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A New Frailty Model Based Archimedean Bivariate Copula That Models Only Positive Dependency

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21 April 2025

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21 April 2025

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Abstract
In this paper, the author utilizes the frailty model to construct a new Archimedean copula. This copula depends on the transformed Median Based Unit Rayleigh (MBUR) distribution to unbounded distribution defined on the interval from zero to infinity. The copula only models the positive dependency. In the paper, the joint PDF and CDF of the copula are derived for two bivariate distributions. The singularity of the copula is explained. The generator and inverse generator of the new copula are explored with various graphs to depict the decreasing and convex nature of the generator with different dependency parameter values. The Kendall tau measure of dependency is derived. For this copula, the lower and upper tail dependencies exist. The formula for each one is derived. This new copula is one of the parametric Archimedean copulas. Unfortunately, the Archimedean copulas are not widely used.
Keywords: 
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Introduction

A copula is a function mapping 0,1 2   0,1 and satisfying the boundary condition in the form of C u , 0 = C 0 , v = 0     u   &   v   0,1 , the unit marginal conditions in the form of C 1 , v = v   &   C u , 1 = u     u   &   v     0,1   , and 2-increasing property that states,
u , u ' , v , v ' 0,1   a n d   u u '   a n d   v v ' then,
C u , u ' × v , v ' = C u ' , v ' C u , v ' C u ' , v + C u ' , v ' 0
C u , v C u ' , v and C u , v C u , v ' for u u '   a n d   v v ' , hence satisfying Lipschitz condition that is
C u , v C u ' , v ' u u ' + v v ' u , u ' , v , v ' 0,1
Sklar (Sklar, 1973) showed that a copula exists for any multivariate distribution, such that the joint distribution equals the copula applied to the marginal. In other words, Let X and Y be random variables with joint distribution H and marginal distribution functions F   and G , respectively. Then there is a uniquely determined copula, C, on the R a n g e   F × R a n g e   G , such that H x , y = C F x , G y for   x , y     ,   . So copulas connect joint distributions functions to their margins. They are crucial for constructing bivariate and multivariate distributions because they are a statistical method for studying scale-free measures of dependence.
Definition 1
(Sklar’s theorem 1): For any bivariate distribution function H with marginal F
and G , there exists a copula such that
H x , y = C F x , G y   ,   x , y ,
If H is continuous, then the copula C is unique. Otherwise, it is uniquely determined on the F R × G R . The converse is also true, for any copula and univariate distribution functions F and G , the function C F x , G y   is a bivariate distribution function with margins F and G .
Definition 2
: A bivariate Archimedean copula C ( u , v ) can be written in the form of C u , v = φ 1 φ u + φ v with marginal u = F X ( x ) and v = F Y ( y ) , where φ u is the generator function being continuous, strictly decreasing and convex function mapping [ 0,1 ] onto [ 0 , ) , in other words, φ ' u < 0   , decreasing) and φ ' ' u > 0 (convex), φ 0 = , and → φ1=0
Definition 3
: a bivariate copula has C u , v u v = c ( u , v ) which is the joint PDF of the copula.
So the copula links the marginal distributions through the dependency parameter.
The singular part of the copula is defined by (Genest & Mackay, 1986) in the following Theorem, the ratio between the generator and the first derivative of the generator evaluated at zero does not equal zero.
Theorem 
: the distribution C ( u , v ) generated by φ has a singular component iff φ 0 φ ' 0 0 in that case, φ u + φ v = φ 0 with probability = φ 0 φ ' 0
