Research article Special Issues

Characterization of extension map on fuzzy weakly cut-stable map

  • In this paper, based on a complete residuated lattice, we propose the definition of fuzzy weakly cut-stable map and prove the extension property of the fuzzy weakly cut-stable map. Following this, it is explored the conditions under which the extension map to be fuzzy order isomorphism.

    Citation: Nana Ma, Qingjun Luo, Geni Xu. Characterization of extension map on fuzzy weakly cut-stable map[J]. AIMS Mathematics, 2022, 7(5): 7507-7518. doi: 10.3934/math.2022421

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  • In this paper, based on a complete residuated lattice, we propose the definition of fuzzy weakly cut-stable map and prove the extension property of the fuzzy weakly cut-stable map. Following this, it is explored the conditions under which the extension map to be fuzzy order isomorphism.



    Abbreviations: BE(s): Bayes estimate(s)\estimator(s); ML: Maximum likelihood; MLE(s): Maximum likelihood estimate(s)\estimator(s); Type-Ⅰ APHCS: Type-Ⅰ adaptive progressive hybrid censoring scheme; Type -Ⅱ APHCS: Type-Ⅱ adaptive progressive hybrid censoring scheme; PCS: Progressive censoring scheme; HPD: Highest posterior density; MC: Monte Carlo; MCMC: Markov Chain Monte Carlo; MH: Metropolis-Hastings; IWD: Inverse Weibull distribution; pdf: Probability density function; cdf: Cumulative density function; hrf: Hazard rate function; sf: Survival function; i.i.d: Independent and identically distributed; IP(s): Informative prior(s); Non-IP: Non-informative prior; CI(s): Confidence interval(s); Asy-CI: Asymptotic confidence interval; St.E: Standard error; MSE: Mean squared-error; AILs: Average interval lengths; CPs: Coverage probabilities

    Statistical inference for the life products requires placing some units of the product under test to get more information about the life testing experiments to get the complete data, there are many situations where observed data are censored in nature. Different censoring schemes are widely used in practice to make a life testing experiment be more time and cost--effective. Type-Ⅰ and Type-Ⅱ censoring schemes are popular censoring schemes. The experimental duration is set in a Type-Ⅰ censoring scheme, but the number of reported losses is a random variable. Conversely, in a Type-Ⅱ censoring system, the duration of the trial is random while the number of reported losses is constant. However, none of these two censoring schemes any experimental unit can be withdrawn during the experiment. The PCS allows the withdrawal of some experimental units during the experiment. The combination of Type-Ⅰ and Type-Ⅱ censoring schemes is known as a hybrid censoring scheme. Different PCS have been suggested in the literature. The most popular one is the progressive Type-Ⅰ. They are as follows: supposing n identical units are tested; in the traditional Type-Ⅰ censoring system, the experiment continues until a set time has passed τ. In the traditional Type-Ⅱ censoring technique, the experiment is ended after a predefined number of failures m<n. Reference [1] created the Type-Ⅰ hybrid censoring system, which is a combination of Type-Ⅰ and Type-Ⅱ censoring systems and has been widely utilized in the literature. The life test experiment is ended at a random moment in a mixed censoring strategy. The life test experiment is stopped at a random time τ=min(ym:m:n,τ) under the hybrid censoring system. Reference [2] suggested a novel hybrid censoring strategy to end the τ=max(ym:m:n,τ). Type-Ⅱ hybrid censoring is the name of this hybrid censoring technique. One of the disadvantages of these approaches is that they prevent the units from being removed from the experiment at any time other than the end. To address this issue, a broader censoring system known as progressive Type-Ⅱ censoring is employed.

    The next is a description of the progressive Type-Ⅱ censoring scheme is: during a life-testing experiment, consider an experiment in which n units are placed with m units required to fail. Units y1:m:n,R1 are randomly taken from the remaining n1 surviving units when the first failure occurs. Similarly, when the second failure y2:m:n,R2 occurs, n2R1 units are withdrawn at random from the surviving units, and so on. At the time of the mth failure ym:m:n all remaining nmR1R2...Rm1units are eliminated when the system fails. Prior the study, the progressively censoring technique R1,R2,...,Rmwas fixed and set. A Type-Ⅰ PHC system, which is a combination of Type-Ⅱ progressive and hybrid Type-Ⅰ censoring systems, was investigated by references [3,4]. In this experiment, nidentical units are tested using a predetermined progressive filtering technique R1,R2,...,Rm, and the experiment is stopped at a random period τ=min(ym:m:n,τ). If the mth failure occurs before the time point τ, the experiment ends at that time point if the failure happens before the time point ym:m:n. Alternatively, assume the mth failure does not happen before time point τ and only J failures happen before the time point τ, the experiment concludes at the time point τ when all the remaining units are removed. Reference [5] showed a Type-Ⅱ PHC method, in which the experiment ends at time τ=max(ym:m:n,τ). Reference [6] suggested a Type-Ⅱ APHC system, within which the number of failures m and the related progressive method is provided, but the units are not deleted as the experiment advances time τ. For an all-inclusive survey of the literature on hybrid censoring, see Reference [7]. Because of the short time, it takes to create a product, reliability testing has to be undertaken under stern time limitations, which makes failure censored systems out of date in many goods fields. Reference [8] presents Type-Ⅰ APHCS that assurances the finish of the lifetime testing experiment at a predetermined time which outcomes in higher estimate competence.

    The following is a description of the Type-Ⅰ APHCS (see Reference [8]): Assume n similar units are tested using a progressive censoring scheme R1,R2,...,Rm, 1mn, and the test concludes at a certain point τ, where τ(0,) and integers Ri's are prefixed. At the time of the first failure y1:m:n,R1 of the remaining units are randomly removed. Similarly, at the time of the second failure y2:m:n,R2 of the remaining units are randomly removed and so on. Let J denote the number of failures that happen before time τ. If the mth failure ym:m:n happens before time τ (i.e.,ym:m:n<τ), the process will not stop, but continue on observing failures without any further withdrawals until reach time τ. Then, at time τ all remaining units RJ=nJJi=1Ri are eliminated, and the project is halted. The PCS in this case will become R1,R2,...,Rm,Rm+1,...,RJ, where Rm=Rm+1=...=RJ=0. Otherwise, the process when ym:m:n>τ will have a PCS as R1,R2,...,RJ. Type-Ⅰ APHCS is useful when time is the primary consideration in the test and the test must be terminated at a set time irrespective of the amount of failures. Additionally, clarifications may be found in references [8,9,10,11,12,13,14,15,16,17,18].

