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Original article
02 2022
:35;
102444
doi:
10.1016/j.jksus.2022.102444

Exponentiated odd Lindley-X family with fitting to reliability and medical data sets

Department of Mathematics, Faculty of Science, Tanta University, Tanta 31527, Egypt
Department of Statistics, Federal University of Pernambuco, Brazil

⁎Corresponding author. ahmed.abdelbar@science.tanta.edu.eg (Ahmed M. T. Abd El-Bar)

Disclaimer:
This article was originally published by Elsevier and was migrated to Scientific Scholar after the change of Publisher.

Peer review under responsibility of King Saud University.

Abstract

This paper concerns constructing a general family of distributions called exponentiated odd Lindley-X (EOL-X) family. We demonstrate that the EOL-X density can be represented as an infinite linear combination of the exponentiated-F densities and, as a result, that many of its mathematical features are derived directly. The fundamental statistical properties, including moments, mean deviations, generating function, order statistics, stochastic ordering, and entropies were investigated. EOL-X special models are introduced. The suggested model presents superior performance when compared to the other models studied, in the reliability and “medical” data. In addition, its bimodal density shape enhances the possibility of good tuning in applications in several other areas, such as survival. Thus, it is expected that this proposal will be of great help to the community studying new families and their adjustments to real data sets.

Keywords

Exponentiated odd Lindley
Moments
Medical data set
Reliability data set
Survival data set
1

1 Introduction

The most diverse distributions proposed in the literature are extremely important for understanding and modeling real data. Unfortunately, it has not yet been proposed a family of distributions that satisfactorily fits the phenomena studied in all areas of knowledge. For this reason, more and more researchers are dedicated to proposing new models that have a better fit in certain cases when compared to other models previously established in the literature. Over the decades, many families have been proposed. Below, we cite a few: Gleaton and Lynch (Gleaton and Lynch, 2006) proposed the generator odd-log-logistic-G; Alexander et al. (Alexander et al., 2012) developed the class Generalized Beta-Generated, among others.

More recently, some new families are proposed using the generator of families proposed by Alzaatreh et al. (Alzaatreh et al., 2013). For example, Ferreira (Ferreira, 2021), using this generator, proposed and studied the Quasi-Lindley-X family of distributions.

In addition, studies with combinations between transformations and this generator have also been carried out, such as the work done by Klakattawi et al. (Klakattawi et al., 2022), where the authors combine the Marshall-Olkin transformation with the T-X family of distributions.

Therefore, based on the knowledge that the Lindley distribution and its extensions have been shown to be quite adequate in modeling “medical” data sets, we seek to motivate the choice of the generator of families of T-X distributions, using the exponentiated odd Lindley, and we will see that this family can, depending on the baseline, embody at least three of the four important forms for the risk function, namely: increasing, decreasing and bathtub. This constitutes an important point of the family, since it allows a better suitability for different types of data set.

Recently, Alzaatreh et al. (Alzaatreh et al., 2013) have introduced the T-X family as

(1)
G x = 0 - log 1 - F x r t d t ,

Moreover, the exponentiated T-X family proposed by Alzaghal et al. (Alzghal et al., 2013). In addition, Gomes-Silva et al. (Gomes-Silva et al., 2017) described the odd Lindley-G family. In this work, we will develop some mathematical properties of one member of the exponentiated odd S-X family which is also a general family of distributions, namely the exponentiated odd Lindley-X (EOL-X) family and illustrate the versatility of the EOL-X family to fit and model real data. Various shapes of the hazard rate function (hrf) and density of sub-models for EOL-X family support the family to fit several real lifetime data which represent one of the motivations to the family beside others that will be mention through the paper, such as mixture representation of the density and cdf of the family in terms of exp-F distributions.

Next, we give some remarks and properties on the EOS-X family.

Remark 1

Replacing - log 1 - F x by F α x 1 - F α x in (1), we have the cdf of the EOS-X.

(2)
G x = 0 F α x 1 - F α x r s d s = Ψ F α x 1 - F α x ,
where α > 0 is an additional parameter and Ψ s is the cdf of S . As a result, the pdf of the family defined by (2) is
(3)
g x = α f x F α - 1 x 1 - F α x 2 r F α x 1 - F α x .

The hrf of the EOS-X is

(4)
h x = α f x F α - 1 x 1 - F α x 2 r F α x 1 - F α x 1 - Ψ F α x 1 - F α x - 1 .
Remark 2

Let X follows the EOS-X family (3), the associated quantile function Q u is.

