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APPLIED & INTERDISCIPLINARY MATHEMATICS

Some mathematical properties of Odd Kappa-G family

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Article: 2095091 | Received 06 Apr 2022, Accepted 23 Jun 2022, Published online: 07 Jul 2022

ABSTRACT

We present in this paper further mathematical properties of the Odd Kappa-G family of distributions. These structural properties of this family hold for any baseline model including characterizations results based on two truncated moments and hazard and reversed hazard functions. In addition, kth lower record values and extreme values of this Odd Kappa-G family are introduced. Lastly, the bivariate probability distributions of the Odd Kapp-G (BFGMOKG) family based on FGM copula are obtained.

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1. Introduction

In recent decades, many classical distributions have been widely employed for data modeling in a variety of fields such as demographics, economics, finance, insurance, biological research, medicine, engineering, environment and actuarial sciences. However, because of their lack of flexibility, various methods for generating new distributions from these old ones have piqued the interest of theoretical and applied statisticians in recent years

Albert & Olkin (Citation1997) suggested an innovative method for adding a new parameter to an existing distribution in order to create a more flexible new family of distributions. Eugene et al. (Citation2002) proposed a new class of distributions based on the beta distribution. M.C. Jones (Citation2009) and Gauss & de Castro (Citation2011) extended the beta-generated technique with the Kumaraswamy distribution as a generator instead of beta distribution.

Other known generators, just to mention a few, include gamma-G type 1 by Zografos & Balakrishnan (Citation2009), gamma-G type 2 by Miroslav & Balakrishnan (Citation2012), gamma-G type 3 by Torabi & Montazeri Hedesh (Citation2012), McDonald-G (Mc-G) by Alexander et al. (Citation2012), Weibull-G by Bourguignon et al. (Citation2014), Transformed-Transformer (T-X) by Alzaatreh et al. (Citation2013), exponentiated (T-X) by Alzaghal et al. (Citation2013), T-X { Y } -quantile based approach by Aljarrah et al. (Citation2014), T-R { Y } by Alzaatreh et al. (Citation2014). alpha power transformation introduced by Mahdavi & Kundu (Citation2017). Furthermore, Al-Shomrani et al. (Citation2016) established the Topp–Leone family of distributions by employing the Topp–Leone distribution. Moreover, Al-Shomrani (Citation2018) introduced new generalized statistical probability distributions based on extensions of beta and hypergeometric distributions. For other revisions of other generators, see M. C. Jones (Citation2015), Famoye et al. (Citation2013), Lee et al. (Citation2013), Tahir & Nadarajah (Citation2015) and Muhammad & Gauss (Citation2016).

The Kappa distribution, an attractive asymmetric distribution, was introduced by Paul (Citation1973) and Paul & Earl (Citation1973). This distribution has recently received increased attention in hydro-logical research for the use in the evaluation of precipitation, stream-flow and wind speed data. The three-parameter Kappa cumulative distribution function (cdf; (Paul & Earl, Citation1973)) is

(1.1) Rt=tbλa+tbaλ1afort,a,bandλ>0,(1.1)

where a and λ are shape parameters and b is a scale parameter. The probability density function (pdf) is

(1.2) rt=aλbtbλ1a+tbaλa+1afort,a,bandλ>0.(1.2)

Note that if λ=b=1, the three-parameter Kappa distribution reduces to one-parameter Kappa distribution. Also, if λ=1, the three-parameter Kappa distribution reduces to two-parameter Kappa distribution.

The Kappa distribution was extended in certain ways. Hussain (Citation2015) suggested three expanded versions of the Kappa distribution: Kumaraswamy generalized Kappa (KGK), McDonald generalized Kappa (McGK) and Exponentiated generalized Kappa (EGK). The author examined the different statistical characteristics of those new extended forms, used different approaches to assess their unknown parameters and applied these models to real-world datasets. Javed et al. (Citation2019) proposed the Marshall-Olkin Kappa (MOK) distribution while Nawaz et al. (Citation2020), derived from Hussain (Citation2015), offered the Kumaraswamy generalized Kappa (KGK) distribution.