    Figure 1.  Schematic representation of Type-Ⅰ APHCS.

    In reliability analysis, an item's failure might be attributed to multiple causes at the same time. These "causes" are competing for control of the experimental unit's failure. This issue is known to as competing risks model in the statistical literature. The data used in the study of competing risks consists of a failure time and the reason of failure. It's possible to presume that the causes of failure are either independent or dependent. For further information about this see [19,20,21,22,23].

    The primary goal of this research is to examine the competing risk model in the context of a Type-Ⅰ APHCS. We'll also suppose that the lifetimes of the competing hazards have independent IWD. We derive the MLEs, approximate CIs, and two distinct bootstrap CIs; additionally, we used MCMC approaches, to be able to derive BEs for squared error functions and credible intervals using gamma priors.

    The following is how the rest of the paper is structured: The IWD is introduced as a failure model in Section Ⅱ. The ML inference of unknown parameters is discussed in Section Ⅲ. Section Ⅳ includes two parametric bootstrap CIs and an approximation CI for unknown parameters. Section Ⅴ investigates the Bayesian estimation approach using the MH algorithm and the gamma distribution as a prior distribution for the unknown parameters. In Section Ⅵ, the theoretical results are illustrated using a simulated study and real data. Finally, Section Ⅶ contains the conclusions. Tables can be found in the appendix.

    Due to the Weibull distribution's inability to match data with non-monotone and unimodal hazard rate functions, the IWD is a much more suitable model than the Weibull distribution. Depending on the shape parameter's value, the IWD's hrf can decrease or increase. The IWD's pdf, cdf, sf and hrf for single variable y, are shown as follows, respectively

    f(y;η,φ)=ηφy(φ+1)exp(ηyφ);y,η,φ>0 (1)
    F(y;η,φ)=exp(ηyφ);y,η,φ>0 (2)
    ¯F(y;η,φ)=1exp(ηyφ) (3)

    and

    h(y;η,φ)=ηφy(φ+1)(eηyφ1)1 (4)

    where η and φ are the distribution's scale and shape parameters, respectively.

    The IWD can be used to show a wide range of data, including the time it takes for an insulating fluid to break down under constant tension, as well as the degradation of mechanical parts like pistons and crankshafts in diesel engines. References [24,25,26,27] have all done extensive work on the IWD. For further information on the modifications of the IW distribution, read reference [28]. Moreover, other articles have looked at IWD under various censoring schemes see references [29,30,31,32,33].

    In reliability analysis, an item's failure might be attributed to multiple causes at the same time. To failure this experiment unit, these causes are competing for them. Given a lifetime experiment with nN identical units, in which the lifetimes are described by i.i.d random variables Y1,Y2,...,Yn. Put the assumption that there are just two causes of failure without losing generality. We have Y1=min(Y1i,Y2i) for i=1,2,...,n, where Yki, k=1,2 denotes the ith unit's latent failure time under the kth cause of failure. The latent failure times are assumed to be Y1i and Y2i are independent, and the pairs (Y1i,Y2i) are i.i.d. Assume the failure times are distributed according to IWD with different scale and shape parameters (ηk,φk,k=1,2), with the sf ¯Fk and hrf hk already having form

    ¯Fk=[1exp(ηkyφk)],hk=ηkφky(φk+1)(eηkyφk1)1;y,ηk,φk>0,k=1,2 (5)

    We have the following observation under Type-Ⅰ APHCS under competing risks data:

    (Y1:m:n,δ1,R1),...,(Ym1:m:n,δm,Rm1),(Ym:m:n,δm,0),...,(YJ:m:n,δJ,0),(τ,RJ)

    where, δi is the indicator indicating the reason for failure, J is the number of failures prior to time τ, and RJ is the number of units residual at the time point τ with Rm=Rm+1,...,RJ=0. Let δi(1,2). Here, δi=k, k=1,2 means the unit i has failed due to cause k. Further, we define

    I1(δi=1)={1,δi=10elseandI2(δi=2)={1,δi=20else

    Thus, the random variables J1=Ji=1I1(δi=1) and J2=Ji=1I2(δi=2) show the number of failures due to the first and the second cause of failures, respectively. For a specific censoring scheme, R1,R2,...,Rm1,0,...,0,RJ, the observed data's (x1,δ1),...,(τ,RJ) then, the likelihood function is given by

    L=CJJi=1{[f1(yi)¯F2(yi)]I(δi=1)[f2(yi)¯F1(yi)]I(δi=2)[¯F1(yi)¯F2(yi)]Ri}[¯F1(τ)¯F2(τ)]RJ

    where yi=yi:m:n to simplify the notation, CJ=Ji=1γi with γi=mi+1mi=1Rj. Appling the identityfk=hk¯Fk, The likelihood function can also be written as

    L=CJJi=1{[h1(yi)]I(δi=1)[h2(yi)]I(δi=2)[¯F1(yi)¯F2(yi)]1+Ri}[¯F1(τ)¯F2(τ)]RJ (6)

    In the presence of Type-Ⅰ APHC with competing risks data (6) and from the life time distribution (5), then, ignoring the constant, the likelihood function of the observed data can be written as:

    L(ϕ|x_)2k=1(ηkφk)Jkψki[Ji=1(W1iW2i)(1+Ri)][S1S2]RJ (7)

    where Uki=(eηkyφki1), ψki=(Jki=1y(φk+1)i)[Jki=1U1ki], Wki=[1exp(ηkyφki)], yi=y(i), k=1,2, Sk=[1exp(ηkτφk)] and L(ϕ|y_)=L(η1,η2,φ1,φ2|y_) for simplicity of notation J1=J1i=1I(δi=1) and J2=J2i=1I(δi=2) describe the number of the failures due to the first and the second cause of the failures, respectively. Using the likelihood function of the natural logarithm l=lnL(ϕ) in Eq (7), we obtain

    lJ1lnη1+J1lnφ1(φ1+1)J1i=1lnyiJ1i=1lnU1i+J2lnη2+J2lnφ2(φ2+1)J2i=1lnyiJ2i=1lnU2i+Ji=1(1+Ri)(lnW1i+lnW2i)+RJ(lnS1+lnS2) (8)

    The first order derivatives of Eq (8) with respect to ηk,φk, k=1,2 are given respectively by

    lφk=JkφkJki=1lnyi+ηkJki=1Vkiln(yi)ηkJi=1(1+Ri)Qkiln(yi)ηkRJEkln(τ) (9)
    lηk=JkηkJki=1Vki+Ji=1(1+Ri)Qki+RJEk (10)

    where, Vki=yφkiexp(ηkyφki)U1ki, Qki=yφkiexp(ηkyφki)W1ki, Eki=τβkexp(ηkτφk)S1k and k=1,2. The MLE of ηk,φk and k=1,2 can be obtained by equating the first derivatives in Eqs (9) and (10) to zero. As far as it seems, there is no closed form answer to the system of nonlinear Eqs (9) and (10) in ηk,φk where k=1,2. So, a numerical approach is wanted for competing the MLE of ηk,φk where k=1,2.