(5)
X = Q u = F - 1 Ψ - 1 u Ψ - 1 u + 1 1 / α , 0 < u < 1 ,
where Ψ - 1 . and F - 1 . are inverses of the cdfs of S and X respectively.
Remark 3

Let X follows the EOS-X family with the pdf (3), then the Shannon entropy (SE) of X , ϖ x , is.

(6)
ϖ x = - log α - E log f F - 1 S S + 1 1 / α - α - 1 α E log S S + 1 + 2 E log 1 S + 1 + ϖ S ,
where ϖ S is the SE of S.

Note that, (2) and (3) do not involve any complicated functions. Thus, if we choose distributions with simple density for S, we will have a family of distributions with density and cumulative functions of easy mathematical and computational treatment, when compared with families such as gamma-G and beta-G, for example. Besides that, we can note that (3) provide distribution families generators, depend on the choice of S. In this way, this work ‘opens the doors’ to proposals of new distributions with density in the form (3). Here, we choose S L i n d l e y α , θ by the simplicity of its pdf.

To demonstrate the effectiveness of the proposed model, we study its fit to three real data sets. The first one address the failure time of turbochargers, components play an important role in the safe operation of merchant vessels, since they play a key role in the proper functioning of the main engine. This data is presented in application section. Some papers have been studied the use of some distributions through the adjustment of this data: Singla et. al. (Singla et al., 2012) show that the beta generalized Weibull model is preferable over its sub models using this data set and Benkhelifa (Benkhelifa, 2020) demonstrate the flexibility to the Weibull Birnbaum-Saunders distribution by means this data.

In order to show the flexibility of the proposal to different situations, we also include applications to survival data. In addition, we know that many of the families that are part of the S-X family are well suited to these types of sets. In this sense, the second data constitutes a survival data set, since each observation is the time to death (in months) of patients with breast cancer with different immuno-biochemical responses (for more details, see Klein and Moeschberger (Klein and Moeschberger, 2005).

It is important to study breast cancer data since this type of cancer is one of the most frequent in women around the world. It is the most common in women in the United States. In Brazil, it only loses to non-melanoma skin and accounts for 29 % of new cases each year, according to the National Cancer Institute.

The third data is a study about Aids clinical trial nested and can be found in https://www.umass.edu/statdata/statdata/stat-survival.html. Clinical studies with Aids data are of great relevance in the scientific and social aspects. Despite being a disease already known worldwide since the early 1980 s, there is still a lot of prejudice and, in some countries, lack of access to information and medicines.

Brazil has stood out, among other aspects, with programs for the distribution of condoms and antiretroviral drugs at no additional cost. Although programs like these have not eradicated such an epidemic, they help increase patient survival and quality of life. Much still needs to be done to heal healing, and statistical study is an important tool in this process.

The following is a list of the paper's supplements. We propose the exponentiated odd Lindley-X family and some of its sub-models, in Section 2. In Section 3, we show the mixture representation of the density and cdfs of the family. We provide various of the new family’s mathematical features in Section 4. Stochastic ordering and the two popular entropies are investigated in Sections 5 and 6, respectively. An estimation procedure for EOL-X parameters is obtained in Section 7. Simulation studies are provided in Section 8. We chose some data sets to evaluate the performance of sub-model of the family using a set of goodness-of-fit statistics in Section 9. Finally, some conclusions about the obtained results are reported in Section 10.

2

2 EOL-X family with sub-models

The EOL-X family is proposed in this section. Some sub-models of the family are given and it is observed that their pdfs could be unimodal, left-skewed, right-skewed, bimodal and their hrfs could be bathtub, decreasing, constant, increasing, J and reversed-J shaped. All this gains the family much flexibility for fitting and modeling real life data.

2.1

2.1 The EOL-X family

Let S follows the Lindley distribution with pdf r s = θ 2 θ + 1 1 + s e - θ s , then the pdf of the EOL-X family using (3) is

(7)
g x ; α , θ , ξ = α θ 2 θ + 1 f x ; ξ F α - 1 x ; ξ 1 - F α x ; ξ 3 exp - θ F α x ; ξ 1 - F α x ; ξ ,

where F x ; ξ = F x is a baseline cdf depending on a parameter vector ζ . By using (2) and the cdf of the Lindley distribution, Ψ s = 1 - θ + 1 + θ s θ + 1 e - θ s , The EOL-X family's cdf can be found here

(8)
G x ; α , θ , ξ = 1 - 1 + θ θ + 1 F α x 1 - F α x exp - θ F α x 1 - F α x .

