Type Ii Half Logisitic Exponentiated Lomax Distribution

Type Ii Half Logisitic Exponentiated Lomax Distribution

Article Fingerprint

ReserarchID

4SV4N

Type Ii Half Logisitic Exponentiated Lomax Distribution Banner

Key Research Insights

Synthesized scholarly intelligence & interactive research assistant
  • English
  • Afrikaans
  • Albanian
  • Amharic
  • Arabic
  • Armenian
  • Azerbaijani
  • Basque
  • Belarusian
  • Bengali
  • Bosnian
  • Bulgarian
  • Catalan
  • Cebuano
  • Chichewa
  • Chinese (Simplified)
  • Chinese (Traditional)
  • Corsican
  • Croatian
  • Czech
  • Danish
  • Dutch
  • Esperanto
  • Estonian
  • Filipino
  • Finnish
  • French
  • Frisian
  • Galician
  • Georgian
  • German
  • Greek
  • Gujarati
  • Haitian Creole
  • Hausa
  • Hawaiian
  • Hebrew
  • Hindi
  • Hmong
  • Hungarian
  • Icelandic
  • Igbo
  • Indonesian
  • Irish
  • Italian
  • Japanese
  • Javanese
  • Kannada
  • Kazakh
  • Khmer
  • Korean
  • Kurdish (Kurmanji)
  • Kyrgyz
  • Lao
  • Latin
  • Latvian
  • Lithuanian
  • Luxembourgish
  • Macedonian
  • Malagasy
  • Malay
  • Malayalam
  • Maltese
  • Maori
  • Marathi
  • Mongolian
  • Myanmar (Burmese)
  • Nepali
  • Norwegian
  • Pashto
  • Persian
  • Polish
  • Portuguese
  • Punjabi
  • Romanian
  • Russian
  • Samoan
  • Scots Gaelic
  • Serbian
  • Sesotho
  • Shona
  • Sindhi
  • Sinhala
  • Slovak
  • Slovenian
  • Somali
  • Spanish
  • Sundanese
  • Swahili
  • Swedish
  • Tajik
  • Tamil
  • Telugu
  • Thai
  • Turkish
  • Ukrainian
  • Urdu
  • Uzbek
  • Vietnamese
  • Welsh
  • Xhosa
  • Yiddish
  • Yoruba
  • Zulu
Reading Preferences
Font Size
Line Spacing
Background
This converted HTML version may contain rendering inconsistencies. Please refer to the PDF for the authoritative version, or click here to provide feedback.

Abstract

In this paper, we introduces a new distribution called Type II half logistic exponentiated lomax (TIIHLEE) distribution established from Type II half logistic G family of distribution We investigate some of its mathematical and statistical properties such as the explicit form of the ordinary moments, moment generating function, conditional moments, mean deviations, residual life and Renyi entropy. The maximum likelihood method is used to estimate the model parameters. Simulation studies were conducted to assess the finite sample behavior of the maximum likelihood estimators. Finally, we illustrate the importance and applicability of the model by the study of two real data sets.

I. INTRODUCTION

Lomax distribution can also be called Pareto Type II distribution and its application can be found in many fields like actuarial science, economics, and so on Al-Zahrani and Al-Sobhi (2013). The distribution was defined by Lomax (1954) and it is a heavy-tailed distribution. It has also been considered to be useful in reliability and life testing problems in engineering and in survival analysis as an alternative distribution Kilany (2016), Hassan and Al-Ghamdi (2009).

Modified and extended versions of the Lomax distribution have been studied; examples include the weighted Lomax distribution by Kilany (2016), exponential Lomax distribution by El-Bassiouny et al (2015), exponentiated Lomax distribution by Salem (2014), gamma Lomax distribution Cordeiro et al (2015), transmuted Lomax distribution by Ashour and Eltehiwy (2013), Poisson Lomax distribution by Al-Zahrani and Sagor (2014), McDonald Lomax distribution by Lemonte and Cordeiro (2013), Weibull Lomax distribution by Tahir et al (2015), and power Lomax distribution [12]. Besides, estimation of the parameters of Lomax distribution under general progressive censoring has also been considered by Al-Zahrani and Al-Sobhi by Al-Zahrani and Al-Sobhi (2013).

The half logistic distribution is a member of the family of logistic distributions which is introduced by (Balakrishnan, 1985) which has the following cumulative distribution function (CDF)

F(t)=1−eλt1+eλtt>0,λ>0.
(2)f(t)=2e−λt(1+eλt)2t>0,λ>0

Hassan et al. (2017) use the half logistic generator instead of the gamma generator to obtain type II half logistic family, which is denoted by TIIHL-G. Then the CDF and pdf of TIIHL-G is defined as follows

Notes

(3)F(x;λ)=1−∫0−log⁡G(x)2λe−λ(1+e−λt)2dt=2[G(x)]λ1+[G(x)]λx>0,λ>0
(4)f(x;λ)=2λg(x)[G(x)]λ−1[1+[G(x)]λ]2x>0,λ>0

Where λ is the shape parameter and g(x;λ), and G(x;λ) is the baseline distribution, respectively.

However, the TIIHLEE has tractable properties, especially for simulation, since its quantile function takes a simple form.

(5)Q(u)=G−1[u2−u]1λ

Where u is a uniform distribution on the interval (0,1) and G1 (.) is the inverse function of G(⋅)

Our aim in this work is to study a modified statistical distribution that will be suitable to fit positively skewed and unimodal data and to check the flexibility of the existing and proposed distribution.

II. TYPE II HALF LOGISTIC EXPONENTIATED LOMAX DISTRIBUTION

The cumulative density function (CDF) and probability density function (pdf) of exponentiated Lomax distribution (EE) are defined as follows:

(6)G(x)=(1−(1+βx)−θ)α
(7)g(x)=αβθ(1−(1+βx)−θ)α−1(1+βx)−(θ+1)

Substituting 6 and 7 in 4 and 3 then we define probability density function (pdf) and cumulative density function (CDF) Type II Half Logistic Exponentiated Lomax Distribution (TIIHLEL) as follows:

(8)f(x;α,β,λ,θ)=2αβλθ[1−(1+βx)−θ]α−1(1+βx)−(θ+1)[[1−(1+βx)−θ]α]λ−1[1+[[1−(1+βx)−θ]α]λ]2
(9)F(x;α,β,λ,θ)=2[[1−(1+βx)−θ]α]λ1+[[1−(1+βx)−θ]α]λ

Henceforth, a random variable with probability density function (pdf) is denoted by X∼TIIHLEL(α,β,λ,θ)