As an extension of Kappa distribution with its cdf and pdf is shown, respectively, in EquationEquation (1.1) and (Equation1.2), Al-Shomrani & Al-Arfaj (Citation2021) presented a new flexible family of distributions called the Odd Kappa-G family whose cdf is defined as

(1.3) Fx;α,β,θ,ϑ=G(x;ϑ)β1G(x;ϑ)αθα+G(x;ϑ)β1G(x;ϑ)αθ1α,xR.(1.3)

The pdf of the Odd Kappa-G family of distributions can be expressed as follows:

fx;α,β,θ,ϑ=αθβgx;ϑ1Gx;ϑ2Gx;ϑβ1Gx;ϑθ1×
(1.4) α+G(x;ϑ)β1G(x;ϑ)αθα+1α.(1.4)

where fx;α,β,θ,ϑ=ddxFx;α,β,θ,ϑ and gx;ϑ=ddxGx;ϑ . Gx;ϑ and gx;ϑ are, respectively, the cdf and pdf of the baseline distribution with parameter(s) ϑ. Moreover, the survival or reliability function (sf) of the Odd Kappa-G family of distributions is defined as the following:

(1.5) Sx;α,β,θ,ϑ=1G(x;ϑ)β1G(x;ϑ)αθα+G(x;ϑ)β1G(x;ϑ)αθ1α,(1.5)

Let Fx=Fx;α,β,θ,ϑ, fx=fx;α,β,θ,ϑ, Gx=Gx;ϑ and gx=gx;ϑ. These shortcuts will be used throughout the paper when there is no confusion involved. EquationEquation (1.4) is most tractable when the cdf Gx and the pdf gx have simple analytic expressions

Al-Shomrani & Al-Arfaj (Citation2021) provided a comprehensive study of the mathematical properties of this new family; for instance, linear expansions for its cdf and pdf and explicit expressions for quantile function, the ordinary and incomplete moments, moment generating function, order statistics, Bonferroni and Lorenz curves, mean residual life, mean waiting time, mean deviations, entropy and other mathematical properties are derived. In this paper, further mathematical properties of this family such as characterization results of the Odd Kappa-G family based on two truncated moments and hazard and reversed hazard functions will be discussed. In addition, kth lower record values and extreme values of this Odd Kappa-G family are introduced. Lastly, the bivariate probability distributions of the Odd Kapp-G (BFGMOKG) family based on FGM copula are obtained. These topics will be introduced and studied thoroughly in this paper.

The rest of the paper is organized as follows. In Section 2, we introduce some characterization results of the Odd Kappa-G family including characterizations based on two truncated moments, hazard and reversed hazard functions. We discuss the kth lower record values of the Odd Kappa-G family in Section 3. In Section 4, extreme values for this family are presented. The bivariate cdf, pdf and sf of the Odd Kappa-G family based on FGM copula are obtained in Section 5. Finally, we give some concluding remarks in Section 6.

2. Characterizations results

2.1. Characterizations based on two truncated moments

In this section, we give characterizations of the Odd Kappa-G family of distributions in terms of a simple connection between two truncated moments. The characterization findings reported here will make use of intriguing theorem from Glänzel (Citation1987) stated below. Because of the nature of the Odd Kappa-G family of distributions, we feel that our characterizations of Odd Kappa-G distribution may be the only ones conceivable. In this regard, we would like to highlight the work of Glänzel (Citation1987, Citation1990), Glänzel & Hamedani (Citation2001) and Hamedani (Citation2010).

Theorem 2.1 (Glänzel, Citation1987). Suppose Ω,A,P be a given probability space and let X:ΩΞ be a continuous random variable with distribution function F, where Ξ=a,b for some a<b; a= and b=+ are not excluded. Let ξ1 and ξ2 be two real functions defined on Ξ such that Eξ1X|Xx=Eξ2X|Xx δx,xΞ, is defined with some real function δ. Assume that ξ1,ξ2C1Ξ,δC2ΞandF is twice continuously differentiable and strictly monotone function on the set Ξ. Finally, assume that the equation δξ2=ξ1 has no real solution in the interior of Ξ. Then, F is uniquely determined by the functions ξ1,ξ2andδ, particularly

Fx=axCδtδtξ2tξ1testdt,

where the function s is a solution of the differential equation s=δξ2δξ2ξ1 and C is a constant, chosen to make ΞdF=1.

Remark 1. In the aforementioned Theorem 2.1, we could take ξ2X=1 which reduces the condition to Eξ1X|Xx=δx but in terms of application, adding this function provides a lot more flexibility.