Hence, the hrf of X is

(9)
h x ; α , θ , ξ = α θ 2 f x F α - 1 x θ + 1 - F α x 1 - F α x 2 .

2.2

2.2 Sub-models

Some sub-models in the EOL-X family (7) are given in function of three well-known distributions; exponential (E) with cdf F x ; λ = 1 - e - λ x , Lomax (Lo) with cdf defined as F x ; σ , λ = 1 - 1 + x / σ - λ and Dagum (Da) with cdf F x ; β , λ = 1 + x - λ - β . .

2.2.1

2.2.1 The EOL-E distribution

Using the exponential pdf and cdf as input for (7) and (9), we get the EOL-E pdf and hrf.

(10)
g x ; α , θ , λ = α λ θ 2 θ + 1 e - λ x 1 - e - λ x α - 1 1 - 1 - e - λ x α 3 exp - θ 1 - e - λ x α 1 - 1 - e - λ x α , x > 0 ; α , θ , λ > 0

and

(11)
h x ; α , θ , λ = α λ θ 2 1 - e - λ x α - 1 e - λ x θ + 1 - 1 - e - λ x α 1 - 1 - e - λ x α 2 ,

respectively. The pdf and hrf of EOL-E are plotted in Fig. 1 for distinct parameters values.

Plots of the EOL-E pdf and hrf. (a) α = 6 , θ = 4 , λ = 2 (black), α = 0.2 , θ = 3.9 , λ = 0.01 (red), α = 10 , θ = 2 , λ = 1.6 (green), α = 1 , θ = 1.5 , λ = 2 (blue), α = 0.5 , θ = 0.8 , λ = 1.5 (purple).(b) α = λ = 1 , θ = 3 (green), α = 0.01 , θ = λ = 0.1 (black), α = 0.1 , θ = 0.2 , λ = 1.5 (blue), α = 5 , θ = 1 , λ = 1.5 (red), α = 0.3 , θ = 0.2 , λ = 2 (Purple).
Fig. 1
Plots of the EOL-E pdf and hrf. (a) α = 6 , θ = 4 , λ = 2 (black), α = 0.2 , θ = 3.9 , λ = 0.01 (red), α = 10 , θ = 2 , λ = 1.6 (green), α = 1 , θ = 1.5 , λ = 2 (blue), α = 0.5 , θ = 0.8 , λ = 1.5 (purple).(b) α = λ = 1 , θ = 3 (green), α = 0.01 , θ = λ = 0.1 (black), α = 0.1 , θ = 0.2 , λ = 1.5 (blue), α = 5 , θ = 1 , λ = 1.5 (red), α = 0.3 , θ = 0.2 , λ = 2 (Purple).

2.2.2

2.2.2 The EOL-Lo distribution

Inserting the Lomax pdf and cdf as input for (7) and (9), implies the EOL-Lo pdf and hrf as

(12)
g x ; α , θ , λ , σ = α λ θ 2 σ θ + 1 1 + x / σ - λ + 1 1 - 1 + x / σ - λ α - 1 1 - 1 - 1 + x / σ - λ α 3 exp - θ 1 - 1 + x / σ - λ α 1 - 1 - 1 + x / σ - λ α
(13)
h x ; α , θ , λ , σ = α λ θ 2 σ 1 + x / σ - λ + 1 1 - 1 + x / σ - λ α - 1 θ + 1 - 1 - 1 + x / σ - λ α 1 - 1 - 1 + x / σ - λ α 2 , x > 0 ; α , θ , λ , σ > 0

respectively. Fig. 2 shows plots of the pdf and hrf of the EOL-Lo for the specified parameter values.

Plots of the EOL-Lo pdf and hrf. (c) α = λ = 0.5 , θ = 1 , σ = 3 (black), α = 10 , θ = 3 , λ = 7 , σ = 2 (red), α = 3 , θ = 4 , λ = σ = 2 (green), α = 1 , θ = λ = 3 , σ = 5 (purple), α = 0.3 , θ = 0.2 , λ = 2 , σ = 0.8 (blue)(d) α = θ = σ = 1 , λ = 2 (green), α = 0.3 , θ = 2 , λ = 0.5 , σ = 3 (black), α = σ = 2 , θ = 10 , λ = 1.5 (purple), α = λ = 1 , θ = 2 , σ = 3 (blue), α = 5 , θ = σ = 1 , λ = 3 (red),
Fig. 2
Plots of the EOL-Lo pdf and hrf. (c) α = λ = 0.5 , θ = 1 , σ = 3 (black), α = 10 , θ = 3 , λ = 7 , σ = 2 (red), α = 3 , θ = 4 , λ = σ = 2 (green), α = 1 , θ = λ = 3 , σ = 5 (purple), α = 0.3 , θ = 0.2 , λ = 2 , σ = 0.8 (blue)(d) α = θ = σ = 1 , λ = 2 (green), α = 0.3 , θ = 2 , λ = 0.5 , σ = 3 (black), α = σ = 2 , θ = 10 , λ = 1.5 (purple), α = λ = 1 , θ = 2 , σ = 3 (blue), α = 5 , θ = σ = 1 , λ = 3 (red),