Notes

a) Hazard Function of TIIHLEL

(10)h(x;α,β,λ,θ)=f(x)F(x)=2λg(x)[G(x)]λ−11−[G(x)]2λ=2αβλθ(1−(1+βx)−θ)α−1(1+βx)−(θ+1)[(1−(1+βx)θ)α]λ−1(1−((1−(1+βx)θ)α)2λ)

b) Survival Function of TIIHLEL

F―(x;α,β,λ,θ)=1−F(x;α,β,λ,θ)
(11)=1−[1−[G(x;α,β,λ,θ)]λ1+[G(x;α,β,λ,θ)]λ]=1−[1−((1−(1+βx)−θ)α)λ1+((1−(1+βx)−θ)α)λ]

Plots of the density function (8) can be represented through Fig. 1. As it seems from Fig. 1 that the pdf of TIIHLEL can take different shapes according to different values of θ and λ. It can be symmetric, right-skewed, unimodal

Figure 1: Plot of the Density function of TIIHLEL
Figure 1: Plot of the Density function of TIIHLEL

Plots of cumulative distribution function (9) for the TIIHLEL distribution are displayed in Fig. 2. The CDF graph tends to move at a constant value from 0 to 1 on the x-axis before projecting to one on the y-axis

Figure 2: Plot of the Distribution function (CDF) of TIIHLEL
Figure 2: Plot of the Distribution function (CDF) of TIIHLEL

Plots of hazard function (10) for the TIIHLEL distribution are displayed in Fig. 3 It was examined from Fig. 3 show that the shape of the h(x) of the TIIHLEL shows the hazard functions can be constant, increasing or decreases, depending on the shape and scale parameters.

Figure 3: Plot of the Hazard function of TIIHLEL
Figure 3: Plot of the Hazard function of TIIHLEL

Plots of survival function (11) for the TIIHLEL distribution are displayed in Fig. 4. It was deduced from Fig. 4 that the shape parameters have a strong effect on the survival plot. A decrease in the shape parameter tends to reduce the movement of the line on the y-axis, and no plot is exceeding the benchmark of 1

Figure 4: Plot of the Survival function of TIIHLEL
Figure 4: Plot of the Survival function of TIIHLEL

c) Some Special case of TIIHLEL

  1. Whenα=1, the TIIHLEL model reduces to Type II half Logistic Lomax (TIIHLL) model withλandθas shape parameters andβas a scale parameter.
f(x;β,λ,θ)=2βλθ(1+βx)−(θ+1)[1−(1+βx)−θ]λ−1[1+[1−(1+βx)−θ]λ]2

Notes

  1. Whenβ=1, the TIIHLEL model reduces to Type II half Logistic Exponentiated Pareto (TIIHLEP) model withλ,θ, andαas shape parameters.
f(x;α,λ,θ)=2αλθ[1−(1+x)−θ]α−1(1+x)−(θ+1)[[1−(1+x)−θ]α]λ−1[1+[[1−(1+x)−θ]α]λ]2
  1. When λ=1, the TIIHLEL model reduces to Half Logistic Exponentiated Lomax (HLEL) model with α and θ are shape parameters λ is scale parameter.
f(x;α,β,θ)=2αβθ[1−(1+βx)−θ]α−1(1+βx)−(θ+1)[1+[(1−(1+βx)−θ]α]2
  1. Whenα=β=1, the TIIHLEL model reduces to Type II Half Logistic Pareto (TIIHLP) model withλandθas shape parameters.
f(x;λ,θ)=2λθ(1+x)−(θ+1)[(1+x)−θ]λ−1[1+[1−(1+x)−θ]λ]2
  1. When α=λ=1, the TIIHLEL model reduces to Half Logistic Lomax (HLL) model with λ and θ and α are shape parameters.
f(x;β,θ)=2βθ(1+βx)−(θ+1)[1+[1−(1+βx)−θ]]2
  1. Whenα=λ=β=1, the TIIHLEL model reduces to Half Logistic Pareto (HLP) model withθas a scale parameter.
f(x;β,θ)=2θ(1+x)−(θ+1)[1+[1−(1+x)−θ]]2
Table 1: Summary of Sub-Models from the TIHLEL distribution
Distributionαβλθ
TIIHLL1βλθ
TIIHLEPα1λθ
HLELαβ1θ
TIIHLP11λθ
HLL1β1θ
TIIHLEL111θ

Table 1 depict some existing model obtained when some parameters of the proposed distribution are relaxed.

III. MATHEMATICAL PROPERTIES FOR TIIHLEL

a) Infinite Linear Combination

f(x)=2λαβθ(1−(1+βx)−θ)α−1(1+βx)−(θ+1)(1−(1+βx)−θ)α(λ−1)×((1+1−(1+βx)−θ)αλ)−2f(x)=2λαβθ(1−(1+βx)−θ)αλ−1(1+βx)−(θ+1)((1+1−(1+βx)−θ)αλ)−2

Let v=λa

Notes

f(x)=2vβθ(1−(1+βx)−θ)v−1(1+βx)−(θ+1)((1+1−(1+βx)−θ)v)−2=2vβθ∑k=0∞(−1)kΓ(v)Γ(v−k)k!(1+βx)−θk−θ−1∑w=0∞(−2w)(wvi)(−1)i(1+βx)−θi=2vβθ∑k=0∞∑w=0∞∑i=0∞(−1)k+iΓ(v)(v−k)k!(−2w)(wvi)(1+βx)−θk−θi−θ−1
f(x)=2vθ∑k=0∞∑w=0∞∑i=0∞(−1)k+iΓ(v)(v−k)k!(−2w)(wvi)β(1+βx)−θk−θi−θ−1

Let

φi,k,w=2vθ∑k=0∞∑w=0∞∑i=0∞(−1)k+iΓ(v)(v−k)k!(−2w)(wvi)
f(x)=φi,k,wβ(1+βx)−θk−θi−θ−1

b) Moment of Proposed TIIHLEL Distribution

It is imperative to derive the moments when a new distribution is proposed. They play a significant role in statistical analysis, particularly in applications. Moments are used in computing measures of central tendency, dispersion, and shapes, among others.

Suppose the rth moment for the TIIIHL-G family is derived.