    The asymptotic variance covariance matrix of the MLEs of ϕ=(ηk,φk) and k=1,2 are given by the elements that are the negative expectation values of the second derivatives of logarithms of the likelihood functions. Cohen found that by substituting expected values with MLEs, the approximate variance covariance matrix could be calculated—see reference [34]. Now, the approximate sample information matrix should now be as follows

    I(ˆϕ)=[2lη2102lη1φ1002lη2202lη2φ22lφ1η102lφ21002lφ2η202lφ22](ηk=ˆηk,φk=ˆφk) (11)

    where k=1,2 and the elements of 4×4 matrix I(ϕ) can be obtained as follows:

    2lη2k=Jkη2kJki=1yφkiVki+Jki=1V2kiJi=1(1+Ri)yφkiQkiJi=1(1+Ri)Q2kiRJτφkEkRJE2k,
    2lφ2k=Jkφ2kη2kJki=1yφkiVki(lnyi)2ηkJki=1Vki(lnyi)2+η2kJki=1V2ki(lnyi)2η2kJi=1(1+Ri)yφkiQki(lnyi)2+ηkJi=1(1+Ri)Qki(lnyi)2η2kJi=1(1+Ri)Q2ki(lnyi)2η2kRJτφkEk(lnτ)2+ηkRJEk(lnτ)2η2kRJE2k(lnτ)2,

    and

    2lηkφk=ηkJki=1xφkiVki(lnyi)+Jki=1Vki(lnyi)ηkJki=1V2ki(lnyi)+ηkJi=1(1+Ri)yφkiQki(lnyi)+ηkRJE2k(lnτ)Ji=1(1+Ri)Qki(lnyi)+ηkJi=1(1+Ri)Q2ki(lnyi)+ηkRJτφkEk(lnτ)RJEk(lnτ).

    Now, we calculate the relative risk rates, π1 and π2 due to case 1 and 2, respectively. The relative risk related to case 1 is calculated as follows:

    π1=p(Y1iY2i)=0f1(y)ˉF2(y)dy=0f1(y)dy0f1(y)exp(η2yφ2)dy

    therefore,

    π1=1η1φ10y(φ1+1)exp[(η1yφ1+η2yφ2)]dy (12)

    Once π1 is computed, we determine π2 using the relation π2=1π1

    π2=η1φ10y(φ1+1)exp[(η1yφ1+η2yφ2)]dy

    We must apply a numerical methodology to solve the integral on the right side of Eq (12) because it has no analytical solution. The MLE of the relative risk rates π1 and π2 can be calculated by substituting the MLE of ηk,φk and k=1,2 in according to the MLE's invariance property Eq (12).

    In this section, Different CIs are suggested. The asymptotic distribution of ηk,φk, k=1,2 and two separate bootstrap CIs are used in one.

    The asymptotic distribution of the MLEs of the components of the vector of ϕ=(ηk,φk) and k=1,2 is being used to derive the approximate CIs for both the parameters. The asymptotic distribution of the MLEs of the parameters is known as

    (ˆϕϕ)N4(0,I1(ˆϕ))

    where I(ϕ) is a matrix of Fisher information. When certain regularity constraints are met, the two-sided 100(1γ)%, 0<γ<1, asymptotic CIs for the unknown parameters ϕ=(ηk,φk) and k=1,2 can be obtained as

    ˆϕ±Zγ2Var(ˆϕ)

    where Var(ˆϕ) is the element of the main diagonal of I1(ˆϕ) and Zγ2 is the 100(1γ)% standard normal percentile.

    Here, we construct two parametric bootstrap CIs for ηk,φk, k=1,2 as

    1) Calculate the MLE of ϕ=(ηk,φk) and k=1,2 under Type-Ⅰ APHCS competing risks data.

    2) Generated a bootstrap sample using ηk,φk, k=1,2 to obtain the bootstrap estimate of ηk say ˆηbk, φk say ˆφbk and k=1,2 using the bootstrap sample.

    3) Step (2) is repeated B times to have (ηb(1)k,ηb(2)k,...,ηb(B)k) and (φb(1)k,φb(2)k,...,φb(B)k).

    4) By arranging (ηb(1)k,ηb(2)k,...,ηb(B)k), (φb(1)k,φb(2)k,...,φb(B)k) in ascending order as (ηb[1]k,ηb[2]k,...,ηb[B]k) and (φb[1]k,φb[2]k,...,φb[B]k).

    A two side 100(1γ)% percentile bootstrap CI for ηk,φk and k=1,2 is given by {ˆηb[Bγ2]k,ˆηb[B(1γ2)]k} and (ˆφb[Bγ2]k,ˆφb[B(1γ2)]k).

    1) The same as in Boot-p steps (1-2).

    2) Calculate the t-statistic of ϕ=(ηk,φk) and k=1,2 as T=(ˆϕbkˆϕk)Var(ˆϕbk) where Var(ˆφbk) is asymptotic variances of ˆϕbk and it can be obtained using the Fisher information matrix.

    3) Step 2–3 are repeated B times and obtain T(1),T(2),...,T(B).

    4) By arranging T(1),T(2),...,T(B) in ascending order as T[1],T[2],...,T[B].

    5) A two side 100(1γ)% percentile bootstrap-t CI for ηk,φk and k=1,2 is given by

    {ˆηk+T[Bγ2]kVar(ˆηk),ˆηk+T[B(1γ2)]kVar(ˆηk)},and{ˆφk+T[Bγ2]kVar(ˆφk),ˆφk+T[B(1γ2)]kVar(ˆφk)}.