2.2.3

2.2.3 The EOL-Da distribution

Taking the Dagum pdf and cdf as input for (7) and (9), the following functions hold

(14)
g x ; α , θ , λ , β = α λ β θ 2 θ + 1 x - λ - 1 1 + x - λ - α β - 1 1 - 1 + x - λ - β α 3 exp - θ 1 + x - λ - β α 1 - 1 + x - λ - β α ,

and

(15)
h x ; α , θ , λ , β = α λ β θ 2 1 + x - λ - β α + 1 x - ( λ + 1 ) θ + 1 - 1 + x - λ - β α 1 - 1 + x - λ - β α 2 .

The pdf and hrf curves of the EOL-Da model are displayed in Fig. 3.

Plots of the EOL-D pdf and hrf. (e) α = λ = 0.5 , θ = 1 , β = 3 (black), α = β = θ = 1 , λ = 5.5 (blue), ( α = 2 , θ = 1 , λ = 3 , β = 0.1 ) (red), ( α = 2 , θ = 1 , λ = 3 , β = 1.6 ) (green), α = λ = 2 , θ = 1 , β = 0.3 (pruple). (f) α = λ = 0.5 , θ = β = 1 (black), α = 0.3 , θ = β = 0.2 , λ = 2 (blue), α = 0.1 , θ = 3 , β = 2 , λ = 0.3 (green), α = θ = β = 1 , λ = 3 (red), ( α = 1 , θ = 3 , β = 0.9 , λ = 1.2 ) (purple).
Fig. 3
Plots of the EOL-D pdf and hrf. (e) α = λ = 0.5 , θ = 1 , β = 3 (black), α = β = θ = 1 , λ = 5.5 (blue), ( α = 2 , θ = 1 , λ = 3 , β = 0.1 ) (red), ( α = 2 , θ = 1 , λ = 3 , β = 1.6 ) (green), α = λ = 2 , θ = 1 , β = 0.3 (pruple). (f) α = λ = 0.5 , θ = β = 1 (black), α = 0.3 , θ = β = 0.2 , λ = 2 (blue), α = 0.1 , θ = 3 , β = 2 , λ = 0.3 (green), α = θ = β = 1 , λ = 3 (red), ( α = 1 , θ = 3 , β = 0.9 , λ = 1.2 ) (purple).

3

3 Expansions for the EOL-X family

This section displays a mixture representation of the EOL-X family's pdf and cdf. This family's quantile function is also provided.

3.1

3.1 Expansion for the dansity function

By making of the power series for the following term, we get

(16)
exp - θ F α x ; ξ 1 - F α x ; ξ = k = 0 - 1 k θ k k ! F α k x ; ξ 1 - F α x ; ξ k .

Applying (16) in (7), we have

(17)
g x ; α , θ , ξ = α θ 2 θ + 1 f x ; ξ k = 0 - 1 k θ k k ! F α k + 1 - 1 x ; ξ 1 - F α x ; ξ k + 3 .

We should use the generalized binomial theorem to find

(18)
1 - F α x ; ξ - ( k + 3 ) = m = 0 Γ k + 3 + m m ! Γ k + 3 F α m x ; ξ .

Inserting (18) in (17), the pdf (7) can be stated as

(19)
g x ; α , θ , ξ = m , k = 0 ω m , k r υ m , k x , where.

ω m , k = - 1 k α θ k + 2 Γ k + 3 + m θ + 1 k ! m ! Γ k + 3 α k + 1 + m , υ m , k = α k + 1 + m , and r b x = b f x F b - 1 x . .

Hence, the pdf of the EOL-X family can be expressed as an infinite linear combination of the exponentiated-F (exp-F) density. As a result, the exp-F distribution may be used to derive several mathematical features of EOL-X. Nadarajah and Kotz (Nadarajah and Kotz, 2006) investigate several mathematical features of exp-F distributions.