(13)E(Xr)=μr=∫0∞xrf(x)dx=∫0∞xrϕi,k,wβ(1+βx)−θk−θi−θ−1dx=ϕi,k,w∫0∞xrβ(1+βx)−(θk+θi+θ+1)dx

Let

βx=ax=aβdx=daβ
=ϕi,k,wβ∫0∞(aβ)r(1+a)−(θk+θi+θ+1)daβ=ϕi,k,wβ−rβ∫0∞ar(1+a)−(θk+θi+θ+1)da

Notes

(14)∫0∞Zx−1(1+Z)x+ydz=B(x,y)

Beta function is given

(15)x−1=rx=r+1x+y=θk+θi+θ+1

Therefore y=θk+θi+θ−r

Comparing 3.79 and 3.80 we have

μ1r=ϕi,k,wβ−r+1∫0∞ar(1+a)−(θk+θi+θ+1)da=ϕi,k,wβ−r+1B(r+1,θk+θi+θ−r)
(16)μ1r=ϕi,k,wβ−r+1B(r+1,θk+θi+θ−r)

The mean of the proposed TIIHLEL distribution is gotten by making μr moment equal to one (—r=1)

(17)μ11=ϕi,k,wB(2,θk+θi+θ−1)

When r=2

(18)μ12=ϕi,k,wβ−1B(3,θk+θi+θ−2)

When r=3

(19)μ13=ϕi,k,wβ−2B(4,θk+θi+θ−3)

Whenr=4

(20)μ14=ϕi,k,wβ−3B(4,θk+θi+θ−4)

The variance of TIIHLEL is obtained.

(21)var⁡(x)=σ2=E(x2)−[E(x)]2=μj2−(μj1)2

Substituting equation 17 and 18 into 21 to obtain the variance of TIIHLEL

(22)σ2=ϕi,k,wβ−1B(3,θk+θi+θ−2)−(ϕi,k,wB(2,θk+θi+θ−1))2

Standard Deviation of TIIHLEL

σ=Std(x)=Var(x)
(23)σ=ϕi,k,wβ−1B(3,θk+θi+θ−2)−(ϕi,k,wB(2,θk+θi+θ−1))2

Coefficient of Variation of TIIHLE (Theta)

CV=Stan⁡dard deviation (x)E(x)
(24)CV=ϕi,k,wβ−1B(3,θk+θi+θ−2)−(ϕi,k,wB(2,θk+θi+θ−1))2ϕi,k,wB(2,θk+θi+θ−1)

c) Moment Generating Function of TIIHLEE Distribution

A random variable x with pdf f(x) is defined as a

Mx(t)=E(etx)
E(etx)=∫0∞etxf(x)dx
=∑r=0∞trr!μr1(x)
Mx(t)=∑r=0∞trr!ϕi,k,wβ−r+1B(r+1,θk+θi+θ−r)

d) Incomplete Moment

The incomplete moment plays an important role in computing the mean deviation, median deviation.

The rth incomplete moment of the TIIHLEL is given by

vs(t)=∫0∞xsf(x)dx
(26)=2vθ∑k=0∞∑w=0∞∑i=0∞(−1)k+iΓ(v)(v−k)k!(−2w)(wvi)β−r+1B(r+1,θk+θi+θ−r)

Where B(..) is the incomplete beta function and r=1,2,3.....

 IV. MEAN DEVIATION 

The variation in a population can be measured to some degree by the totality of deviations from the mean and the median. If the random variable X follows the TIIHLEL distribution, then the mean and the median deviations are given as

δ1(x)=∫0∞|x−μ|g(x)dx=∫0μ(μ−x)g(x)dx+∫μ∞(μ−x)g(x)dx=2μG(μ)−2∫0μxg(x)dx

Notes

δ1(x)=2μG(μ)−4vθ∑k=0∞∑w=0∞∑i=0∞(−1)k+iΓ(v)(v−k)k!(−2w)(wvi)β−r+1B(r+1,θk+θi+θ−r)
θ>1

Where ∫0μxg(x)dx is simplified using the first incomplete moment

(27)δ2(x)=μ−4vθ∑k=0∞∑w=0∞∑i=0∞(−1)k+iΓ(v)(v−k)k!(−2w)(wvi)β−r+1B(r+1,θk+θi+θ−r)θ>1

a) Renyi Entropy

Entropy plays a vital role in science, engineering, and probability theory, and has been used in various situations as a measure of variation or uncertainty of a random variable (Renyi, 1961). The Renyi entropy of TIIHLEL is given as

b) Quantile and Median

Simulation methods utilize quantile function to produce simulated random variables for classical and new continuous distributions.

The inverse of the CDF in (6) yields the quantile function of the

x=1β(1−(((p2−p)1λ)1α)1θ−1)

When p = 0.25, 0.5 and 0.75 we obtain the first quantile, median and third quartile of TIIHLEL distribution In particular Q(0.5)=F−1(u) is the median of the probability distribution given as

F(x)=pr(X≤m)=∫0mf(x)dx=0.5

The median of TIIHLEL Distribution can be obtained by equating equation 28 to 0.5

(29)x=1β(1−(((13)1λ)1α)1θ−1)

c) Order of Statistics

Let Y1,Y2,…,Yn be independently and identically distributed (i.i.d) random variable with their corresponding cumulative function (cdf) F(x). Let X(1) be the smallest (first-order statistic) of the Y1,Y2,…,Yn, X(2) is the second-order statistics greater than X(1), and X(n) is the largest order statistics. Hence, X(1)<X(2)…<X(n) is the order statistics corresponding to random variable Y1,Y2,…,Yn (see Kapur and Sexena (1960)).

Notes

The density fn:i(x) of the ith order statistics, for i=1,…,n, from independent identical distribution random variable Y1…Yn is given by

fn:i(x)=f(x)B(i,n−i+1)F(x)i−1(1−F(x))n−i

i. Order Statistic of TIIHLEL

(30)f(x;α,β,λ)=f(x;α,β,λ,θ)B(r,n−r−1)∑ν=0n−r(−1)ν(n−rν)F(x;α,β,λ,θ)ν+r−1

B(.,.) is the beta function. The pdf of the rth order statistic for TIIHLEL distribution is derived by substituting (6) and (7) in (30) as follows.

f(x;α,β,λ,θ)=1B(r,n−r+1)∑ν=0n−r(−1)ν(n−rν)αβλθ[1−(1+βx)−θ]α−1(1+βx)−(θ+1)[[1−(1+βx)−θ]α]λ(ν+r)−1[[1−(1+βx)−θ]α]−(λ+r+1)

Applying the binomial expansion (12) in (31), then we have

f(x;α,β,λ)=1B(r,n−r+1)∑v=0n−r(−1)v+i(n−rv)(v+r+ii)
×αβλθ[1−(1+βx)−θ]α−1(1+βx)−(θ+1)[[1−(1+βx)−θ]α]λ(v+r+i)−1

Again, using the binomial expansion (12) in the previous equation, then the pdf of the rth order statistic for TIIHLEE distribution is obtained as follows.