Proposition 1. Suppose X:ΩR be a continuous random variable and let

ξ2x=β1Gx1+θα+Gxβ1Gxαθα+1α

and ξ1x=ξ2xGx for xR. The pdf of X is (1.4) if and only if the function δ defined in Theorem 2.1 has the form

(2.1) δx=θθ+11Gxθ+11Gxθ,xR.(2.1)

Proof. Using the same proof techniques used in Proposition 6 on page 83 in the work by Merovci et al. (Citation2016), let X has pdf (1.4); then, for xR,

1FXxEξ2X|Xx=αβ1Gxθ,

and

1FXxEξ1X|Xx=αθβ1Gxθ+1θ+1,

and lastly,

δxξ2xξ1x=ξ2xθ+11GxθθGxθ+1Gxθ>0.

Conversely, if δx is stated as in EquationEquation (2.1), then

sx=δxξ2xδxξ2xξ1x=θgxGxθ11Gxθ,xR,

from which we have

sx=log1Gxθ,xR.

Hence, in light of Theorem 2.1, X has pdf (1.4).

Corollary 2.2. Suppose X:ΩR be a continuous random variable and let ξ1x be as in Proposition 1. The pdf of X is (1.4) if and only if there exist functions ξ2x and δx defined in Theorem 2.1 satisfying the differential equation

δxξ2xδxξ2xξ1x=θgxGxθ11Gxθ,xR.

Remark 2. (1) The general solution of this differential equation in Corollary 2.2 is

δx=1Gxθ1θgtGtθ1ξ1tξ2tdt+D,

where D is a constant. One set of appropriate functions ξ1,ξ2,δ that fulfill the aforementioned differential equation is given in Proposition 1 with D=0.

(2) It should be observed, however, that there are triplets ξ1,ξ2,δ that meet the criteria of Theorem 2.1.

2.2. Characterizations based on hazard function

Definition 2.3. Assume that Fx be an absolutely continuous distribution with the associated pdf fx. The hazard function indicated by hx and corresponding to Fx is defined by

hx=fx1FxforxsupportofF.

The hazard function (hx) of a twice differentiable distribution function (Fx) is known to satisfy the first-order differential equation

(2.2) fxfx=hxhxhx(2.2)

The Proposition 2 that follows offers a non-trivial characterization of the Odd Kappa-G distribution, which does not have the trivial form given in Equation (2.2).

Proposition 2. Assume X:ΩR be a continuous random variable. For α=1, the pdf of X is (1.4) if and only if its hazard function hx satisfies the differential equation

hxgxgxhx=θgx2Gxβ1Gxθ×
(2.3) θ+2Gx11+Gxβ1GxθGx1Gx21+Gxβ1Gxθ2(2.3)

Proof. Suppose X has pdf (1.4), then the above differential Equationequation (2.3) clearly holds. Conversely, if the differential Equationequation (2.3) holds, then

ddx[(g(x))1h(x)]=(θβ)ddx[(1[1G(x)]2) (G(x)β[1G(x)])θ1
1+G(x)β1G(x)θ1,

or

hx=θβgx1Gx2Gxβ1Gxθ11+G(x)β1G(x)θ1,

which is the hazard function of the Odd Kappa-G distribution for α=1.

2.3. Characterizations based on the reversed hazard function

Definition 2.4. Assume that Fx be an absolutely continuous distribution with the associated pdf fx. The reversed hazard function indicated by rx and corresponding to Fx is defined by

rx=fxFxforxsupportofF.

The reversed hazard function (rx) of a twice differentiable distribution function (Fx) is known to satisfy the first-order differential equation

(2.4) fxfx=rxrx+rx(2.4)

The following Proposition 3 provides a non-trivial characterization of the Odd Kappa-G distribution, which does not have the simple form provided in Equation (2.4).

Proposition 3. Let X:ΩR be a continuous random variable. For α=1, the pdf of X is (1.4) if and only if its reversed hazard function rx satisfies the differential equation

(2.5) rxgxgxrx=θgx2×2Gx11+Gxβ1GxθθGxβ1GxθGx1Gx21+Gxβ1Gxθ2(2.5)

Proof. let X has pdf (1.4), then the above differential Equationequation (2.5) clearly holds. Conversely, if the differential Equationequation (2.5) holds, then

ddx[(g(x))1r(x)]=θddx[(1G(x)[1G(x)]) [1+(G(x)β[1G(x)])θ]1,

or

rx=θgxGx1Gx1+G(x)β1G(x)θ1,

which is the reversed hazard function of the Odd Kappa-G distribution for α=1.