Then, the mixture representations of the cdf and hrf of EOL-X family are presented, respectively, as

(20)
G x ; α , θ , ξ = m , k = 0 ω m , k R υ m , k x ,

and h x ; α , θ , ξ = m , k = 0 ω m , k r υ m , k x 1 - m , k = 0 ω m , k R υ m , k x .

3.2

3.2 Quantile function

The quantile function, Q u , 0 < u < 1 , for the EOL-X family is obtained by using (6) and (8) as

(21)
Q u = F - 1 Ψ - 1 u Ψ - 1 u + 1 1 / α , where
(22)
Ψ - 1 u = - θ + 1 + W u - 1 θ + 1 exp - θ + 1 θ ,
where Ψ - 1 u is the inverse of cdf for Lindley and W . is Lambert function.

4

4 Mathematical properties

The mathematical properties of the distributions are important characteristics and must be obtained, whenever possible, in a closed form, that is, in function of known mathematical functions. However, we know that often proposing new distributions brings with it the problem of obtaining such properties in this format. Therefore, when we can express the density and distribution functions as a linear mixture of accumulated densities, respectively, of the exponential distributions-G, we use power series properties to obtain these results.

In this sence, we intrduced various mathematical features of the EOL-X family in this section, including moments, mean deviations, generating function, (reversed) residual lifetime moments and order statistics.

4.1

4.1 Moments

Using (19) and the definition of the nth moment about the origin of X , we have

(23)
E X n = m , k = 0 ω m , k E Z m , k n , where Z m , k is a random variable having an exp-F pdf r υ m , k x .

The baseline quantile function Q F x can be used as another formulation for E X n as follows:

Using (19), we can write E X n as

(24)
E X n = m , k = 0 υ m , k ω m , k ψ n , υ m , k , where ψ n , υ m , k = - x n F x υ m , k - 1 f x d x = 0 1 Q F u n u υ m , k - 1 d u .

Cordeiro and Nadarajah (Cordeiro and Nadarajah, 2011) obtained υ n , υ m , k for some well-known distributions which can be used to determine the EOL-X moments.

4.2

4.2 Incomplete moments

The nth incomplete moment of X is given by

(25)
m n y = E X n X < y = m , k = 0 υ m , k ω m , k 0 F y Q F u n u υ m , k - 1 d u , where Q F u is directly obtained from (21).

4.3

4.3 Moment generating function

The moment generating function (mgf) of the EOL-X family is presented two expressions here. The first one can be obtained from the Exp-F mgf as

(26)
M X t = m , k = 0 ω m , k Ξ υ m , k t , where Ξ υ m , k t is the mgf of random variable Z k , m . A second form for M X t can be obtained from (19) as
(27)
M X t = m , k = 0 υ m , k ω m , k φ t , υ m , k ,
where φ t , υ m , k = - e t x F x υ m , k - 1 f x d x = 0 1 exp t Q F u u υ m , k - 1 d u .

4.4

4.4 Mean deviations

The mean deviations about the mean ( γ 1 ) and about the median ( γ 2 ) of the EOL-X family can be obtained as.

(28)
γ 1 = 2 μ 1 ' G μ 1 ' - 2 m 1 μ 1 ' , a n d γ 2 = μ 1 ' - 2 m 1 M ,

respectively, where μ 1 = E . is obtained from (23), M = Q G Ψ - 1 0.5 Ψ - 1 0.5 + 1 1 / α is the median of X and Ψ - 1 0.5 is obtained from (21) and (22), G μ 1 is evaluated by the cdf of the EOL-X family and m 1 z is the first incomplete moment can be obtained from (19) as

(29)
m 1 z = m , k = 0 ω m , k J υ m , k z , where J υ m , k z = - z x r υ m , k x d x .

4.5

4.5 Moments of residual and reversed residual lifetime

The moments of residual and reversed residual lifetime of the EOL-X family are given by

(30)
κ t = 1 S t E X n - 0 t x n g x d x - t = 1 S t E X n - m n t - t , t 0

and

(31)
ϕ t = t - 1 G t 0 t x n g x d x = t - 1 G t m n t , t 0

respectively, where G . and S . are the cdf and survival function of the EOL-X family, E X n given by (23), and m n t is the nth incomplete moment given by (25).

4.6

4.6 Order statistics

The pdf of the ith order statistic, say X i : n , for a random sample X 1 , X 2 , . . . , X n from the EOL-X family is given by

(32)
g i : n x = n ! i - 1 ! n - i ! g x G i - 1 x 1 - G x n - i .