(32)f(x;α,β,λ)=1B(r,n−r+1)∑v=0n−r∑I=0v+r−1∑J=0∞
η∗=(−1)v+i+j(n−rv)(v+r+ii)(λ(v+r+i)−1j)

The distribution of the smallest and largest order statistics are obtained by putting r=1 and r=n in (32) respectively as follows.

(33)f(1)(x;α,β,λ)=1B(r,n−r+1)∑k=0∞∑w=0∞∑i=0∞β(1+βx)−θk−θi−θ−1
η∗∗=(−1)v+i+j(n−1v)(v+1+ii)(λ(v+1+i)−1j)

However

ii. Skewness and kurtosis of the TIIHLEL distribution

Skewness is used to measure the asymmetry, and kurtosis is used to measure the peakedness of probabilistic models. Both measures are the descriptive measures of the shape of the probability distribution.

The skewness and Kurtosis of TIIHLEE are given as follows:

Notes

 Skewness =E(x−μ)3σ3=μ3σ3=μ31−3μ11μ21+2μ13(μ21−μ2)3/2
(34)Skewness=ϕi,k,wβ−2B(4,θk+θi+θ−3)(ϕi,k,wβ−1B(3,θk+θi+θ−2)−(ϕi,k,wB(2,θk+θi+θ−1))2)3

And

 Kurtosis =E(x−μ)4σ4=μ4σ4=μ41−4μ11μ31+6μ12μ31−3μ3(μ21−μ2)2
(35) Kurtosis =ϕi,k,wβ−3B(4,θk+θi+θ−4)(ϕi,k,wβ−1B(3,θk+θi+θ−2)−(ϕi,k,wB(2,θk+θi+θ−1))2)4
 V. PARAMETER ESTIMATION 

a) Maximum Likelihood Estimator (MLE) for TIIHLEL

Let x1;x2;…,xn be a random sample of size n from the TIIHL family of distributions (α;β;λ,θ). The log-likelihood function for the vector of parameters L=(α;β;λ,θ)T can be expressed as

f(x1,x2,x3,…,xn;α,β,λ,θ)=∏i=1nf(x)∏i=1n2αβλθ[1−(1−βx)−θ]α−1(1+βx)−(θ+1)[[1−(1+βx)−θ]α]λ−1[1+[[1−(1+βx)−θ]α]λ]2

The log-likelihood function is expressed as and let w=(1+βx)−θ

l=nlog⁡2+nlog⁡λ+nlog⁡β+nlog⁡θ+α−1∑i=1nlog⁡(1−w)−
(36)(θ+1)∑i=1nlog⁡(1+βx)+(λ+1)∑i=1nlog⁡(1+wα)−2(λ−1)log⁡∑i=1n(1−wα)

Taking the first partial derivatives of ℓ(x;α,β,λ,θ) of (36) with respect to α,β, and λ and letting them equal zero, we obtain a nonlinear system of equations.

Un(φ)=[δlog⁡lδα,δlog⁡lδβ,δlog⁡lδλ,δlog⁡lδθ]
δlog⁡lδα=nα+∑i=1nlog⁡(1−w)+(λ−1)∑i=1nwαlog⁡w1−w+2λ∑i=1nwαlog⁡w(1−wα)λ−1[1+(1+wα)λ]
δlog⁡lδβ=nβ+(α−1)∑i=1nθ(1+βx)θ−1(1+βx)θ+(θ−1)∑i=1nx1−βx+(λ−1)∑i=1nwαlog⁡w(1+wα)−2λβ∑log⁡w(1−wα)λ−1[1+(1−wα)λ]

Notes

δlog⁡lδθ=nθ+∑i=1nα−1(1−w)−∑i=1n(1−βx)+(λ−1)∑i=1nwαlog⁡w(1+wα)−2λ∑I=1nlog⁡wα(1−wα)λ−1[1+(1−wα)λ]

The above-derived equations are in the complex form; therefore, the exact solution of ML estimator for unknown parameters is not possible. So it is convenient to use nonlinear Newton Raphson algorithm for exact numerically solution to maximize the above likelihood function.

However, the above equation cannot be solved analytically, and statistical software can be used to solve them numerically using iterative methods.

Solving the nonlinear system of the equation of ∂lδα=0∂lδβ=0∂lδλ=0, and ∂lδθ=0 we then obtain the Maximum likelihood estimate α, β, λ, and θ respectively. Information matrix of 4x4 will be obtained through

(α^β^λ^θ^)=[(αβλθ)(V^ααV^αβV^αλV^αθV^βαV^ββV^βλV^βθV^λαV^λαV^λλV^λθV^θαV^θβV^θλV^θθ)]
V−1=−E(V^ααV^αβV^αλV^αθV^βαV^ββV^βλV^βθV^λαV^λαV^λλV^λθV^θαV^θβV^θλV^θθ)
Vαα=δ2lδα2Vβα=Vαβ=δ2lδαβVαλ=Vαλ=δ2lδαλ
Vββ=δ2lδβ2Vλβ=Vβλ=δ2lδβλVλθ=Vθλ=δ2lδθλ
Vλλ=δ2lδλ2Vθβ=Vβθ=δ2lδβθVθα=Vαθ=δ2lδαθ
Vθθ=δ2lδθ2
Vαλ=Vλα=δ2lδαλ
Vλβ=Vβλ=δ2lδβλ

The solution to the above equation inverse dispersion matrix yields the asymptotic variance and covariance of the maximum likelihood estimators α^,β^,λ^ and θ

b) Confidence Interval for the Parameters

The approximate confidence intervals for 100(α−1)% for α, β and λ is given respectively by

α^±Zα2Vαα,β^±Zα2Vββλ^±Zα2Vλλθ^and±Zα2Vθθ

Where the Zα2 is the αth percentiles of the standard normal distribution.

VI. SIMULATION STUDY FOR TIIHLEL DISTRIBUTION

A simulation study was carried out to check MLE of TIIHLEL for different sample size n=10 and 100 in order to obtain Mean, Median, Standard Deviation, Skewness, and Kurtosis of the parameters. The quantile function of TIIHLEL used for simulation studies is given in (28) with α, θ, and λ as shape parameters while β is a scale parameter.