In the last few years many models have been proposed for copulas. The applications of copulas are too plentiful to list so further improvements of copulas are encouraged to be further advanced. The applied applications rely mainly on the parametric models for copulas in comparison to the semi-parametric and non-parametric model for copulas which have limited applied implementations in real life.
Many eminent scientists and authors had in depth papers discussing the estimation methods, simulation, probabilistic interpretations, and analytical properties. Many problems face the statistical scientific community and in need for solutions. (Nadarajah et al., 2018) mentioned some of these problems like estimation of copula under misspecification, copula density estimation, Bayesian copula, change point estimation of copulas, efficient estimation and simulation algorithms, characterization of copulas, selection criteria between two or more copulas, time series models constructed on copulas, bounds for copulas, copula calibration, transformations to enhance fits of copulas, extreme value manners of bivariate and multivariate copulas, compatibility of copulas, additional measures of asymmetry for bivariate and multivariate copulas, extra tests for symmetry for bivariate and multivariate copulas, time varying copulas, space changing copulas and copulas fluctuating with sense of both time and space.
Many books had been written by pioneer and innovator scientists in the field of copulas like books written by (Drouet-Mari & Kotz, 2001), (Cuadras et al., 2002), (Cherubini et al., 2004), (Genest, 2005a), (Genest, 2005b), (Nelson, 2006), (McNeil et al., 2005), (Alsina et al., 2006), (Mai & Scherer, 2014), (Durante & Sempi, 2015), (Salvadori et al., 2007), (Malevergne & Sornette, 2006), (Schweizer & Sklar, 2005), (Jaworski et al., 2010),(Jaworski et al., 2013), (Joe, 2014), (Joe, 1997)and many others. Numerous papers had been published by many prominent scientists like (Nelsen, 2002), (Embrechts et al., 2003), (Manner & Reznikova, 2012), (Patton, 2012),(Genest et al., 2009),(Schweizer, 1991), (Kolev et al., 2006), (Kolev & Paiva, 2009), and (Frees & Valdez, 1998).
The copula can be grouped into five subgroups which are the Archimedean copulas, the elliptical copulas, the Eyraud-Farlie-Gumbel-Morgenstern (EFGM) copula, extreme value copulas, and other copulas. Each of these subgroups includes more copulas. For more details, the reader can be referred to the paper of (Nadarajah et al., 2018) and references therein.
The simplest copula is the product copula or the independence copula C u , v = u v . It is for two independent random variables with H x , y = F x G y . The other two very essential dependencies between two variables are the perfect positive and the perfect negative dependencies. These can be expressed by copulas. For the positive state, this yields M u , v = m i n u , v . Hence, for random variables X and Y with distributions F , G and the joint distribution M F x , G y , and because the copula is symmetric, the random variable X is an increasing function of Y and vice versa. The converse, with decreasing instead of increasing holds true for the joint distribution function W F , G with W u , v = m a x u + v 1 . This one is also a copula. These boundaries are themselves copulas and they are called Frechet-Hoeffding upper and lower bound respectively. As long as both M and W are not differentiable in u and v, they have no density functions. Joe (Joe, 1990), (Joe & Hu, 1996), (Joe, 1993) developed copulas that allow for positive dependency only. These copulas are recently used in portfolio risk analysis with Asian equity markets (Ozun & Cifter, 2007).
This paper is structured in 6 sections. Section 1 discusses the methodology of derivation. section 2 illustrates the generator and its properties. Section 3 explores the inverse generator and its properties. Section 4 explains the Kendal Tau measure of dependency. Section 5 enlightens how the copula can model both lower and upper tail dependencies. Section 6 elucidates the final conclusions and future works. Numerous figures for its PDF and CDF are depicted.