Inserting (7) and (8) into (32), the g i : n x becomes

(33)
g i : n x = m = 0 i - 1 ω m g x ; α , θ m + n - i + 1 1 + θ θ + 1 F α x 1 - F α x n + m - i , where ω m = n ! n + m - i + 1 i - 1 ! n - i ! - 1 m i - 1 m

and g x ; α , θ n + m - i + 1 denotes the EOL-X pdf with parameters α and θ n + m - i + 1 .

5

5 Stochastic ordering

The EOL-X family is ordered in terms of likelihood ratio ordering, as shown by the next theorem.

Theorem 1

Let X EOL-X α , θ 1 , ξ and Y EOL-X α , θ 2 , ξ . If θ 2 < θ 1 , then X is stated to be smaller than Y in the likelihood ratio order (denoted by X lr Y ).

Proof. The likelihood ratio is given by g X x g Y x = θ 1 θ 1 + 1 θ 2 + 1 θ 2 E x p - θ 1 F α x ; ξ 1 - F α x ; ξ E x p θ 2 F α x ; ξ 1 - F α x ; ξ .

Since θ 2 < θ 1 , d dx log g X x g Y x = θ 2 - θ 1 α f x ; ξ F α - 1 x ; ξ 1 - F α x ; ξ 2 < 0

Hence g X x g Y x is decreasing in X . That is X lr Y , which completes the proof.

6

6 Entropies

Here, we discuss two common entropy measures that are the Shannon entropy and Rényi entropy. In what follows, we derive two entropies of the EOL-X family.

Theorem 2

The EOL- family's Shannon entropy (SE) is given by.

ϖ x = - log α - E log f F - 1 S S + 1 1 / α - α - 1 α E log S S + 1 + 2 E log 1 S + 1 + l o g θ - θ + 2 - exp θ θ + 1 Γ γ + 1 , θ γ γ γ = 1 .

Proof. The proof follows from Remark 4 and the SE for the Lindley distribution:

ϖ S = l o g θ - θ + 2 - exp θ θ + 1 Γ γ + 1 , θ γ γ γ = 1 , which is given by Ghitany et al. (Ghitany et al., 2008).

Theorem 3

The EOL- family's Rényi entropy is described by

ψ R γ = 1 1 - γ log j , k = 0 Ω j , k - f γ x ; ξ F α j + k + γ - γ x ; ξ d x ,

where the coefficients Ω j , k = α γ γ j θ j + 2 γ θ + 1 γ - 1 j j ! 3 γ + j + k - 1 k . .

Proof. Using the definition of Rényi entropy and the pdf (7), hence - g γ x ; α , θ , ξ d x = α θ 2 θ + 1 γ - f γ x ; ξ F γ α - 1 x ; ξ 1 - F α x ; ξ 3 γ exp - θ γ F α x ; ξ 1 - F α x ; ξ d x .

Applying (16) in the expression above, we have - g γ x ; α , θ , ξ d x = j = 0 α γ γ j θ j + 2 γ θ + 1 γ - 1 j j ! - f γ x ; ξ F γ α - 1 + α j x ; ξ 1 - F α x ; ξ 3 γ + j d x .

Therefore, desired proof is obtained by expanding the binomial term in the integral above.

7

7 Inference on the EOL-X family parameters

An estimation procedure for EOL-X parameters are discussed here.

Let x 1 , x 2 , . . . , x n be observed values from the EOL-X defined by (7) with parameter vector Θ = α , θ , ξ T . Then, the log-likelihood function = ( Θ ) for Θ is = n log θ 2 θ + 1 + n l o g α + i = 1 n log f x i ; ξ + α - 1 i = 1 n log F x i ; ξ - 3 i = 1 n log 1 - F α x i ; ξ - θ i = 1 n F α x i ; ξ 1 - F α x i ; ξ .

The elements of the score vector are α = n α + i = 1 n log F x i ; ξ + 3 i = 1 n F α x i ; ξ log F x i ; ξ 1 - F α x i ; ξ - θ i = 1 n F 2 α x i ; ξ log F x i ; ξ 1 - F α x i ; ξ 2 + F α x i ; ξ log F x i ; ξ 1 - F α x i ; ξ , θ = - 2 n θ 3 - n 1 + θ 2 - i = 1 n F α x i ; ξ 1 - F α x i ; ξ ,

and ζ k = i = 1 n f k x i ; ξ f x i ; ξ + α - 1 i = 1 n F k x i ; ξ F x i ; ξ + 3 α i = 1 n F α - 1 x i ; ξ F k x i ; ξ 1 - F α x i ; ξ - α θ i = 1 n F α - 1 x i ; ξ F k x i ; ξ 1 - F α x i ; ξ 2 , where k = 1 , 2 , . . . , p . Equating α , θ and ξ k with zero, as well as numerically solving these equations, then the MLEs Θ = α , θ , ξ T of Θ = α , θ , ξ T are obtained.