    In this section, based on competing risks data, the BE utilizing square error loss functions are obtain based on a Type-Ⅰ APHCS under the assumption independently distributed with gamma prior distribution with known parameters ηk,φk where k=1,2 of the IWD as

    πk(ηk)ηak1kexp(ηkbk),ηk,ak,bk>0,k=1,2,

    and

    πk(φk)φck1kexp(φkdk),φk,ck,dk>0,k=1,2.

    where the hyper-parameters ak,bk,ck,dk and k=1,2 are chosen based on prior knowledge of the unknown parameters. Then we can write the jointly prior densities of ηk,φk and k=1,2 as

    πk(ηk,φk)ηak1kφck1kexp[(ηkbk+φkdk)],ηk,φk,ak,bk,ck,dk>0,k=1,2 (13)

    when the IPs are taken into account, the hyper-parameter elicitation will be chosen. The MLEs of ηk,φk and k=1,2 will be used to generate these IPs. Equal the mean and variance of (ˆηqk,ˆφqk) with the mean and variance of the priors under consideration (Gamma priors), where k=1,2 and q=1,2,...,N, here N is really the number of samples from the IWD that are available. Thus, when the mean and variance of ˆηqk and ˆφqk are equal to the mean and variance of gamma priors, one can obtain (see reference [35])

    1NNq=1ˆηqk=akbk&1N1Nq=1(ˆηqk1NNq=1ˆηqk)2=akb2k
    1NNq=1ˆφqk=ckdk&1N1Nq=1(ˆφqk1NNq=1ˆφqk)2=ckd2k

    The estimated hyper-parameters now have the following forms after solving the about equations

    ak=(1NNq=1ˆηqk)21N1Nq=1(ˆηqk1NNq=1ˆηqk)2,bk=(1NNq=1ˆηqk)21N1Nq=1(ˆηqk1NNq=1ˆηqk)2,
    ck=(1NNq=1ˆφqk)21N1Nq=1(ˆφqk1NNq=1ˆφqk)2anddk=(1NNq=1ˆφqk)21N1Nq=1(ˆφqk1NNq=1ˆφqk)2.

    For the observed data y acquired from a life test experiment's Type-Ⅰ APHCS with two independent IW (η1,φ1) and IW (η2,φ2) and given the likelihood function in Eq (7) and prior distribution in Eq (13). The corresponding posterior density of ϕ=(ηk,φk) and k=1,2 is given by

    π(ϕ|x_)L(ϕ|x_).g(η1,φ2,η1,φ2).

    The posterior density function is given by

    π(ϕ|y_)=2k=1ηJk+ak1kφJk+ck1kexp[(ηkbk+φkdk)]ωki(ϕ);ak,bk,ck,dk,ηk,φk, (14)

    where ωki(ϕ)=ψki[Ji=1(W1iW2i)(1+Ri)][S1S2]RJ.

    The conditional posterior densities of ϕ=(ηk,φk) and k=1,2 are as follows

    π1(η1|y)ηJ1+a111exp(η1b1)[J1i=1(eη1yφ1i1)1][Ji=1(1eη1yφ1i)(1+Ri)](1eη1τφ1)RJ,
    π2(η2|y_)ηJ2+a212exp(η2b2)[J2i=1(eη2yφ2i1)1][Ji=1(1eη2yφ2i)(1+Ri)](1eη2τφ2)RJ,
    π3(φ1|y)φJ1+c111exp(φ1d1)(J1i=1y(φ1+1)i)[J1i=1(eη1yφ1i1)1][Ji=1(1eη1yφ1i)(1+Ri)](1eη1τφ1)RJ,
    π4(φ2|y)φJ2+c212exp(φ2d2)(J2i=1y(φ2+1)i)[J2i=1(eη2yφ2i1)1][Ji=1(1eη2yφ2i)(1+Ri)](1eη2τφ2)RJ

    As a result, we use the MH method to generate according to the above distribution see reference [36]. Readers can consult reference [37] for more information on how to implement the MH algorithm. We started also with MLEs to drive the Gibbs sampler algorithm. We then choose samples from different complete conditionals in the runs, using very latest readings of all other conditioning variables, unless a consistent pattern of convergence was seen. While, the BEs of any function say g(η1,φ1,η2,φ2) based on Type-Ⅰ APHCS with competing risks under square error loss functions; denoted by ˜g(ηk,φk) can be studied through the following equation as

    ˜g(η1,φ1,η2,φ2)=0000g(η1,φ1,η2,φ2)π(ϕ|y_)dη1dη2dφ1dφ2 (15)

    Closed form of equations cannot be used for obtaining the ratio of the four integrals demonstrated in Eq (15). Therefore, we recommend the MCMC method to reach an approximated value of the BEs of ηk,φk,k=1,2. Using MH algorithm, this technique can generate a posterior sample. Several authors state that MCMC is a computer-based sampling technique that enables a user to indicate and define a distribution regardless of its mathematical characteristics obtained by random sampling values—see reference [38]. Working with posterior distributions, it is more profitable to use MCMC rather than using analytic examination which is very hard to work with. The MCMC makes it easy for the user to reach rough values of posterior distributions which is cannot be easily measured using a computer (like posteriors means and its random samples). Using the MCMC technique, samples are:

    1) Start with a wild preliminary guess: a single value that could be derived from the distribution.

    2) Using this preliminary assumption, generate a series of new samples. Two steps are created as a result of each new sample:

    ● Proposal: the most recent sample is disturbed with a small random perturbation to provide a proposal for the new sample.

    ● Acceptance: a novel suggestion will be either approved as a new sample or rejected (in which case the old sample is retained). There are several methods for introducing random noise into the system to generate ideas, as well as numerous methods for approving and refusing them, such as Gibbs sampling and the MH algorithm.

    A proposing distribution and also a preliminary value of ϕ=(ηk,φk) and k=1,2 must always be defined in order to conduct the MH method for the IWD. A multivariate normal distribution can be used to represent the proposal distribution as

    q({η'kk,φ'k}|{ηk,φk})N4({ηk,φk}|S{ηk,φk})

    where S{λk,βk} represents the variance-covariance matrix, it is possible to acquire negative observations, which is undesirable. For starting values, the MLE may be used as ϕ=(ηk,φk) and k=1,2, that is {η(0)k,φ(0)k}={ˆηk,ˆφk}. The selection of S{ηk,φk} is considered to be the asymptotic variance-covariance matrix I1{ˆηk,ˆφk}, where I{.} is an abbreviation for Fisher information matrix. It is worth noting that the choice of S{ηk,φk} is a critical issue in the MH algorithm, as the acceptance is dependent on it. The steps of the MH method for drawing a sample from the posterior density Eq (14) are as follows

    Step 1. Set initial value of ϕ as ϕ(0)={ˆη1,ˆφ1,ˆη2,ˆφ2}.