3. kth Lower record values

Chandler (Citation1952) developed the notion of record values as a model for dependence structure of successive extremes in a sequence of randomly independently and identically generated variables. This indicates that the distribution of system component life-lengths may shift once each component fails. Many real-world applications requiring data relating to economics, sports, weather and life testing problems use record values. Therefore, the statistical analysis of record values has now been extended in many ways. Dziubdziela & Kopociński (Citation1976) proposed the limiting distribution of kth upper record values by observing successive k largest values in a sequence, where k is a positive integer. Many researchers have thought about characterizing distributions using conditional expectation of record values (Al-Shomrani, Citation2016a; Al-Shomrani & Shawky, Citation2016; M. Franco & Ruiz, Citation1996; Hamid Khan et al., Citation2010; López Bláquez & Luis Moreno Rebollo, Citation1997; Manuel Franco & Jose, Citation1997; H. N. Nagaraja, Citation1988a and Al-Shomrani, Citation2016b). Further information on the theory of records and their characterizations and distributional properties can be found in, for example, Ahsanullah (Citation1995, Citation2004), Barry et al. (Citation1998), Deheuvels (Citation1984), H.N. Nagaraja (Citation1988b; Nevzorov (Citation2001) and references therein.

Let Xrk denote the kth lower record value. The pdf fXrkx of the kth lower record value, for k=1,,r, from independently and identically distributed (iid) random variables X1,,Xr from the Odd Kappa-G distribution is given by (Ahsanullah, Citation2004; Barry et al., Citation1998)

fXrkx=krΓrlogFxr1Fxk1fxforr1

By expanding the logarithm function in power series, we obtain

fXrkx=krΓri=11iFx1iir1Fxk1fx

See equation (1.512) on page 53 in the work by Solomonovich Gradshteyn & Moiseevich Ryzhik (Citation2007).

By using the binomial expansion, we have

fXrkx=krΓri=1j=0i1jiijFxjr1Fxk1fx

See equation (1.111) on page 25 in the work by Solomonovich Gradshteyn & Moiseevich Ryzhik (Citation2007). This is the same as

fXrkx=krΓri=1j=01jiijFxjr1Fxk1fx,

since ij=0ifj>i. Therefore,

fXrkx=krΓrj=0i=11jiijFxjr1Fxk1fx.

From which we have

fXrkx=krΓrj=0ajFxjr1Fxk1fx,

where aj=i=11jiij. Then,

fXrkx=krΓrj=0bjFxjFxk1fx,

where

b0=a0r1andforj1,bj=1ja0k=1jkrjakbjk,

See equation (0.314) on page 17 in the work by Solomonovich Gradshteyn & Moiseevich Ryzhik (Citation2007). Therefore,

(3.1) fXrkx=krΓrj=0bjFxj+k1fx.(3.1)

From Proposition 5.1 in the work by Al-Shomrani & Al-Arfaj (Citation2021), we have

(3.2) Fx=p=0wpGxp,(3.2)

and

(3.3) fx=p=0pwpgxGxp1,(3.3)

Substituting (3.2) and (3.3) into (3.1), we obtain

fXrkx=krΓrj=0bjp=0wpGxpj+k1q=0qwqgxGxq1.

From which we have

(3.4) fXrkx=krΓrj=0bjp=0cpGxpq=0qwqgxGxq1.(3.4)

where

c0=w0j+k1andforp1,cp=1pw0m=1pmj+kpwmcpm,

See equation (0.314) on page 17 in the work by Solomonovich Gradshteyn & Moiseevich Ryzhik (Citation2007). Then, from EquationEquation (3.4), we have

(3.5) fXrkx=j,p,q=0φj,p,qhp+qx,(3.5)

where

φj,p,q=krΓrqbjcpwqp+qandhp+qx=p+qgxGxp+q1

EquationEquation (3.5) is the main result of this section. This shows that the pdf of the Odd Kappa-G kth lower record values is a triple linear combination of Exp-G densities. Some properties of the exp-G distributions are discussed by Gupta et al. (Citation1998), Nadarajah & Kotz (Citation2006) and Al-Hussaini & Ahsanullah (Citation2015) among others.