Table 2: The Mean, Median and Standard of TIIHLEL Distribution for β=2, 4 and 6 for n=10
αλθβ=2β=4β=6
MeanMedianSD(σ)MeanMedianSD(σ)MeanMedianSD(σ)
0.50.50.50.45680.11461.1677-0.0612-0.03780.0769-0.1373-0.08530.1412
0.872.4466-0.000321.525636.1165-0.0098160.674224.006-0.0201107.0571
2.53.6512-0.005615.7741.7188-0.04017.7977-0.1627-0.09560.1772
50.0246-0.03320.3320-0.1373-0.08530.1412-0.1341-0.09420.1322
0.80.5-0.1341-0.09420.1322-0.1088-0.09760.0949-0.2155-0.19010.1574
0.873.5713-0.0064325.962836.6245-0.04936162.903924.3089-0.0681108.551
2.5187.21950.1497829.03321.6962-0.10427.91761.0233-0.13375.2270
5-0.0145-0.07830.3475-0.1684-0.14860.1606-0.2197-0.17630.1596
2.50.5-0.2416-0.29670.1691-0.4400-0.52430.1643-0.4400-0.52430.1643
0.80.67820.21581.8055-0.1262-0.14350.1140-0.1810-0.37350.5405
2.50.0746-0.05770.5156-0.2693-0.31630.0931-0.3823-0.49440.1715
5-0.2266-0.28080.0830-0.2680-0.37270.2282-0.4827-0.57730.1776
50.5-0.4969-0.59060.1889-0.3401-0.37980.0684-0.5510-0.61650.1233
0.80.70130.25361.9227-0.0302-0.28380.9234-0.2741-0.47280.5955
2.50.0424-0.07850.5637-0.3597-0.45150.2536-0.4937-0.57560.1713
5-0.2921-0.32740.0760-0.5270-0.58640.1100-0.6053-0.67630.1326
50.50.540.179611.4196101.185620.00065.610850.520713.2743.67433.6324
0.83.38261.74716.88941.60210.77463.36981.00860.45042.1969
2.50.09640.05870.1796-0.0409-0.05970.0365-0.0867-0.11240.0623
5-0.0228-0.03340.0199-0.1006-0.11820.0852-0.1630-0.14480.1127
0.80.553.769820.9489123.643526.735510.292861.743417.72406.740741.1101
0.84.81073.20568.36314.09641.42112.25591.40430.82632.6748
2.50.13830.10770.2196-0.0802-0.12000.0608-0.1531-0.20630.0899
5-0.044-0.06710.0332-0.1718-0.2170.1118-0.2142-0.26580.1455
2.50.577.590341.6750154.4153-0.3633-0.43210.1223-0.2030-0.24820.0960
0.87.55886.378210.352638.489720.475977.144625.456213.409551.3878
2.50.20470.21430.29223.47402.82755.09952.11241.64393.3496
50.20470.21430.2922-0.1159-0.13680.05306-0.3389-0.40530.1065
50.5-0.4458-0.52910.1601-0.1581-0.16320.0657-0.4600-0.50500.0834
0.885.208748.9973162.514642.223324.073481.214027.894915.765554.1138
2.58.49427.499210.86533.86613.32445.37762.32341.93273.5490
50.21460.25200.3287-0.2736-0.29520.1119-0.4364-0.47520.0812

Table 3: The Skewness and Kurtosis of TIIHLEL Distribution for

β=2, 4 and 6 for n=10

αλθβ=2β=4β=6
SkewnessKurtosisSkewnessKurtosisSkewnessKurtosis
0.50.50.53.546411.9068-0.0399-0.41024.127415.0420
0.84.129315.05174.129315.05184.129315.052
2.54.125315.03084.127315.0411-1.07890.2465
54.021214.4969-0.80800.5781-0.7710-0.4931
0.80.5-0.7710-0.49310.2994-0.5633-0.3013-1.3714
0.84.129215.05144.129215.05164.129315.0517
2.54.123715.02204.126115.03484.125915.0341
53.963414.19640.4488-0.0229-0.4095-1.2322
2.50.5-0.0479-0.61491.16630.03561.16630.0356
0.82.59304.8830-0.94250.70852.50434.5680
2.52.56684.80551.38550.54070.9324-0.7940
50.99810.46931.91092.42841.22560.1210
50.51.0998-0.05431.65491.68961.56301.1823
0.82.55474.76662.61074.93912.58794.8580
2.52.47244.52252.34063.98071.58611.0848
51.37360.19681.66571.61721.61611.3417
50.50.52.64235.03532.64285.03702.64345.0387
0.82.56184.78752.57674.83282.59104.8764
2.52.47564.52300.3896-1.65300.2895-1.1503
50.3994-1.6633-0.65310.1630-0.88600.5991
0.80.52.61874.96232.61974.96562.620834.9688
0.82.45704.47424.55892.48584.64072.5134
2.52.26353.90130.5666-1.46160.8356-1.0938
5-1.42780.5930-0.95320.3123-0.76280.0933
2.50.52.56374.79511.40430.60121.58161.0399
0.83.79042.216438.489720.47592.56694.8047
2.51.56242.08752.26033.91024.02782.3027
52.08751.56241.64081.30261.33120.6895
50.51.23980.20871.74102.66982.23631.8416
0.84.73642.54414.74022.54544.74402.5467
2.53.56552.13312.54544.74022.20193.7486
51.22111.16343.65762.16801.34640.0667