    Step 2. For i=1,2,...,M the following steps are repeating:

    a) Set ϕ=ϕ(i1).

    b) Generate a new candidate parameter value ς from N4(lnϕ,Sϕ).

    c) Set ϕ'=exp(ς).

    d) Calculate ζ=π(ϕ'|y)π(ϕ|y), where π(.) is the posterior density in Eq (14).

    e) Generate a sample u from the uniform distribution U(0,1).

    f) Accept or reject the new candidate ϕ'

    {Ifuζsetϕ(i)=ϕ'otherwisesetϕ(i)=ϕ'.

    Finally, part of the initial samples taken from the posterior density's random samples of size M can be discarded (burn-in), and the surviving samples may be utilized to compute BEs. More specifically, Eq (14) can be calculated as

    ˜gMH(ηk,φk)=1MlζMi=lζg(η1i,φ1i,η2i,φ2i) (16)

    where lζ defines the number of burn-in samples.

    In this subsection, for k=1,2, one can unutilized method of reference [39] to construct the HPD credible intervals for ηk and φk of the IWD under Type-Ⅰ APHCS with competing risks data using the samples drawn from suggested MH algorithm in the previous subsection. Let ηγk and φγk be the γth quantile of ηk and φk, respectively, that is,

    {ηγk,φγk}=inf[{ηk,φk}:Π({ηk,φk}|y)γ],

    where 0<γ<1 and Π(.) is the posterior distribution function of the unknown parameters ηk,φk and k=1,2. Notice that for a given ηk,φk and k=1,2, a simulation consistent estimator of π(ηk,φk|y) can be evaluated as

    Π(ηk,φk|y)=1MlζMi=lζI{ηk,φk}(ηk,φk).

    Here I{ηk,φk}(ηk,φk) is the indicator function. Then the corresponding estimate is calculated as follows:

    ˆΠ(ηk,φk|y)={0if{ηk,φk}<{ηk(lζ),φk(lζ)}ik=lζwkif{ηk(i),φk(i)}<{ηk,φk}<{ηk(i+1),φk(i+1)}1if{ηk,φk}<{ηk(M),φk(M)}

    where ws=1Mlζ and {ηk(s),φk(s)} are the ordered values of {ηks,φks}. Now, for i=lζ,...,M,{η(γ)k,φ(γ)k} can be convergent by

    {˜η(γ)k,˜φ(γ)k}={{ηk(lζ),φk(lζ)}ifγ=0{ηk(i),φk(i)}ifi1k=lζwk<γ<ik=lζwk.

    Now to obtain a 100(1γ)% HPD credible interval for ηk,φk and k=1,2, let

    HPDηks={˜η[sM]k,˜η[(s+(1γ)M)M]k}&HPDφks={˜φ[sM]k,˜φ[(s+(1γ)M)M]k}

    for s=lζ,...,[γM]. Then choose HPDs among all the HPDs's such that it has the smallest width.

    The purpose of this section is to compare the results of the various estimation methods presented in the previous parts. A MC analysis is used to evaluate the statistical behaviors of the estimators within Type-Ⅰ APHCS under competing risks mode, as well as to check the behavior of the suggested approaches. A real data collection is also evaluated for demonstration. For calculations, the R statistical programming language will be utilized. In addition, the bbmle and HDInterval packages in R can be used to compute MLEs and HPD intervals.

    To compare the performance of suggested MC estimation methods, a simulation study is used. The MC simulation is carried out utilizing two estimate methods: ML and Bayesian estimations. With the following assumptions, 1000 data sets of IWD competing risks model under Type-Ⅰ PHCS are generated for MLEs.

    1) Assume the parameters of the IWD in the following options: (η1,φ1,η2,φ2)=(0.5,1.5,0.75,2).

    2) For each cause of failure, the sample sizes are n=50,100,200 and the number of failures observed m=20,40,60.

    3) Number of re-samplings for bootstrap CI is 1000.

    4) Censoring times for Type-Ⅰ APHCS are assumed as: τ=1,1.5,2.

    5) Removed items Rj are assumed to as follows:

    Scheme Ⅰ: R1=nm and R2=...=Rm=0.

    Scheme Ⅱ: R1=...=Rm2=0, R(m2+1)=nm and R(m2+2)=...=Rm=0.

    Scheme Ⅲ: R1=...=Rm1=0 and Rm=nm.

    MLEs and related to 95% asymptotic CI and two types of bootstrap CI are calculate based on the generated data. Note that the preliminary guess values are regarded as the same as the true parameter values whilst gaining MLEs. Also, we used the MH algorithm to computed BEs by the IP and Non-IP. Thus:

    ● For IP, we assume that the hyper-parameter values as a1=b1=0.5, c1=d1=1.5, a2=b2=0.75, c2=d2=2.

    ● For Non-IP, we assume that the hyper-parameter values are a1=b1=c1=d1=a2=b2=c2=d2=0, hence the joint prior density is defined as π(η1,φ1,η2,φ2)=1η1×φ1×η2×φ2.

    These values, referred to as hyper-parameters, are then used to produce the desired estimations. When the MH method is used, the MLEs are used as preliminary guess estimates, together with the associated variance-covariance matrix Sϕ of [ln(η1),ln(φ1),ln(η2),ln(φ2)] which can be obtained using delta method (see reference [40]). Lastly, 1200 burn-in samples are removed from the total 6000 samples obtained from the posterior density and subsequent BE and HPD interval estimations.

    Tables 13 are showing all of the average bias estimates and related MSEs for both methods. Furthermore, the corresponding AILs and CPs are presented in Tables 46 for all of the suggested CIs, namely; Asy-CI, bootstrap (Boot-P and Boot-T) CI, and HPD interval.