1. Methodology of Derivation

This copula depends on the frailty method for generating the copula. Assuming two individuals have survival time distributed as exponential T 1 and T 2 . They have exponential baseline hazard function with λ 1 = λ 2 = 1 . The survival function is shown in equation (1) and the hazard function in equation (2)
S t = P r o b T > t = 1 F t
h t = ln S t   t = F t S t
The Cox proportional hazard model uses the hazard function as shown in equation (3)
t , Z = e β Z   b t
where the Z are the explanatory variables in survival analysis and b(t) is the baseline hazard function. And B is the vector of regression coefficients. It is proportional because all information is contained in the multiplicative factor γ = e B Z , this is called the frailty model when some explanatory variables (Z) and hence the factor γ are unobserved. And the factor γ is called the frailty parameter. Integrating and exponentiating the negative hazard
λ = e β 0 + β 1 Z 1 + β 2 Z 2 = e β 0   e β 1 Z 1 + β 2 Z 2 = λ 0 e β 1 Z 1 + β 2 Z 2 for 2 explanatory variables for example
S t | γ = e x p 0 t ln S t t d t = e x p 0 t h t d t = e x p 0 t λ d t e x p 0 t e β 0 + β 1 Z 1 + β 2 Z 2 d t = e x p 0 t e β 0 γ d t = e x p γ 0 t e β 0 d t e γ 0 t e β 0 d t = e 0 t λ 0 d t γ = e t λ 0 γ   w h e r e   e β 0 = λ 0   a s s u m e   λ 0 = 1 B t γ   w h e r e   B t i s   t h e   b a s e l i n e   h a z a r d , to sum up e t λ 0 γ = e S 0 t γ = e t γ = S t | γ
The marginal distribution for a single life time T is obtained by taking expectation over the potential values of γ that is E e t γ , assuming the f γ is the PDF of the frailty variable so
E e t γ = 0 e t γ   f γ d γ  
Let y be a random variable distributed as Median Based Unit Rayleigh (BMUR) (Attia, M.I., 2024), transform this variable to be defined on the interval from zero to infinity as shown below. The PDF of the Median Based Unit Rayleigh (MBUR) is shown in equation (4)
6 α 2   1 y 1 α 2 y 2 α 2 1 ,   0 < y < 1 ,   α > 0
The following transformation will be applied to the above PDF:
Let w = ln y 1 α 2 w = ln y α 2 w α 2 = ln y y = e α 2 w
The Jacobian is shown in equation (5) d y = e α 2 w α 2 d w . . ( 5 )
Replace the transformation of equation (5) into equation (4) as shown in equation (6):
0 6 α 2 1 e α 2 w 1 α 2 e α 2 w 2 α 2 e α 2 w 1 α 2 e α 2 w d w 0 6 1 e α 2 w α 2 e 2 α 2 w α 2 d w
f W w = 6 1 e w e 2 w
Now this w is the frailty variable   γ which is distributed as unbounded MBUR defined on the interval 0 , . Now take the conditional expectation of the survival function of the time distributed as exponential random variable with hazard rate equal one (scale parameter or lambda=1) given the frailty variable as shown in equation (7)
E e t γ = 0 e t γ f γ d γ = 0 e t γ 6 1 e γ e 2 γ d γ = 6 0 e γ t + 2 d γ 6 0 e γ t + 3 d γ = 6 e γ t + 2 t + 2 0 6 e γ t + 3 t + 3 0 = 6 1 t + 2 1 t + 3 E e t γ = E S ( t | γ ) = 6 t + 2 t + 3 = 6 t 2 + 5 t + 6
We can think of this expectation as a function of the frailty variable, it is averaging the probability to survive beyond specific time given that frailty. It is the expectation of a function of the frailty not the variable frailty itself so this function which is the baseline survival function should be multiplied by the PDF of the frailty variable. This way the frailty variable is integrated out. So this expectation is considered as the joint CDF of the two random variables T1 and T2. How to get this time? By inverting this expectation as shown in equation (8). Let us call this expectation u then solving second degree polynomial to get its root.
u = 6 t 2 + 5 t + 6 6 u = t 2 + 5 t + 6 t 2 + 5 t + 6 6 u = 0 t = 5 + 25 4 ( 1 ) 6 1 1 u 2 = 5 + 25 24 1 1 u 2 t = 5 + 25 24 + 24 u 2 = 5 + 1 + 24 u 2

2. The Generator

In previous work by Iman M. Attia (Attia, 2025), the generator obtained by this method (modeling the frailty variable) yielded a Kendall tau measure that is fixed. As shown here the same method with different re-parameterization yielded a generator with no dependency parameter; therefore, the author did some manipulations to enhance the Kendall tau measures. The author added dependency parameter and remove the denominator as shown in the following equation (9), u is the marginal CDF.
t = θ 5 + 1 + 24 u 1 2 1 θ ,   0 < u < 1
This (t) is the generator and (u) is the inverse generator. So the time (t) is a function of (u)
Preposition 1
: the generator shown in equation (9), t = θ 5 + 1 + 24 u 1 2 1 θ can be considered as a generator for this new Archimedean copula.
Proof 
: The generator fulfills the sufficient conditions of a generator.
1)
φ 0 = θ 5 + 1 + 24 0 1 2 1 θ =
2)
φ 1 = θ 5 + 1 + 24 1 1 2 1 θ = 0
3)
φ ' u = 5 + 1 + 24 u 1 2 1 θ 1   1 + 24 u 0.5   12 u 2 < 0
This ensures that the generator is a decreasing function in u.
4)
φ ' ' u = 1 θ 1 5 + 1 + 24 u 1 2 1 θ 2   1 + 24 u 1   12 u 2 2 + 5 + 1 + 24 u 1 2 1 θ 1 1 2 1 + 24 u 1.5 12 u 2 2 + 5 + 1 + 24 u 1 2 1 θ 1 1 + 24 u 0.5 24 u 3 > 0
This ensures that the generator is a convex function at 0 < θ   1
For bivariate distribution with uniform marginal CDF (u) and (v), the generators are shown in equations (10-12)
φ u = θ 5 + 1 + 24 u 1 2 1 θ
φ v = θ 5 + 1 + 24 v 1 2 1 θ
φ w = φ u + φ v = θ 5 + 1 + 24 u 1 2 1 θ + θ 5 + 1 + 24 v 1 2 1 θ ) φ w = θ 5 + 1 + 24 u 1 2 1 θ + 5 + 1 + 24 v 1 2 1 θ