4. Extreme values

Let X1,,Xn be a random sample from the pdf of the Odd Kappa-G distribution as in EquationEquation (1.4) and X=X1++Xn/n denote the sample mean; then, the distribution of nXEX/VarX approaches the standard normal distribution as n by the usual central limit theorem under suitable conditions. In some cases, it is of interest to consider the asymptotic distributions of the extremes of order statistics Mn=maxX1,,Xn and mn=minX1,,Xn. For further information in this topic, see, for instance, Coles (Citation2001), Galambos (Citation1987), Haan & Ferreira (Citation2006), Kotz & Nadarajah (Citation2000), Sidney (Citation1987) and Arnold et al. (Citation2008).

First, suppose that G belongs to the maximal domain of attraction of the Gumbel extreme value distribution (see, Leadbetter et al., Citation2012). Let ωG=supx|Gx<1 be the upper (right) end point of the cdf G. Then, there must exist a strictly positive function, say ρt>0, such that

limtωG1Gt+xρt1Gt=expx

for every xR. Let ωF=supx|Fx<1 be the upper (right) end point of the cdf F. But, using L’Hopital’s rule and assuming ωF=ωG, we have

limtωF1Ft+xρt1Ft=limtωF1+xρtft+xρtft
=limtωG1+xρtgt+xρtgt1Gt+xρt1Gt2×
Gt+xρtGtθ11Gt+xρt1Gt1θ×
αβ1G(t+xρt)αθ+G(t+xρt)αθαβ1G(t)αθ+G(t)αθα+1α×
1G(t+xρt)1G(t)θα+1
=exp(αθx)

for every xR. Hence, it follows that F also belongs to the maximal domain of attraction of the Gumbel extreme value distribution with

limnPrMnan/bnx=expexp(αθx),<x<

for some appropriate choices of the norming constants an and bn>0, where an represents a shift in location and bn represents a change in scale. For instance, it follows from Corollary 1.6.3 in the work by Leadbetter et al. (Citation2012) that the normalizing constants are an=F111/n and bn=ρan>0.

Second, assume that G belongs to the maximal domain of attraction of the Fréchet extreme value distribution (see, Leadbetter et al., Citation2012). Then, ωG= and there must exist a τ>0 such that

limt1Gtx1Gt=xτ

for every x>0. Therefore, ωF=ωG= and by using L’Hopital’s rule, we note that

limt1Ftx1Ft=limtxftxft=limtxgtxgt1Gtx1Gt2×
GtxGtθ11Gtx1Gt1θ×
αβ1G(tx)αθ+G(tx)αθαβ1G(t)αθ+G(t)αθα+1α1G(tx)1G(t)θα+1×
=xαθτ

for every x>0. So, it follows that F also belongs to the maximal domain of attraction of the Fréchet extreme value distribution with

limnPrMnan/bnx=expxαθτ,x>0

for some appropriate choices of the norming constants an and bn>0. For example, it follows from Corollary 1.6.3 in the work by Leadbetter et al. (Citation2012) that the normalizing constants are an=0 and that bn>0 satisfies 1Fbn1/n.

Third, Let G belong to the maximal domain of attraction of the Weibull extreme value distribution (see, Leadbetter et al., Citation2012). Then, ωG< and there must exist a ϕ>0 such that

limt01GωGtx1GωGt=xϕ

for every x<0. Then, since ωF=ωG< and by using L’Hopital’s rule, we have

limt01FωFtx1FωFt
=limt0xfωFtxfωFt
=limt0xgωGtxgωGt1GωGtx1GωGt2×
GωGtxGωGtθ11GωGtx1GωGt1θ×
αβ1G(ωGtx)αθ+G(ωGtx)αθαβ1GωGtαθ+GωGtαθα+1α×
1G(ωGtx)1GωGtθα+1=xθϕ

for every x<0. Hence, it follows that F also belongs to the maximal domain of attraction of the Weibull extreme value distribution with

limnPrMnan/bnx=expxθϕ,x<0

for some suitable choices of the norming constants an and bn>0. For instance, it follows from Corollary 1.6.3 in the work by Leadbetter et al. (Citation2012) that the normalizing constants are an=ωF=F1(1) and bn=ωFF111/n>0.