Table 4: The Mean, Median and Standard of TIIHLEL Distribution for

β=2, 4 and 6 for n=100

αλθβ=2β=4β=6
MeanMedianSD(σ)MeanMedianSD(σ)MeanMedianSD(σ)
0.50.50.5-0.5481-0.56470.0866-0.0599-0.02320.0714-0.1157-0.04260.1413
0.820.8214-0.0022197.975610.3249-0.012498.94636.8260-0.018965.9366
2.51.0874-0.00498.66880.4579-0.02154.28890.2480-0.02722.8305
5-0.0196-0.01690.1671-0.0956-0.03510.1206-0.1209-0.04720.1448
0.80.5-0.1343-0.04760.1683-0.1027-0.07230.0855-0.1859-0.12440.1626
0.821.2299-0.01517200.31010.4804-0.0548100.1186.8972-0.071766.7204
2.51.12112-0.026168.77720.4259-0.07644.34650.1942-0.09572.8718
5-0.05502-0.05740.1772-0.1620-0.10940.1430-0.1977-0.12740.1699
2.50.5-0.2474-0.25150.0827-0.1865-0.23210.2013-0.4139-0.41900.1417
0.821.6878-0.0906202.994410.5537-0.2745101.47526.8423-0.343267.6354
2.51.09779-0.16508.91410.2586-0.32514.4306-0.0210-0.39132.9379
5-0.2136-0.13890.1920-0.3834-0.399370.1384-0.4491-0.44710.1529
50.510.51839-0.184895.5571-0.3265-0.34580.0694-0.5363-0.54730.0956
0.821.7714-0.1782203.634510.5126-0.4272101.80386.7597-0.503367.8602
2.51.0558-0.23018.95290.1548-0.45924.4596-0.1454-0.54732.9627
5-0.2613-0.31820.2144-0.5036-0.52680.1151-0.5844-0.60680.1096
50.50.5-0.6062-0.61820.1136-0.0020-0.0100.0850-0.0868-0.03700.099
0.82047.1480.904019528.851023.4880.42329764.385682.26810.26296509.56
2.520.93900.2003154.376910.38370.071477.14046.86520.028451.395
50.183710.00050.59850.0060-0.01710.2319-0.0531-0.03200.1384
0.80.5-0.1150-0.04390.1383-0.0207-0.03470.0920-0.1449-0.09820.1169
0.82088.7022.637419758.931044.2161.23489879.42696.05460.76726586.26
2.522.52560.5845156.233611.12820.208378.07147.32910.082952.0175
50.21730.00140.6242-0.0258-0.06040.2430.1069-0.09060.153
2.50.5-0.1863-0.12810.1593-0.1020-0.13940.1166-0.3412-0.35270.1003
0.82143.598.875720022.41071.5054.155410011.19-0.30200.34380.1745
2.525.24761.9671158.32512.33360.701179.13348.02890.279152.7363
50.25460.00490.6716-0.1629-0.23820.2800-0.3020-0.34380.1745
50.5-0.4209-0.41600.13520.6716-0.13940.1166-0.3412-0.35270.1003
0.82143.598.875720022.431071.5054.155410011.19714.14312.58196674.113
2.525.24761.9671158.32512.33360.701179.13348.02890.279152.7363
50.254600.00490.6716-0.1629-0.23820.2800-0.3020-0.30200.1745

Table 5: The Skewness and Kurtosis of TIIHLEL Distribution for

β=2,4 and 6 for n=100

αλθβ=2β=4β=6
SkewnessKurtosisSkewnessKurtosisSkewnessKurtosis
0.50.50.51.17360.7588-0.6676-0.1583-1.22380.2005
0.89.845794.96229.846094.96709.846494.9714
2.59.761793.8539.796894.31739.815594.5665
58.996984.1612-0.56740.5139-1.19800.1487
0.80.5-1.31570.5088-0.1719-0.8034-0.7097-0.7971
0.89.844794.94949.845194.95509.845594.9601
2.59.735793.50779.776194.04329.794794.2936
58.328575.7668-0.1286-0.2565-0.6729-0.8766
2.50.51.54563.88657.474464.33240.3906-0.8094
0.89.843294.92969.843594.93429.843894.9384
2.59.686792.85749.722193.32739.740593.5753
5-0.7875-0.64941.65035.01710.5092-0.7558
50.59.834294.81213.572220.17400.96090.2476
0.89.842794.92359.842994.92669.843294.9295
2.59.666892.59429.693492.94659.711793.1910
57.133459.36323.984224.29801.50162.6275
50.50.50.02570.81558.323074.7721-1.0862-0.1474
0.89.846394.97019.846394.97029.846394.9702
2.59.737993.537693.57529.740789.743593.6121
57.047757.74578.997783.65606.805358.3758
0.80.5-1.19050.11527.344662.3746-0.5338-1.0873
0.89.845594.95989.845594.95989.845594.95993
2.59.707493.13319.710893.17869.7142493.223
56.399949.73718.433176.29195.877947.5133
2.50.5-0.6689-0.855736.36405.26280.8337-0.2018
0.89.84494.94489.8494.94480.8337-0.2018
2.59.663892.55639.666892.59529.669792.6338
55.352937.729.844394.94496.452852.3660
50.50.4957-0.67745.262836.36400.8337-0.2018
0.89.844394.94489.844394.94489.844394.9449
2.592.55639.66389.666892.59529.669792.6335
55.352937.72326.977457.25136.452852.3660

From the above table 2, and 4 present simulation study for sample 10 and 100 respectively, this observed that the mean, standard deviation, and median are increasing, and decreasing functions of the shape parameters θ when the other parameters are held constant, an increase in scale parameter β increases the mean, standard deviation and median for fixed α, λ, and θ. Also, Table 3 and 5, Skewness, and kurtosis is an increasing function as the scale parameter β increases when the shape parameters are held constant. An increase in the shape parameters reduces the values of skewness and kurtosis when the scale parameter is held constant.

VII. APPLICATIONS OF TIIHLEL DISTRIBUTION

In this section, the flexibility of the TIIHLEL Distribution is illustrated employing two (2) real data sets are demonstrated. We compare the fits of the TIIHLEL distribution with some distribution namely; Type II half Burr X (TIIHLBX), Type I half Burr X (TIHLBX), Type II half exponential (TIIHLE), Exponential distribution, Exponentiated Exponential (EE), Pareto Distribution.

The Log-likelihood (LL), Akaike Information Criterion (AIC), Bayesian Information Criterion (BIC), Anderson-Darling ( A∗ ), Cramér-von Mises ( W∗ ) and Kolmogorov-Smirnov (K-S) are computed to compare the fitted model, the smaller the value of these statistics the better the fit to the data.

Table 6: First data set: Here apply the data consist the remission times (in months) of a random sample of 128 bladder cancer patients studied by Lee et al. (2003) reported by Cordeiro and Lemonte (2013) and Oluyede et al. (2014) as presented in Table 4.5 Source: Lee et al. (2003)
0.0800.2000.4000.5000.5100.8100.9001.0501.1901.2601.3501.4001.4601.760
2.0202.0202.0702.092.2302.2602.4602.5402.6202.6402.6902.6902.7502.830
2.8703.0203.253.3103.3603.3603.4803.5203.5703.6403.7003.8203.8804.180
4.2304.2604.3304.3404.4004.5004.5104.8704.9805.0605.0905.1705.3205.320
5.3405.4105.4105.4905.6205.7105.8506.5406.7606.9306.946.9707.0907.260
7.2807.3207.3907.5907.6207.6307.6607.8707.9308.2608.3708.5308.6508.660
9.0209.2209.4709.74010.0610.3410.6610.7511.2511.6411.7911.9812.0212.03
12.0712.6313.1113.2913.8014.2414.7614.7714.8315.9616.6217.1418.1019.13
21.7322.6923.6325.7425.8226.3132.1534.2636.6643.0146.1279.05

Empirical density
Fig. 5: Histogram and CDF Plots of an Empirical Distribution for bladder cancer patient The empirical density plot in Fig. 4.1: Histogram and CDF Plots of an Empirical Distribution for Bladder Cancer Patient
Fig. 5: Histogram and CDF Plots of an Empirical Distribution for bladder cancer patient The empirical density plot in Fig. 4.1: Histogram and CDF Plots of an Empirical Distribution for Bladder Cancer Patient

Table 8 shows the parameters estimates obtained from the proposed distribution and it sub distributions

Table 7: Descriptive Statistics Bladder Cancer Patient The Summary statistics of data in table 6 displayed in table 7 shows that the first data set on a bladder cancer patient is over-dispersed and right-skewed, Correlation matrix of TIIHLEL
MinMaxMeanSDMedianQ1Q3SkewnessKurtosis
0.08079.0509.36610.50836.3953.34811.8403.286615.4831

Notes

1.00000000.008513745-0.9995557980.006030967
0.0085137451.00000000.006280632-0.978044473
-0.9995557980.0062806321.0000000-0.004450433
-0.006030967-0.006030967-0.0044504331.0000000

The above correlation matrix indicates the pairs which have negative and positive correlation coefficient depending on the combination of the parameters.