3. The Inverse Generator

To get the inverse generator of this modified generator, the author inverts this (t) as shown in equation (13), as long as t equals:
t = φ u = θ 5 + 1 + 24 u 1 2 1 θ   ,   0 < θ 1 u = φ 1 u = 24 t θ θ + 5 2 1 = 24   t θ θ + 5 2 1 1 ,   0 < θ 1
Recall that C φ u + φ v = φ 1 φ u + φ v
As a valid bivariate Archimedean copula can be expressed as C ( u , v ) = C ( F X ( x ) , F Y ( y ) )
Proposition 2
: The copula expressed in equation (13) can be assumed to be a valid copula as it fulfills the boundary conditions, the marginal uniformity and 2- increasing conditions. And this is equivalent to the necessary conditions of the inverse generator to be fulfilled which are the following:
Proof: 
C 0 , v = C u , 0 = 0 , boundary conditions are fulfilled
C 0 , v = 24   θ 5 + 1 + 24 0 1 2 1 θ + 5 + 1 + 24 v 1 2 1 θ θ θ + 5 2 1 1 = 0
C 1 , v = v   a n d   C u , 1 = u , the marginal uniformity, when u=1
C 1 , v = 24   θ 5 + 1 + 24 1 1 2 1 θ + 5 + 1 + 24 v 1 2 1 θ θ θ + 5 2 1 1 = v C 1 , v = 24   5 + 1 + 24 1 1 2 1 θ + 5 + 1 + 24 v 1 2 1 θ θ + 5 2 1 1 C 1 , v = 24   5 + 1 + 24 v 1 2 1 θ θ + 5 2 1 1 C 1 , v = 24   5 + 1 + 24 v 1 2 + 5 2 1 1 = 24     1 + 24 v 1 2 2 1 1 C 1 , v = 24   1 + 24 v 1 1 = 24   24 v 1 = v
The same is true for v, if v=1 so C u , 1 = 24   24 v 1 = v
Proposition 3
: This is a valid copula as it is 2-increasing, i.e., 2 C u , v u v 0 in equation (14)
Proof: 
Let
p = 5 + 1 + 24 u 1 2   a n d   q = 5 + 1 + 24 v 1 2 C u , v u = 48 p 1 θ + q 1 θ θ + 5 2 1 2 p 1 θ + q 1 θ θ + 5 p 1 θ + q 1 θ θ 1 p 1 θ 1 1 + 24 u 1 2 12 u 2 v C u , v u = 2 C u , v u v = = 48 144 u 2 v 2 p q 1 θ 1 1 + 24 u 1 + 24 v 1 2 p 1 θ + q 1 θ θ + 5 2 1 2 p 1 θ + q 1 θ θ 2 × 4 p 1 θ + q 1 θ θ + 5 2 1 1 p 1 θ + q 1 θ θ + 5 2 p 1 θ + q 1 θ θ + p 1 θ + q 1 θ θ + p 1 θ + q 1 θ θ + 5 θ 1 θ   0   ,   0 < θ 1  
Proposition 4
: This copula is absolutely continuous copula and it has no singular part.
Proof: 
to test for singularity: lim u 0 φ 0 φ ' 0 = 0 in equation (15). If this limit is zero so the copula has no singular part.
φ u φ ' u =   θ 5 + 1 + 24 u 1 2 1 θ   θ 1 θ 5 + 1 + 24 u 1 2 1 θ 1 1 2 1 + 24 u 0.5 24 u 2 lim u 0 φ u φ ' u = θ 12 5 + 1 + 24 u 1 2 1 + 24 u 0.5 u 2 l i m u 0   5 θ   24 + u u 0.5 u 2 12 + l i m u 0   θ 24 + u u u 2 12 l i m u 0   5 θ u + 24 0.5 u 1.5 12   + l i m u 0   θ u 24 + u 12 = 0 0 = 0
As long as this limit is zero at u=0 so the copula has no singular part and it is absolutely continuous copula.