Similar arguments can be obtained for minimal domains of attraction. That is, F belongs to the same minimal domain of attraction as that of G. For instance, since the normal distribution belongs to the maximal/minimal domain of attraction of the Gumbel extreme value distribution, it follows that the Odd-Kappa normal distribution also belongs to the maximal/minimal domain of attraction of the Gumbel extreme value distribution.

5. FGM copula

Copulas were introduced by Roger (Citation2006) as a function that combines multivariate distribution functions with uniform [0,1] margins. Sklar (Citation1996) defined the cdf and pdf for two-dimensional copulas as follows: given two random variables X and Y with, respectively, distribution functions F(x) and F(y), the cdf and pdf for bivariate copulas were provided, respectively, as

(5.1) Fx,y=CFx;ϑ1,Fy;ϑ2,(5.1)

and

(5.2) fx,y=fx;ϑ1fy;ϑ2cFx;ϑ1,Fy;ϑ2,(5.2)

where x,y,×, and ϑ1 is a parameter vector for the first variable X, and ϑ2 is a parameter vector for the second variable Y. Moreover, the sf for bivariate copulas was defined by Roger (Citation2006) as

Sx,y=CˆFx,Fy
(5.3) =Fx;ϑ1+Fy;ϑ21+C1Fx;ϑ1,1Fy;ϑ2.(5.3)

From Sklar’s theorem and using EquationEquation (5.1)-(Equation5.3) and Odd Kappa-G family EquationEquation (1.3)-(Equation1.5), we get the joint cdf, pdf and sf of bivariate Odd Kappa-G family based on any copula function, respectively, as the following:

(5.4) Fx,y=CG(x;ϑ1)β11G(x;ϑ1)α1θ1α1+G(x;ϑ1)β11G(x;ϑ1)α1θ11α1,G(y;ϑ2)β21G(y;ϑ2)α2θ2α2+G(y;ϑ2)β21G(y;ϑ2)α2θ21α2,(5.4)
fx,y=α1θ1gx;ϑ1β11Gx;ϑ12Gx;ϑ1β11Gx;ϑ1θ11×
α1+G(x;ϑ1)β11G(x;ϑ1)α1θ1α1+1α1α2θ2gy;ϑ2β21Gy;ϑ22×
Gy;ϑ2β21Gy;ϑ2θ21α2+G(y;ϑ2)β21G(y;ϑ2)α2θ2α2+1α2×
(5.5) cG(x;ϑ1)β11G(x;ϑ1)α1θ1α1+G(x;ϑ1)β11G(x;ϑ1)α1θ11α1,G(y;ϑ2)β21G(y;ϑ2)α2θ2α2+G(y;ϑ2)β21G(y;ϑ2)α2θ21α2,(5.5)

and

Sx,y=1Gx;ϑ1β11Gx;ϑ1α1θ1α1+Gx;ϑ1β11Gx;ϑ1α1θ11α1G(y;ϑ2)β21G(y;ϑ2)α2θ2α2+G(y;ϑ2)β21G(y;ϑ2)α2θ21α2+
(5.6) CG(x;ϑ1)β11G(x;ϑ1)α1θ1α1+G(x;ϑ1)β11G(x;ϑ1)α1θ11α1,G(y;ϑ2)β21G(y;ϑ2)α2θ2α2+G(y;ϑ2)β21G(y;ϑ2)α2θ21α2(5.6)

Many copulas, such as Farlie-Gumbel-Morgenstern (FGM), have been defined using EquationEquation (5.1)-(Equation5.3). The FGM copula is one of the most well-known parametric families of copulas explored by Gumbel (Citation1960), Morgenstern (Citation1956) and Farlie (Citation1960). In addition, it is considered to be the most effective in describing quantity dependence. Sriboonchitta & Kreinovich (Citation2018), Almetwally (Citation2019) and El-Sherpieny et al. (Citation2021) discussed the FGM copula in order to introduce the bivariate Weibull distribution.

For the FGM copula, we know that its copula function and the associated copula density are, respectively

(5.7) CFx;ϑ1,Fy;ϑ2=Fx;ϑ1Fy;ϑ21+ρ1Fx;ϑ11Fy;ϑ2,(5.7)

and

(5.8) c(F(x;ϑ1),F(y;ϑ2))=1+ρ[(12F(x;ϑ1))(12F(y;ϑ2)),(5.8)

where 1ρ1. Note that, if ρ=0, then X and Y are independent.

