester fibers data.
Table 9. MLE and different measures for KMPTL and comparative method: polyester fibers data.
EstimatesSEKSDSM1SM2SM3SM4CVMAD
KMPTL λ 6.66391.58430.0624−2.8736−0.0712−2.4291−1.97710.01690.1450
δ 0.14780.2745
PTL λ 1.89492.38140.0718−2.09770.7047−1.6533−1.20120.02330.1955
δ 0.48950.7559
Betaa0.96660.22380.0669−2.61010.1923−2.1657−1.71360.01840.1559
b1.62050.4107
Kwa0.96220.20160.0649−2.62210.1803−2.1776−1.72560.01830.1550
b1.60770.4135
MOK α 0.43630.47070.0630−1.20872.9949−0.28560.13610.01710.1456
β 1.18690.3460
θ 1.25840.6442
UG α 1.03800.77020.0734−2.8098−0.0695−2.4053−1.90010.01840.1461
β 0.42120.1917
UL θ 1.05050.14550.272120.170421.571620.313320.61870.16561.0870
TL θ 1.10900.20250.0665−3.8078−2.4066−3.6649−3.35950.01890.1600
UGLBXII α 1167.4551810.12700.0658−1.43062.7730−0.5076−0.08590.01730.1457
β 0.68460.1003
λ 261.56421342.7096
UEPD α 0.66300.08820.105274.779078.982675.702176.12380.06370.4734
β 0.9585106.1478
λ 0.975171.5895
Table 10. Bayesian estimation.
Table 10. Bayesian estimation.
MeanSELowerUpper
Economic Growth λ 1.20550.25540.76431.7374
δ 2.79030.76581.37564.2750
polyester fibers λ 6.58532.07642.752510.6469
δ 0.17030.07260.05240.3178
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Alotaibi, N.; Al-Moisheer, A.S.; Elbatal, I.; Shrahili, M.; Elgarhy, M.; Almetwally, E.M. Bayesian and Non-Bayesian Estimation for a New Extension of Power Topp–Leone Distribution under Ranked Set Sampling with Applications. Axioms 2023, 12, 722. https://doi.org/10.3390/axioms12080722

AMA Style

Alotaibi N, Al-Moisheer AS, Elbatal I, Shrahili M, Elgarhy M, Almetwally EM. Bayesian and Non-Bayesian Estimation for a New Extension of Power Topp–Leone Distribution under Ranked Set Sampling with Applications. Axioms. 2023; 12(8):722. https://doi.org/10.3390/axioms12080722

Chicago/Turabian Style

Alotaibi, Naif, A. S. Al-Moisheer, Ibrahim Elbatal, Mansour Shrahili, Mohammed Elgarhy, and Ehab M. Almetwally. 2023. "Bayesian and Non-Bayesian Estimation for a New Extension of Power Topp–Leone Distribution under Ranked Set Sampling with Applications" Axioms 12, no. 8: 722. https://doi.org/10.3390/axioms12080722

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