4. Kendall Tau Measure of Dependency

Proposition 5
: Kendall tau for this copula is τ = 1 0.797   θ in equation (16)
Proof: 
τ = 4   0 1 φ u φ ' u d u + 1 0 1 φ u φ ' u   d u = 0 1 5 θ u + 24 0.5 u 1.5 12   + θ u 24 + u 12   d u = = 5 θ 12 0 1 u + 24 0.5 u 1.5   d u + θ 12 0 1   24   u + u 2   d u = = 5 θ 12 0.8286 θ 12 12 + 1 3 = 0.1992 θ τ = 4   0 1 φ u φ ' u d u + 1 = 4   0.1992   θ + 1 = 1 0.797   θ
For this copula, new one can be created using the following pattern for the generator:
t = φ u = θ 5 + 1 + 24 u 1 2 1 θ = θ k + 1 + h u 1 2 1 θ
Let the 1 + h   = k so other generators can be created and hence related new copulas for each generator such as:
t 1 = φ u = θ 2 + 1 + 1 u 1 2 1 θ t 2 = θ 6 + 1 + 35 u 1 2 1 θ t 3 = θ 100 + 1 + 9999 u 1 2 1 θ
But the Kendall Tau measure of dependency calculation will be
2   k   θ h 0 1 u + 24 0.5 u 1.5   d u + 2   θ h 0 1   24   u + u 2   d u =
For large values of h the first part of integration will converge to 0.8001 and when added to the second part, the final result will converge to 0.1999 , when h attains large values so the Kendall tau measure of dependency will be
τ = 4 0.1999 θ + 1 = 1 0.8 θ for large values of h
Figure 1, Figure 2, Figure 3, Figure 4, Figure 5, Figure 6, Figure 7, Figure 8, Figure 9, Figure 10, Figure 11, Figure 12, Figure 13, Figure 14, Figure 15, Figure 16, Figure 17, Figure 18, Figure 19, Figure 20, Figure 21, Figure 22, Figure 23, Figure 24, Figure 25, Figure 26, Figure 27, Figure 28, Figure 29 and Figure 30 illustrate the joint PDF, the joint CDF and the related generator for the copula with different values of dependency parameter.