8

8 Simulation study

Here, we present a simulation analysis to demonstrate the MLEs parameters vector's asymptotic behavior. To do this, we choose the sub-model EOLE, defined in (10). Using the R software, we execute a Monte Carlo simulation study, with 1000 replications. Setting α = 1 , θ = 2 and λ = 3 , The MLEs' accuracy is measured. Aside from that, we use the random censoring system on the right to censor percentages ( 0 % , 10 % and 20 % ) and n = 50 , 100 , and 150 . As a result, we present the MLEs' average estimates (AEs) as well as the mean squared errors (MSEs), for each parameter point. The results in Table 1 show that the sufficiency condition is valid and that the estimators are consistent.

Table 1 Simulations for the EOL-E.
0 % c e n s o r e d 10 % c e n s o r e d 20 % c e n s o r e d
n Parameter AE MSE AE MSE AE MSE
α 1.002 0.007 1.091 0.017 1.078 0.014
50 θ 2.030 0.054 1.828 0.074 1.850 0.066
λ 3.048 0.007 2.764 0.122 2.798 0.105
α 1.002 0.003 1.097 0.014 1.079 0.010
100 θ 2.008 0.027 1.800 0.059 1.842 0.046
λ 3.016 0.039 2.724 0.105 2.789 0.075
α 1.007 0.002 1.086 0.010 1.073 0.007
150 θ 2.009 0.017 1.815 0.048 1.848 0.036
λ 3.016 0.025 2.746 0.084 2.793 0.062

9

9 Applications to modeling reliability and medical data

Here, we compare the performance of the EOLE model at Subsection 2.2 to a set of classical and recent lifetime distributions.

The lifetime distributions used in comparison are:

For comparison purposes, we consider some real data sets in many areas. The main aim here is to show that our proposed model fits well several types of data. The first piece of data reflects the time it takes for a turbocharger to fail (103h), see Xu et al. (Xu et al., 2003). The second one lists the time to death (in months) of patients with breast cancer with different immuno-bistochemical responses (for more details, see Klein and Moeschberger (Klein and Moeschberger, 2005). In this case, we consider all the observations as uncensored observation. The third data is a study about aids clinical trial nested. For each distribution, we get the maximum-likelihood estimate, AIC, BIC, HQIC, W* and A* goodness-of-fit statistics. To do this, we use the function goodness.fit from software R, with the SANN method. Besides that, the initial kicks were obtained through a heuristic method with the GenSA. Table 2 gives some descriptive statistics for all data sets. The first data is left skewed and while the rest of the data sets are right skewed. The obtained results are presented in Tables 3-8. We developed different situations depend on each application. As we can see the EOLE is powerful competitor to the compared distributions. Moreover, the least values for the considered goodness-of-fit statistics are achieved for EOLE model. The EOLE model performed the best, as predicted from the previous findings.