Table 8: Maximum Likelihood Estimates of Parameters and their Standard Errors for Bladder Cancer Patient
Estimated Parameter
Distributionsα^β^λ^θ^
TIIHLEL8.0874(34.3684)0.0161(0.0108)0.2017(0.8573)7.4603(4.2817)
TIIHLBX0.1758(0.6831)0.0432(0.0039)2.7817(10.8111)
TIHLBX0.1758(0.6831)0.0432(0.0039)2.7817(10.8111)
TIIHLE1.5988(0.2032)0.1454(0.0149)
EE1.2186(0.1489)8.2466(0.9228)
E6.0891(0.3999)
Table 9: Goodness-of-fit Statistics, Log-likelihood and Information Criteria for Bladder Cancer Patient
DistributionAICBICLLA∗W∗K-S
TIIHLEL828.4315839.8397-410.21580.19710.02790.0385
TIIHLBX847.7955856.3516-420.89782.82600.55450.1242
TIHLBX847.7955856.3516-420.897845.90309.83900.5000
TIIHLE973.9203979.6243-484.96015.63650.95160.1365
EE830.8943835.8593-413.07760.71100.12720.0723
E1023.3481026.2000-510.673911.28311.99380.1792

Table 9 revealed that the TIIHLEE distribution provides a better fit to the bladder cancer patient data than other competitive models, the TIIHLE, HLEE, HLE, and the E distribution. The TIIHLEE distribution has the highest log-likelihood and the smallest K-S, W*, A*, AIC, and BIC values compared to the other models. Although the TIIHLEE distribution provides the best fit to the data and the EE distribution is alternatively good model for the data since it measures of fit value are close to that of the TIIHLEE distribution.

The estimated asymptotic variance-covariance matrix of the TIIHLEL distribution for the bladder cancer patient data is given by

Iij−1=(1.181187e+033.178176e−03−2.945031e+01−0.887500733.178176e−031.179766e−045.848234e−05−0.04548612−2.945031e+015.848234e−057.349316e−01−0.01633609−8.875007e−01−4.548612e−021.633609e−0218.33346935)

Notes

However, the confidence interval at 95% for the estimate α^, β^, λ^ and θ^ are (-59.2747, 75.44947), (0.0052, 0.0379), (-1.4786, 1.8819) and (-0.9319, 11.7421) respectively. The confidence interval for the parameters contains zero. Thus, all the estimated parameters of the TIIHLEL distribution were significant at the 5% significance level

Histogram and theoretical densities Fig. 6: Fit Plot of TIIHLEE Model with other Models for Bladder Cancer Patient

Fig 6 shows the histogram of the bladder cancer data set along with the fitted model. The theoretical density of TIIHLEL distribution has a better spread to the right than other existing models on the data set.

Table 10: Second Data Set
17.8828.9233.0041.5242.1245.6048.8051.84
51.9654.1255.5667.8068.4468.6468.8884.12
93.1298.64105.12105.84127.92128.04173.40

Table 10 Represents the number of million revolutions before failure for each of twenty-three (23) deep groove ball bearings in the life tests. The data set was given by Lawless (1982).

Table 11: Summary Statistics of Deep Groove Ball Bearings
MinMaxMeanSDMedianQ1Q3SkewnessKurtosis
17.88173.4072.2337.480467.847.2095.880.94190.4889

figure 5 shows that the data set is right skewed. Cumulative distribution
Fig. 7: Histogram and CDF Plots of an Empirical Distribution for deep groove ball bearings
Fig. 7: Histogram and CDF Plots of an Empirical Distribution for deep groove ball bearings

Figure 7 shows the empirical plot of data set in table 10 which is right skewed Correlation matrix of TIIHLEL Distribution

1.00000000.06631924-0.934932490.05851001
0.066319241.00000000.06631901-0.70226965
-0.934932490.066319011.00000000.05850993
0.05851001-0.93681860.058509931.0000000

The above correlation matrix indicates the pairs which have negative and positive correlation coefficient depending on the combination of the parameters.

Table 12: Maximum Likelihood Estimates of Parameters and their Standard Errors for Deep Groove Ball Bearings Table 12 shows the parameters estimates obtained from the proposed distribution and it sub distributions.
Estimated Parameter
Distributionsα^β^λ^θ^
TIIHLEL2.6919(2.9647)0.0056(0.0018)2.5214(2.7769)6.3149(1.8623)
TIIHLBX0.5337(3.1771)0.0119(0.0017)2.7063(16.1097)
TIHLBX0.5337(3.1771)0.0119(0.0017)2.7063(16.1097)
TIIHLE5.7321(2.2575)0.0332(0.0065)
EE5.2936(2.0542)30.9302(6.1506)
PARETO0.2399(0.0500)
Table 13: Goodness-of-fit Statistics, Log-likelihood and Information Criteria for Deep Groove Ball Bearings
DistributionAICBICLLA*W*K-S
TIIHLEL438.8069446.2917-215.40340.16810.02410.0740
TIIHLBX452.346457.9596-223.17301.58150.27690.1572
TIHLBX452.346457.9596-223.173015.68563.33330.5000
TIIHLE439.8658448.6082-217.93290.57300.07980.0963
EE442.8943446.6367-219.44710.86290.13010.1169
PARETO593.7705595.6417-295.885316.91443.64820.5483

Notes

The TIIHLEL distribution provides a better fit to the data set compared to the other models. From Table 13, the TIIHLE distribution has the highest log-likelihood and the smallest K-S, W*, A*, AIC, and BIC values compared to the other fitted models.