Using the FGM copula function given in EquationEquation (5.7) and (Equation5.8) and the bivariate Odd Kapp-G family based on any copula function in EquationEquation (5.4)-(Equation5.6), we get the bivariate cdf, pdf and sf of the Odd Kapp-G (BFGMOKG) family based on FGM copula as follows:

FBFGMOKGx,y=G(x;ϑ1)β11G(x;ϑ1)α1θ1α1+G(x;ϑ1)β11G(x;ϑ1)α1θ11α1G(y;ϑ2)β21G(y;ϑ2)α2θ2α2+G(y;ϑ2)β21G(y;ϑ2)α2θ21α2×
1+ρ1G(x;ϑ1)β11G(x;ϑ1)α1θ1α1+G(x;ϑ1)β11G(x;ϑ1)α1θ11α1×
1G(y;ϑ2)β21G(y;ϑ2)α2θ2α2+G(y;ϑ2)β21G(y;ϑ2)α2θ21α2,
fBFGMOKGx,y=α1θ1gx;ϑ1β11Gx;ϑ12Gx;ϑ1β11Gx;ϑ1θ11
α1+G(x;ϑ1)β11G(x;ϑ1)α1θ1α1+1α1α2θ2gy;ϑ2β21Gy;ϑ22×
Gy;ϑ2β21Gy;ϑ2θ21α2+G(y;ϑ2)β21G(y;ϑ2)α2θ2α2+1α2×
1+ρ12G(x;ϑ1)β11G(x;ϑ1)α1θ1α1+G(x;ϑ1)β11G(x;ϑ1)α1θ11α1×
(24) 12G(y;ϑ2)β21G(y;ϑ2)α2θ2α2+G(y;ϑ2)β21G(y;ϑ2)α2θ21α2,(24)

and

SBFGMOKGx,y=1
Gx;ϑ1β11Gx;ϑ1α1θ1α1+Gx;ϑ1β11Gx;ϑ1α1θ11α1Gy;ϑ2β21Gy;ϑ2α2θ2α2+Gy;ϑ2β21Gy;ϑ2α2θ21α2+
Gx;ϑ1β11Gx;ϑ1α1θ1α1+Gx;ϑ1β11Gx;ϑ1α1θ11α1Gy;ϑ2β21Gy;ϑ2α2θ2α2+Gy;ϑ2β21Gy;ϑ2α2θ21α2×
1+ρ1Gx;ϑ1β11Gx;ϑ1α1θ1α1+Gx;ϑ1β11Gx;ϑ1α1θ11α1×
1Gy;ϑ2β21Gy;ϑ2α2θ2α2+Gy;ϑ2β21Gy;ϑ2α2θ21α2.

The bivariate pdf of the BFGMOKG family given in Equation (5.9) has Odd Kappa-G family marginals. The marginal density functions for X and Y, respectively, are

fx;α1,β1,θ1,ϑ1=α1θ1gx;ϑ1β11Gx;ϑ12Gx;ϑ1β11Gx;ϑ1θ11
α1+G(x;ϑ1)β11G(x;ϑ1)α1θ1α1+1α1

and

fy;α2,β2,θ2,ϑ2=α2θ2gy;ϑ2β21Gy;ϑ22Gy;ϑ2β21Gy;ϑ2θ21
α2+G(y;ϑ2)β21G(y;ϑ2)α2θ2α2+1α2.

The conditional cdf and pdf of X given Y, respectively, are

Fx|y=G(x;ϑ1)β11G(x;ϑ1)α1θ1α1+G(x;ϑ1)β11G(x;ϑ1)α1θ11α1×
1+ρ1G(x;ϑ1)β11G(x;ϑ1)α1θ1α1+G(x;ϑ1)β11G(x;ϑ1)α1θ11α1×
12G(y;ϑ2)β21G(y;ϑ2)α2θ2α2+G(y;ϑ2)β21G(y;ϑ2)α2θ21α2

and

fx|y=α1θ1gx;ϑ1β11Gx;ϑ12Gx;ϑ1β11Gx;ϑ1θ11×
α1+G(x;ϑ1)β11G(x;ϑ1)α1θ1α1+1α1×
1+ρ12G(x;ϑ1)β11G(x;ϑ1)α1θ1α1+G(x;ϑ1)β11G(x;ϑ1)α1θ11α1×
12G(y;ϑ2)β21G(y;ϑ2)α2θ2α2+G(y;ϑ2)β21G(y;ϑ2)α2θ21α2.