    Table 1.  Bias and MSEs of the MLE and BEs based on the Type-Ⅰ APHCS under various censoring schemes at (η1=0.5,φ1=1.5,η2=0.75,φ2=2), and (n,m)=(50,20).
    τ Scheme Parm. MLE MCMC: IP MCMC: Non-IP
    Bias MSE Bias MSE Bias MSE
    1.00 η1 0.1782 0.1371 0.1984 0.1928 0.2065 0.2176
    φ1 0.1929 0.6695 0.1688 0.7014 0.2169 0.9156
    η2 0.0721 0.1111 0.0849 0.1342 0.0455 0.1789
    φ2 0.2947 0.8145 0.2885 0.7188 0.2632 1.2457
    η1 0.1819 0.1567 0.2114 0.2304 0.2893 0.2364
    φ1 0.1243 0.7738 0.0908 0.7439 0.1823 1.0724
    η2 0.0669 0.1266 0.0823 0.2231 0.0617 0.1849
    φ2 0.3809 0.8589 0.3637 0.7335 0.3920 1.0488
    η1 0.1307 0.1450 0.1592 0.2068 0.1694 0.2528
    φ1 0.3045 1.2015 0.2736 1.1935 0.3168 1.3615
    η2 0.1189 0.1420 0.1359 0.1635 0.1856 0.2324
    φ2 0.1981 1.1229 0.1946 0.9810 0.2600 1.4263
    1.50 η1 0.1834 0.1426 0.1874 0.1720 0.2073 0.2204
    φ1 0.2053 0.7629 0.17924 0.7072 0.2206 0.9859
    η2 0.0661 0.1129 0.0739 0.1395 0.0361 0.1790
    φ2 0.3076 0.7076 0.3059 0.6262 0.3153 0.8918
    η1 0.1751 0.1517 0.1918 0.1975 0.2279 0.2595
    φ1 0.1331 0.8100 0.0972 0.7113 0.1145 1.0073
    η2 0.0752 0.1272 0.0952 0.1609 0.0277 0.2079
    φ2 0.3648 0.9613 0.3535 0.7886 0.3761 1.2223
    η1 0.1243 0.1482 0.1350 0.1950 0.1827 0.2659
    φ1 0.3354 1.2688 0.3039 1.1397 0.3127 1.4749
    η2 0.1260 0.1489 0.1279 0.1750 0.0658 0.2373
    φ2 0.1722 1.1369 0.1921 1.0350 0.1920 1.4392
    2.00 η1 0.1817 0.1421 0.1837 0.1771 0.2181 0.2304
    φ1 0.1879 0.7337 0.1821 0.7224 0.1812 0.8879
    η2 0.0683 0.1138 0.0790 0.1446 0.0458 0.1682
    φ2 0.3128 0.7984 0.2991 0.7114 0.3055 0.9193
    η1 0.1735 0.1577 0.1920 0.2145 0.2258 0.2681
    φ1 0.1258 0.7363 0.1058 0.7574 0.1285 1.6146
    η2 0.0751 0.1321 0.0924 0.1597 0.0441 0.2021
    φ2 0.3609 1.0153 0.3554 0.8740 0.3673 1.1849
    η1 0.1368 0.1555 0.1370 0.1967 0.2048 0.3047
    φ1 0.3212 1.2075 0.3184 1.2011 0.3116 1.4986
    η2 0.1133 0.1495 0.1166 0.1841 0.0553 0.2498
    φ2 0.1627 1.2822 0.1673 1.1622 0.1840 1.4961

     | Show Table
    DownLoad: CSV
    Table 2.  Bias and MSEs of the MLE and BEs based on the Type-Ⅰ APHCS under various censoring schemes at (η1=0.5,φ1=1.5,η2=0.75,φ2=2), and (n,m)=(100,40).
    τ Scheme Parm. MLE MCMC: IP MCMC: Non-IP
    Bias MSE Bias MSE Bias MSE
    1.00 η1 0.2675 0.1232 0.2606 0.1417 0.2803 0.1632
    φ1 0.0843 0.1328 0.0674 0.1704 0.0868 0.1965
    η2 0.0175 0.0519 0.0001 0.0744 0.0377 0.0845
    φ2 0.5848 0.4645 0.5492 0.4590 0.5980 0.5336
    η1 0.2561 0.1257 0.2604 0.1582 0.2830 0.1752
    φ1 0.1594 0.1386 0.1518 0.1874 0.1766 0.2000
    η2 0.0061 0.0602 0.0067 0.0870 0.0059 0.0924
    φ2 0.6593 0.5480 0.6257 0.5465 0.6451 0.5961
    η1 0.2236 0.1198 0.2480 0.1696 0.2647 0.1980
    φ1 0.0329 0.2480 0.0449 0.2884 0.0503 0.3526
    η2 0.0261 0.0701 0.0302 0.1008 0.0018 0.1143
    φ2 0.5385 0.5061 0.5170 0.5106 0.5493 0.5954
    1.50 η1 0.2580 0.1199 0.2578 0.1430 0.2732 0.1616
    φ1 0.0711 0.1236 0.0604 0.1663 0.0694 0.1805
    η2 0.0080 0.0533 0.0012 0.0764 0.0199 0.0842
    φ2 0.5710 0.4447 0.5470 0.4555 0.5700 0.5019
    η1 0.2514 0.1225 0.2530 0.1527 0.2767 0.1755
    φ1 0.1465 0.1485 0.1376 0.1977 0.1598 0.2230
    η2 0.0013 0.0593 0.0171 0.0827 0.0210 0.0980
    φ2 0.6465 0.5450 0.6085 0.5448 0.6488 0.6185
    η1 0.2185 0.1199 0.2332 0.1622 0.2479 0.1794
    φ1 0.0179 0.3234 0.0207 0.3629 0.0336 0.4038
    η2 0.0315 0.0732 0.0382 0.1024 0.0063 0.1211
    φ2 0.5276 0.5196 0.5010 0.5322 0.5309 0.6038
    2.00 η1 0.2620 0.1253 0.2602 0.1506 0.2774 0.1684
    φ1 0.0720 0.1506 0.0615 0.2008 0.0736 0.2165
    η2 0.0119 0.0570 0.0008 0.0763 0.0390 0.0906
    φ2 0.5698 0.4803 0.5478 0.4901 0.5939 0.5707
    η1 0.2735 0.1358 0.2735 0.1668 0.2930 0.1819
    φ1 0.1708 0.1743 0.1537 0.2036 0.1779 0.2462
    η2 0.0235 0.0614 0.0129 0.0890 0.0408 0.1014
    φ2 0.6734 0.5829 0.6444 0.5758 0.6751 0.6512
    η1 0.2227 0.1215 0.2336 0.1646 0.2576 0.1835
    φ1 0.0352 0.2079 0.0337 0.2488 0.0569 0.2701
    η2 0.0273 0.0726 0.0348 0.0980 0.0033 0.1233
    φ2 0.5369 0.4842 0.5119 0.4901 0.5485 0.5827