The asymptotic variance covariance matrix for the estimated parameters is

Iij−1=(8.78941492343.583368e−047.69689387530.323040360.00035833683.321573e−060.0003356335−0.00238354−7.69689387533.356335e−047.71099680350.302573890.3230403634−2.383540e−03−0.30257388973.46811291)

The confidence interval at 95% for the estimate α^, β^, λ^ and θ^ are (-3.1189, 8.5028), (0.0055, 0.0167), (-2.92126, 7.9641) and (2.6648, 9.9649) respectively.. It can be observed that the confidence intervals for the parameters do not contain zero, this shows that all the parameters of the TIIHLEL distribution were significant at the 5% significance level.

Histogram and theoretical densities Fig. 8: Fit Plot of TIIHLEL Model with other Models for Deep Groove Ball Bearings Discharge

Fig 8 also shows the histogram of the Deep Groove Ball Bearings data set along with the fitted model. The theoretical density of TIIHLEL distribution has a better spread to the right than other competing models on the data set.

VIII. CONCLUSIONS

In this study, we have derived, studied the properties and applications Type II Half Logistic Exponentiated Lomax (TIIHLEL). Some structural mathematical properties; Moment Incomplete moments, Probability Weighted Moment, Order Statistic, and Rényi entropy of the derived model are investigated. A simulation study is carried out to estimate the behavior of the shape and scale model parameters. Also, maximum likelihood estimators were investigated. The application of two real-life data set shows that the TIIHLEE strong and better fit as compare to other existing distribution. However, we hope that this distribution will attract wider applications in the areas of sciences and applied sciences.

References

19 Cites in Article
  1. 1. Al-Zahrani B,Al-Sobhi M (2013). On parameters estimation of Lomax distribution under general progressive censoring. Journal of Quality and Reliability Engineering
  2. 2. B Al-Zahrani,H Sagor (2014). The Poisson-Lomax distribution. Revista Colombiana de Estad´ıstica, 37(1), 225-245.
  3. 3. S Ashour,M Eltehiwy (2013). Transmuted Lomax Distribution. American Journal of Applied Mathematics and Statistics, 1(6), 121-127.
  4. 4. N Balakrishnan (1985). Order statistics from the half logistic distribution. Journal of Statistical Computation and Simulation, 20, 287-309.
  5. 5. Gauss Cordeiro,Artur Lemonte (2013). On the Marshall–Olkin extended Weibull distribution. Statistical Papers, 54(2), 333-353.
  6. 6. G Cordeiro,E Ortega,B Popovi´c (2015). The gamma-Lomax distribution. Journal of Statistical Computation and Simulation, 85(2), 305-319.
  7. 7. A H.El-Bassiouny,N F. Abdo,H S. Shahen (2015). Exponential Lomax Distribution. International Journal of Computer Applications, 121(13), 24-29.
  8. 8. A Hassan,M Elgarhy,M Shakil (2017). Type II Half Logistic -generated family of distributions with applications. Pakistan Journal of Statistics and Operation Research, 13, 245-264.
  9. 9. A Hassan,A Al-Ghamdi (2009). OPTIMUM STEP-STRESS ACCELERATED LIFE TEST MODELS. Optimum Accelerated Life Testing Models with Time-Varying Stresses, 5, 63-88.
  10. 10. J Kapur,H Sexena (1960). Mathematical Statistics, First Edition S. Mathematical Statistics, First Edition S
  11. 11. N Kilany (2016). Weighted Lomax distribution. SpringerPlus, 5(1), 1862.
  12. 12. A Law,W Kelton (1991). Simulation Modeling and Analysis. Simulation Modeling and Analysis
  13. 13. Carl Lee,Felix Famoye,Ayman Alzaatreh (2013). Methods for generating families of univariate continuous distributions in the recent decades. WIREs Computational Statistics, 5(3), 219-238.
  14. 14. K Lomax (1954). Business Failures: Another Example of the Analysis of Failure Data. Journal of the American Statistical Association, 49(268), 847-852.
  15. 15. B Oluyede,S Huang,M Pararai (2014). A new class of generalized dagum distribution with applications to income and lifetime data. Journal of Statistical and Econometric Methods, 125-151.
  16. 16. El-Houssainy A. Rady,W Hassanein,T Elhaddad (2016). The power Lomax distribution with an application to bladder cancer data. SpringerPlus, 5(1), 1838.
  17. 17. A Renyi (1961). On measures of entropy and information. Fourth Berkeley Symposium on Mathematical Statistics and Probability, 547-561.
  18. 18. H Salem (2014). The exponentiated lomax distribution: different estimation methods. American Journal of Applied Mathematics and Statistics, 2(6), 364-368.
  19. 19. M Tahir,Gauss Cordeiro,M Mansoor,M Zubair (2015). WEIBULL-LOMAX DISTRIBUTION: PROPERTIES AND APPLICATIONS. Hacettepe Journal of Mathematics and Statistics, 44(14), 1-1.

Funding

No external funding was declared for this work.

Conflict of Interest

The authors declare no conflict of interest.

Ethical Approval

No ethics committee approval was required for this article type.

Data Availability

Not applicable for this article.

How to Cite This Article

Bukoye Abdulwasiu, Bada Olatunbosn, Muritala Abdulkabir, Ajadi, A.Akeem. 2021. "Type Ii Half Logisitic Exponentiated Lomax Distribution". Global Journal of Science Frontier Research - F: Mathematics & Decision GJSFR-F Volume 21 (GJSFR Volume 21 Issue F3).

More Citation Formats

Download Citation

Journal Specifications

Crossref Journal DOI 10.17406/GJSFR

Print ISSN 0975-5896

e-ISSN 2249-4626

Keywords
Classification
GJSFR-F Classification MSC 2010: 11D61
Version of record

v1.2

Issue date
July 2, 2021

Language
English
Order Article Reprint
Experience in AR

Explore published articles in an immersive Augmented Reality environment. Our platform converts research papers into interactive 3D books, allowing readers to view and interact with content using AR and VR compatible devices.

Read in 3D

Your published article is automatically converted into a realistic 3D book. Flip through pages and read research papers in a more engaging and interactive format.

Article Matrices
Total Views: 873
Total Downloads: 77
All Trends

Request Access

Please fill out the form below to request access to this research paper. Your request will be reviewed by the editorial or author team.
X

This is the heading

Lorem ipsum dolor sit amet, consectetur adipiscing elit. Ut elit tellus, luctus nec ullamcorper mattis, pulvinar dapibus leo.

High-quality academic research articles on global topics and journals.

Type Ii Half Logisitic Exponentiated Lomax Distribution

Bukoye Abdulwasiu
Bukoye Abdulwasiu
Bada Olatunbosn
Bada Olatunbosn
Muritala Abdulkabir
Muritala Abdulkabir
Ajadi, A.Akeem
Ajadi, A.Akeem