5. Tail Dependency

Preposition 6:
Lower and upper tail dependencies for this copula exist.
Proof: 
λ U = lim u 1 1 2 u + C u , u 1 u   =
λ U = lim u 0 C u , u u =
φ ' 0 = 5 + 1 + 24 u 1 2 1 θ 1   1 + 24 u 0.5   12 u 2 =
Since both limits in equation (17-18) are infinite and as illustrated in Figure 3) so both lower and upper tail dependencies exist. Moreover, as shown in equation (19) and in Figure 32 the first derivative of the generator approaches at u = 0 so the upper tail dependency exists.
Preposition 7
: The values of lower and upper tail dependency can be calculated as shown in equations (20-21)
λ U = 2 2 . lim u 0   φ ' 2 u φ ' u = 2 2 1 θ + 2
λ L = 2 2 . lim u 0   φ ' u φ ' 2 u = 2 1 2   2 1 θ 2
Proof: 
Lower tail dependency:
lim u 0   φ ' u φ ' 2 u = l i m u 0   5 + 1 + 24 u 1 2 1 θ 1   1 2 1 + 24 u 0.5   24 u 2 5 + 1 + 24 2 u 1 2 1 θ 1   1 2   1 + 24 2 u 0.5   24 2 u 2 lim u 0   φ ' u φ ' 2 u = 5 + 1 + 24 u 1 2 1 θ 1   1 + 24 u 0.5   24 u 2 5 + 1 + 12 u 1 2 1 θ 1   1 + 12 u 0.5   12 u 2 1 + 24 u 1 2   24 u 1 2   f o r   u 0,1 lim u 0   φ ' u φ ' 2 u = 5 + 24 u 1 2 1 θ 1   u 24   2 5 + 12 u 1 2 1 θ 1   u 12   = lim u 0 2   12 24   5 u + 24 u 5 u + 12 u 1 θ 1 = lim u 0   2 12 24   5 0 + 24 5 0 + 12 1 θ 1 = = 2   1 2   2 1 θ 1 = 2 2   2 1 θ 1 = 2   2 1 θ 2 λ L = 2 2 . lim u 0   φ ' u φ ' 2 u = 2 2 2   2 1 θ 2 = 2 1 2   2 1 θ 2
Upper tail dependency
lim u 0   φ ' 2 u φ ' u = l i m u 0   5 + 1 + 24 2 u 1 2 1 θ 1   1 2   1 + 24 2 u 0.5   24 2 u 2 5 + 1 + 24 u 1 2 1 θ 1   1 2 1 + 24 u 0.5   24 u 2 lim u 0   φ ' 2 u φ ' u = l i m u 0   5 + 1 + 24 2 u 1 2 1 θ 1   1 + 12 u 0.5   12 u 2 5 + 1 + 24 u 1 2 1 θ 1   1 + 24 u 0.5   24 u 2
As long as u is small 1 + 24 u 1 2 24 u 1 2 f o r u 0,1
l i m u 0   5 + 24 2 u 1 2 1 θ 1   12 u 0.5   12 5 + 24 u 1 2 1 θ 1   24 u 0.5   24 = l i m u 0   5 + 12 u 1 θ 1   u 12   12 5 + 24 u 1 θ 1   u 24   24 = l i m u 0   5 u + 12 u 5 u + 24 u 1 θ 1   2   1 2 = l i m u 0   5 0 + 12 5 0 + 24 1 θ 1   2   1 2 =   12   24 1 θ 1   2   1 2 = 2 2   12 24 1 θ 1 = 2 2   1 2 1 θ 1 = 2 2   2 1 θ + 1 = 2 1 θ + 2 2 λ U = 2 2 . lim u 0   φ ' 2 u φ ' u = 2 2 2 1 θ + 2 2 = 2 2 1 θ + 2

6. Conclusions

This copula which is based on frailty model and cox proportional hazard model can only model positive dependency. These types of copula can be used in applications to model the positive dependency between variables. This copula can also model lower and upper tail dependency. This copula has a generator whose derivative is zero when evaluated at zero and this supports modeling upper tail dependency. The definitions of lower and upper tail dependencies that involve the copula equation yielded infinite values and this also supports the tail dependencies.
While the joint distribution function, H x , y = C F x , G y   for two random variables X and Y, the bivariate density function these 2 variables is shown in equation (22)
h X , Y x , y = H x , y x y = f X x f Y y c F X x , F Y y = f X x f Y y 2 C u , v u v

Future Works

More works are needed to develop efficient estimation and simulation algorithms. Also Bayesian estimation can be used to enhance the estimation procedures. The copula can also be tested for some of the problems mentioned earlier in the introduction.

Author Contributions

AI carried the conceptualization by formulating the goals, aims of the research article, formal analysis by applying the statistical, mathematical and computational techniques to synthesize and analyze the hypothetical data, carried the methodology by creating the model, software programming and implementation, supervision, writing, drafting, editing, preparation, and creation of the presenting work.

Funding

No funding resource. No funding roles in the design of the study and collection, analysis, and interpretation of data and in writing the manuscript are declared

Ethics Approval and Consent to Participate

Not applicable.

Consent for Publication

Not applicable

Data Availability Statement

Not applicable. Data sharing not applicable to this article as no datasets were generated or analyzed during the current study.

Conflicts of Interest

The author declares no competing interests of any type.