     | Show Table
    DownLoad: CSV
    Table 3.  Bias and MSEs of the MLE and BEs based on the Type-Ⅰ APHCS under various censoring schemes at (η1=0.5,φ1=1.5,η2=0.75,φ2=2), and (n,m)=(200,60).
    τ Scheme Parm. MLE MCMC: IP MCMC: Non-IP
    Bias MSE Bias MSE Bias MSE
    1.00 η1 0.2557 0.1053 0.2721 0.1344 0.2706 0.1373
    φ1 0.1107 0.0818 0.1171 0.1154 0.1154 0.1224
    η2 0.0057 0.0381 0.0028 0.0592 0.0282 0.0653
    φ2 0.6104 0.4432 0.5813 04436 0.6218 0.4972
    η1 0.2727 0.1172 0.2728 0.1426 0.2826 0.1534
    φ1 0.1977 0.1207 0.1855 0.1529 0.1901 0.1603
    η2 0.0227 0.0433 0.0122 0.0668 0.0456 0.0869
    φ2 0.6972 0.5697 0.6648 0.5632 0.7001 0.6257
    η1 0.2226 0.1061 0.2317 0.1427 0.2458 0.1608
    φ1 0.0844 0.1182 0.0769 0.1580 0.0859 0.1773
    η2 0.0275 0.0575 0.0388 0.0848 0.0098 0.1007
    φ2 0.5833 0.4540 0.5528 0.4513 0.6008 0.5215
    1.50 η1 0.2485 0.0971 0.2545 0.1236 0.2685 0.1348
    φ1 0.1031 0.0789 0.0946 0.1130 0.1073 0.1214
    η2 0.0014 0.0353 0.0018 0.0545 0.0077 0.0663
    φ2 0.6032 0.4321 0.5904 0.4496 0.5979 0.4713
    η1 0.2648 0.1154 0.2752 0.1507 0.2790 0.1585
    φ1 0.1913 0.1174 0.1866 0.1515 0.1876 0.1577
    η2 0.0148 0.0454 0.0031 0.0730 0.0229 0.0796
    φ2 0.6912 0.5587 0.6561 0.5530 0.6834 0.5919
    η1 0.2172 0.1039 0.2257 0.1385 0.2461 0.1638
    φ1 0.0803 0.1127 0.0747 0.1486 0.0896 0.1684
    η2 0.0328 0.0579 0.0398 0.0853 0.0026 0.1039
    φ2 0.5795 0.4440 0.5493 0.4493 0.5883 0.5117
    2.00 η1 0.2461 0.0972 0.2483 0.1236 0.4366 0.1318
    φ1 0.0969 0.0783 0.0851 0.1150 0.0995 0.1173
    η2 0.0037 0.0366 0.0022 0.0585 0.0058 0.0614
    φ2 0.5969 0.4253 0.5787 0.4366 0.5941 0.4617
    η1 0.2682 0.1154 0.2755 0.1443 0.2857 0.1577
    φ1 0.1988 0.1131 0.1954 0.1437 0.1962 0.1573
    η2 0.0182 0.0438 0.0075 0.0658 0.0349 0.0807
    φ2 0.6986 0.5621 0.6758 0.5648 0.6965 0.6070
    η1 0.2009 0.0983 0.2174 0.1388 0.2338 0.1585
    φ1 0.0542 0.1184 0.0546 0.1608 0.0622 0.1899
    η2 0.0491 0.0605 0.0474 0.0919 0.0238 0.1026
    φ2 0.5522 0.4288 0.5333 0.4424 0.5599 0.4943