Similarly, the conditional cdf and pdf of Y given X, respectively, are

Fy|x=G(y;ϑ2)β21G(y;ϑ2)α2θ2α2+G(y;ϑ2)β21G(y;ϑ2)α2θ21α2×
1+ρ1G(y;ϑ2)β21G(y;ϑ2)α2θ2α2+G(y;ϑ2)β21G(y;ϑ2)α2θ21α2×
12G(x;ϑ1)β11G(x;ϑ1)α1θ1α1+G(x;ϑ1)β11G(x;ϑ1)α1θ11α1

and

fy|x=α2θ2gy;ϑ2β21Gy;ϑ22Gy;ϑ2β21Gy;ϑ2θ21×
α2+G(y;ϑ2)β21G(y;ϑ2)α2θ2α2+1α2×
1+ρ12G(x;ϑ1)β11G(x;ϑ1)α1θ1α1+G(x;ϑ1)β11G(x;ϑ1)α1θ11α1×
12G(y;ϑ2)β21G(y;ϑ2)α2θ2α2+G(y;ϑ2)β21G(y;ϑ2)α2θ21α2.

Some measures of dependence were presented by Roger (Citation2006). One of these is Kendall’s tau correlation (τ), which is defined as the difference between the probabilities of concordance and discordance, given in terms of any copula function as

τ=4ECU,V1=40101Cu,vcu,vdudv1

Using FGM copula function, Kendall’s tau correlation (τ) is

τ=40101Cu,v1+ρ12u12vdudv1=49+2ρ361=2ρ9.

The other one is the median regression curve of Y on X, which is a method for describing the dependence of one random variable on another, for any copula as follows:

PrYy|X=x=Fy|x=CFx,FyFx=12.

By using FGM copula function, the median regression model of BFGMOKG family is as the following:

12=PrYy|X=x=Gy;ϑ2β21Gy;ϑ2α2θ2α2+Gy;ϑ2β21Gy;ϑ2α2θ21α2×
1+ρ1Gy;ϑ2β21Gy;ϑ2α2θ2α2+Gy;ϑ2β21Gy;ϑ2α2θ21α2×
12Gx;ϑ1β11Gx;ϑ1α1θ1α1+Gx;ϑ1β11Gx;ϑ1α1θ11α1.

Let u=Fx=Gx;ϑ1β11Gx;ϑ1α1θ1α1+Gx;ϑ1β11Gx;ϑ1α1θ11α1 and v=Fy=Gy;ϑ2β21Gy;ϑ2α2θ2α2+Gy;ϑ2β21Gy;ϑ2α2θ21α2. After simplifications, we have

v=1+ρ24uρ2+4ρ2u2+2ρuρ12ρ2u1

Thus, the median regression curve of V on U is the line in I2 connecting the points 1,ρ1+1+ρ22ρ and 0,1+ρ1+ρ22ρ. Furthermore, the median regression line is v=2u24u+4u222u1 when ρ=1, and v=2u1+24u+4u222u1 when ρ=1. Moreover, the slope of the median regression line is 1+1+ρ2ρ. As an illustration, see .

Figure 1. Plots of slope and regression curve of V on U of BFGMOKG family.

Figure 1. Plots of slope and regression curve of V on U of BFGMOKG family.

6. Concluding remarks

In this research paper, more mathematical properties of Odd Kappa-G family are introduced. We study some characterization results of the Odd Kappa-G family including characterizations based on two truncated moments, hazard and reversed hazard functions. We present the kth lower record values of the Odd Kappa-G family. Extreme values for this family are discussed. The bivariate cdf, pdf and sf of the Odd Kappa-G family based on FGM copula are obtained. Finally, we hope that this paper will encourage more researchers to study this attractive new family of distributions and inspire practitioners to apply it in their fields.

Data Availability

Data sharing not applicable to this article as no real data set was analyzed during the current study.

Acknowledgements

The author would like to thank the editor and anonymous referees for their insightful comments that helped to enhance the paper.

Disclosure statement

No potential conflict of interest was reported by the author.

Additional information

Funding

The author received no direct funding for this research.

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