Table 2 Descriptive statistics of all data sets.
Real data sets
Statistics Data1 Data 2 Data 3
Mean 6.2525 97.02 234.7
Median 6.5 87.5 265
SD 1.95553 51.679 93.854
MD-Mean 1.58723 45.70 78.282
MD-Median 4.73251 46.613 72.278
Kurtosis − 0.42501 −1.4923 −0.28969
Skewness − 0.65422 0.03268 0.898730
Table 3 Parameter estimates for the first data.
Model Parameter estimates
α θ λ
EOLE 3.2056 0.32662 0.42819
BE 7.87221 6.22419 0.13779
TEE 7.59178 0.31855 0.98999
GEE 10.5505 0.10895 8.11926
Ga 7.72269 0.809627
LE 10.3036 0.448709
α β a b λ
GTLo 2749.69 6107.18 9.52379 0.000025 0.318372
GDa 4.16258 0.50276 10.0245 10.116 1.64758
TELo 10.3998 17.4909 0.0332954 −0.63111
Table 4 Statistics for the first data.
Model W* A* AIC BIC HQIC
EOLE 0.108498 0.36417 166.663 171.73 168.495
Ga 0.209882 1.3834 178.821 182.198 180.042
LE 0.286773 1.8008 184.47 187.848 185.691
TEE 0.218098 1.43834 182.226 187.292 184.058
BE 0.214219 1.41121 181.387 186.454 183.219
GEE 0.221483 1.4507 181.352 186.752 183.517
TELo 0.232215 1.59486 187.744 194.499 190.186
GTLo 0.28377 1.78423 190.3 198.744 193.353
GD 0.701105 3.71635 207.196 215.64 210.249
Table 5 MLE’s (their standard error) for the second data.
Model Parameter estimates
α θ λ
EOLE 1.76770 (0.43848) 1.26683 (0.196734) 0.01077 (0.00166)
TEE 0.02017 (0.00314) 2.91307 (0.89602) − 0.28051 (0.1745)
EL 1.51417 (0.26956) 0.027508 (0.01339) 1.06001 (0.19539)
MW 1.979 (8.878 e-04) 1000 (5.606 e-02) 7.90e-02 (1.19e-02)
GL 1.60462 (0.37948) 0.029136 (0.00590)
LE 3.80833 (0.84147) 0.018864 (0.00300)
Ga 2.92634 (0.58952) 0.030165 (0.006621)
α β a b
GBGL 2.108e-01 (1.22e-04) 3.50 (1.186e-01) 6.81e-02 (1.025e-02) 4.41(3.3e-04)
Table 6 Statistics for the second application.
Model W A AIC BIC HQIC
EOLE 0.183436 1.022546 470.5342 475.886 472.5192
TEE 0.269836 1.701178 654.1809 659.533 656.1659
EL 0.255858 1.615608 557.669 563.022 559.6546
GL 0.207078 1.250375 473.8735 477.441 475.1968
LE 0.213885 1.310178 475.1699 478.738 476.4932
Ga 0.206380 1.244549 473.7209 477.289 475.0442
GBGL 0.209680 1.270334 478.3606 485.497 481.0073
MW 0.195096 1.126919 473.0868 478.439 475.0717
Table 7 MLE’s (their standard error) for the third data.
Model Parameter estimates
α θ λ
EOLE 2.56233 (0.14177) 5.03795 (0.53734) 0.002812 (0.00011)
TEE 0.00859 (0.00031) 2.43428 (0.17779) − 0.69730 (0.04102)
EL 1.11825 (0.04300) 0.00956 (0.00064) 0.94001 (0.02197)
GL 1.50407 (0.09379) 0.011478 (0.00061)
LE 7.99877 (0.63588) 0.011179 (0.00045)
Ga 2.95143 (0.16142) 0.012589 (0.00071)
Table 8 Statistics for the third application.
Model W A AIC BIC HQIC
EOLE 5.99974 33.17757 7022.502 7035.57 7027.598
TEE 12.74718 67.79268 11599.84 11612.8 11604.9
EL 7.534813 41.42356 7200.168 7213.23 7205.264
GL 7.980831 43.6366 7161.384 7170.09 7164.782
LE 9.525479 51.5472 7515.95 7524.662 7519.348
Ga 7.93374 43.34001 7158.165 7166.877 7161.562

Also, Fig. 4 shows the TTT plots for all data sets considered here. These plots indicate an increasing hrf (first, second and third data sets) and then reveal the adequacy of the some sub-models of our family to fit these data.

TTT plot for: (a) the first data, (b) second data (c) third data.
Fig. 4
TTT plot for: (a) the first data, (b) second data (c) third data.

Finally, we can conclude that the model studied in this section (using the exponential as a baseline) presents superior performance when compared to the competitive models chosen in the three applications in question. In addition, it is worth mentioning that in the applications studied, the proposed model also presented a better fit when compared to the gamma model.

10

10 Conclusions

We introduced a new distributions family from the T-X termed exponentiated odd Lindley – X (EOL-X) in this study. A linear representation of the new family's density function makes it simple to determine some of its properties. We developed a mathematical treatment of some sub-models of EOL-X. Besides that, several of their mathematical properties are derived. A simulation study based on the exponentiated odd Lindley exponential was provided. Finally, applications of sub-model of the potential family to three real data evidencing that the EOL-X routinely outperforms other well-known models in the literature. We hope that this research will be useful in a number of areas and that further research will emerge. As future works, the proposed distribution might also be investigated as a bivariate extension, which would likely be a discrete case. Finally, given our suggested model, we may do regression analysis.

Declaration of Competing Interest

The authors declare that they have no known competing financial interests or personal relationships that could have appeared to influence the work reported in this paper.

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