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  35. Sklar, A. Random Variables, Joint distribution functions, and copulas. Kybernetika 1973, 9, 449–460. [Google Scholar]
Figure 1. shows the generator function (decreasing and convex) at theta = 0.3.
Figure 1. shows the generator function (decreasing and convex) at theta = 0.3.
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Figure 2. shows the joint CDF copula (Copula) at theta = 0.3.
Figure 2. shows the joint CDF copula (Copula) at theta = 0.3.
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Figure 3. shows the joint PDF copula (copula density) at theta = 0.3.
Figure 3. shows the joint PDF copula (copula density) at theta = 0.3.
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Figure 4. shows the generator function (decreasing and convex) at theta = 0.6.
Figure 4. shows the generator function (decreasing and convex) at theta = 0.6.
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Figure 5. shows the joint CDF copula (Copula) at theta = 0.6.
Figure 5. shows the joint CDF copula (Copula) at theta = 0.6.
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Figure 6. shows the joint PDF copula (copula density) at theta = 0.6.
Figure 6. shows the joint PDF copula (copula density) at theta = 0.6.
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Figure 7. shows the generator function (decreasing and convex) at theta = 0.888.
Figure 7. shows the generator function (decreasing and convex) at theta = 0.888.
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Figure 8. shows the joint CDF copula (Copula) at theta = 0.888.
Figure 8. shows the joint CDF copula (Copula) at theta = 0.888.
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Figure 9. shows the joint PDF copula (copula density) at theta = 0.888.
Figure 9. shows the joint PDF copula (copula density) at theta = 0.888.
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Figure 10. shows the generator function (decreasing and convex) at theta = 0.999.
Figure 10. shows the generator function (decreasing and convex) at theta = 0.999.
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Figure 11. shows the joint CDF copula (Copula) at theta = 0.999.
Figure 11. shows the joint CDF copula (Copula) at theta = 0.999.
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Figure 12. shows the joint PDF copula (copula density) at theta = 0.999.
Figure 12. shows the joint PDF copula (copula density) at theta = 0.999.
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Figure 13. shows the generator function (decreasing and convex) at theta = 1.
Figure 13. shows the generator function (decreasing and convex) at theta = 1.
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Figure 14. shows the joint CDF copula (Copula) at theta = 1.
Figure 14. shows the joint CDF copula (Copula) at theta = 1.
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Figure 15. shows the joint PDF copula (copula density) at theta = 1.
Figure 15. shows the joint PDF copula (copula density) at theta = 1.
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Figure 16. shows the joint CDF copula (Copula) at theta = 0.001.
Figure 16. shows the joint CDF copula (Copula) at theta = 0.001.
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Figure 17. shows the joint PDF copula at theta = 0.001.
Figure 17. shows the joint PDF copula at theta = 0.001.
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Figure 18. shows the joint CDF copula (Copula) at theta = 0.002.
Figure 18. shows the joint CDF copula (Copula) at theta = 0.002.
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Figure 19. shows the joint PDF copula at theta = 0.002.
Figure 19. shows the joint PDF copula at theta = 0.002.
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Figure 20. shows the joint CDF copula (Copula) at theta = 0.003.
Figure 20. shows the joint CDF copula (Copula) at theta = 0.003.
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Figure 21. shows the joint PDF copula at theta = 0.003.
Figure 21. shows the joint PDF copula at theta = 0.003.
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Figure 22. shows the joint CDF copula at theta = 0.004.
Figure 22. shows the joint CDF copula at theta = 0.004.
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Figure 23. shows the joint PDF copula at theta = 0.004.
Figure 23. shows the joint PDF copula at theta = 0.004.
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Figure 24. shows the joint PDF copula at theta = 0.005.
Figure 24. shows the joint PDF copula at theta = 0.005.
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Figure 25. shows the joint CDF copula at theta = 0.005.
Figure 25. shows the joint CDF copula at theta = 0.005.
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Figure 26. shows the joint PDF copula at theta = 0.006.
Figure 26. shows the joint PDF copula at theta = 0.006.
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Figure 27. shows the joint PDF copula at theta = 0.007.
Figure 27. shows the joint PDF copula at theta = 0.007.
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Figure 28. shows the joint PDF copula at theta = 0.008.
Figure 28. shows the joint PDF copula at theta = 0.008.
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Figure 29. shows the joint PDF copula at theta = 0.009.
Figure 29. shows the joint PDF copula at theta = 0.009.
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Figure 30. shows the joint PDF copula at theta = 0.01.
Figure 30. shows the joint PDF copula at theta = 0.01.
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Figure 31. tail dependency behavior of the Copula at dependency parameter 0.01.
Figure 31. tail dependency behavior of the Copula at dependency parameter 0.01.
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Figure 32. tail dependency behavior of the Copula at dependency parameter 0.6.
Figure 32. tail dependency behavior of the Copula at dependency parameter 0.6.
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