     | Show Table
    DownLoad: CSV
    Table 4.  The length of the difference intervals and CPs for the Type-Ⅰ APHCS under various censoring schemes at (η1=0.5,φ1=1.5,η2=0.75,φ2=2), and (n,m)=(50,20).
    τ Scheme Parm. MLE HPD- MCMC
    Asy-CI Boot-P Boot-T IP Non-IP
    1.00 η1 1.2733 (98.10) 1.2169 (95.50) 1.2079 (96.00) 1.4039 (95.20) 1.4173 (95.10)
    φ1 3.1185 (96.30) 2.8667 (92.10) 1.8982 (88.40) 2.5273 (96.00) 2.8493 (95.40)
    η2 1.2762 (98.10) 1.2143 (96.00) 1.2078 (96.00) 1.3059 (95.90) 1.4638 (95.10)
    φ2 3.3453 (96.70) 2.8659 (93.60) 1.9095 (89.20) 2.3650 (96.30) 2.8020 (95.30)
    η1 1.3715 (98.10) 1.2804 (96.30) 1.1476 (93.30) 1.5152 (95.10) 1.4841 (95.10)
    φ1 3.3320 (95.70) 3.2564 (93.90) 2.9073 (92.50) 2.7897 (95.70) 3.2580 (95.90)
    η2 1.3684 (98.10) 1.2888 (96.50) 1.1481 (93.30) 1.3593 (95.20) 1.4324 (95.10)
    φ2 3.2757 (95.40) 3.4700 (94.10) 2.8743 (92.00) 2.5880 (95.40) 3.0359 (95.30)
    η1 1.3321 (97.90) 1.2814 (96.50) 1.3062 (97.70) 1.4150 (95.10) 1.5595 (95.10)
    φ1 3.8695 (95.70) 4.1000 (95.00) 2.4081 (90.70) 3.2295 (95.20) 3.6285 (95.40)
    η2 1.3323 (97.90) 1.2743 (97.50) 1.2984 (97.60) 1.2993 (95.10) 1.5309 (95.10)
    φ2 3.8432 (95.70) 3.6813 (93.80) 2.2241 (89.20) 3.0101 (95.40) 3.7577 (95.30)
    1.50 η1 1.2945 (98.40) 1.1344 (97.50) 1.2950 (99.00) 1.3263 (95.40) 1.4661 (95.10)
    φ1 3.3295 (96.00) 2.3355 (91.20) 1.2450 (85.00) 2.6097 (95.80) 2.8005 (95.50)
    η2 1.2922 (98.40) 1.1374 (97.00) 1.2974 (99.00) 1.3173 (95.40) 1.4779 (95.10)
    φ2 3.0707 (95.10) 2.3868 (92.00) 1.2514 (85.00) 2.5960 (96.00) 2.7928 (95.70)
    η1 1.3575 (97.80) 1.2518 (93.10) 1.0686 (89.00) 1.3557 (95.10) 1.4899 (95.10)
    φ1 3.3786 (95.90) 2.7974 (96.00) 3.2368 (95.00) 2.6530 (95.70) 3.0505 (95.40)
    η2 1.3586 (97.80) 1.2550 (90.00) 1.0655 (89.00) 1.3698 (95.10) 1.5571 (95.10)
    φ2 3.4198 (96.00) 2.7809 (97.30) 3.3072 (95.50) 2.5752 (95.90) 2.9714 (95.10)
    η1 1.3389 (97.70) 1.2271 (97.70) 1.2703 (96.50) 1.4095 (95.10) 1.5538 (95.10)
    φ1 3.9441 (95.60) 2.7714 (91.00) 2.0155 (86.50) 3.1312 (95.30) 3.7848 (95.20)
    η2 1.3392 (97.70) 1.2649 (97.80) 1.2704 (96.50) 1.3402 (95.10) 1.5876 (95.10)
    φ2 3.8912 (96.10) 2.8981 (94.10) 2.3108 (93.50) 2.8637 (95.20) 3.5192 (95.40)
    2.00 η1 1.2955 (97.80) 1.2091 (94.00) 1.0787 (88.50) 1.3513 (95.20) 1.4914 (95.10)
    φ1 3.2776 (96.00) 2.6724 (90.30) 1.6138 (81.50) 2.4501 (95.20) 2.8315 (95.50)
    η2 1.2959 (97.80) 1.2158 (95.00) 1.0785 (89.00) 1.3112 (95.10) 1.3761 (95.10)
    φ2 3.2826 (95.80) 3.2747 (89.10) 1.6409 (82.00) 2.5791 (95.70) 2.6419 (95.20)
    η1 1.3741 (98.10) 1.2635 (97.50) 1.2312 (95.00) 1.5040 (95.10) 1.5575 (95.10)
    φ1 3.2902 (95.60) 2.8177 (95.50) 2.3093 (91.00) 2.7558 (95.60) 2.9165 (95.70)
    η2 1.3721 (98.10) 1.2163 (96.90) 1.2317 (95.00) 1.3358 (95.10) 1.5075 (95.10)
    φ2 3.4839 (96.80) 1.9829 (94.10) 2.3256 (90.00) 2.4873 (95.50) 2.8610 (95.50)
    η1 1.3621 (98.80) 1.1872 (97.80) 1.3311 (98.50) 1.4292 (95.10) 1.6857 (95.10)
    φ1 3.8819 (95.40) 2.7582 (90.50) 1.6880 (83.00) 3.4134 (95.50) 3.8733 (95.40)
    η2 1.3616 (98.70) 1.1894 (96.50) 1.3312 (98.50) 1.3625 (95.10) 1.6064 (95.10)
    φ2 4.0346 (95.60) 2.7577 (89.60) 1.6376 (82.50) 3.1719 (95.20) 3.8778 (95.90)

     | Show Table
    DownLoad: CSV
    Table 5.  The length of the difference intervals and CPs for the Type-Ⅰ APHCS under various censoring schemes at (η1=0.5,φ1=1.5,η2=0.75,φ2=2), and (n,m)=(100,40).
    τ Scheme Parm. MLE HPD- MCMC
    Asy-CI Boot-P Boot-T IP Non-IP
    1.00 η1 0.8914 (97.80) 0.9132 (97.00) 1.2320 (98.20) 1.0263 (96.60) 1.0697 (96.80)
    φ1 1.3903 (96.30) 1.3041 (92.10) 1.3350 (93.90) 1.5186 (96.80) 1.5668 (96.70)
    η2 0.8912 (97.80) 0.9139 (95.60) 1.2319 (98.20) 1.0189 (97.00) 1.0852 (95.90)
    φ2 1.3724 (96.30) 1.3033 (94.30) 1.3337 (93.90) 1.4665 (95.40) 1.4522 (95.60)
    η1 0.9619 (98.20) 0.9214 (96.40) 1.1690 (96.40) 1.1027 (96.10) 1.1051 (96.30)
    φ1 1.3194 (95.10) 1.3052 (93.20) 0.9789 (89.90) 1.5071 (96.10) 1.5133 (95.80)
    η2 0.9620 (98.20) 0.9210 (94.00) 1.1687 (96.40) 1.1087 (96.00) 1.1103 (95.70)
    φ2 1.3200 (95.10) 1.3051 (92.00) 0.9792 (89.90) 1.4549 (96.50) 1.5883 (96.80)
    η1 1.0363 (98.70) 1.0598 (96.00) 1.2307 (97.40) 1.2591 (96.80) 1.3123 (96.70)
    φ1 1.9488 (96.50) 1.6959 (93.80) 1.0974 (87.60) 1.7495 (96.40) 1.8589 (95.60)
    η2 1.0335 (98.70) 1.0616 (96.10) 1.2306 (97.40) 1.1915 (98.10) 1.2894 (96.20)
    φ2 1.8231 (96.00) 1.7024 (92.00) 1.0938 (87.50) 1.6761 (96.10) 1.8282 (96.40)
    1.50 η1 0.9056 (98.00) 0.9883 (97.80) 1.2091 (97.30) 1.0291 (96.50) 1.0867 (96.50)
    φ1 1.3506 (95.90) 1.5287 (95.50) 1.1267 (90.70) 1.4908 (96.80) 1.5148 (96.80)
    η2 0.9057 (98.00) 0.9783 (96.20) 1.2091 (97.30) 1.0449 (96.90) 1.0783 (96.90)
    φ2 1.3511 (95.90) 1.5229 (97.30) 1.1244 (90.60) 1.4869 (96.40) 1.5558 (96.50)
    η1 0.9554 (97.90) 0.9531 (96.60) 1.1800 (97.20) 1.1396 (96.50) 1.1784 (96.40)
    φ1 1.3980 (96.10) 1.3992 (95.20) 1.5537 (94.90) 1.4871 (96.40) 1.6021 (96.60)
    η2 0.9553 (97.90) 0.9531 (96.50) 1.1798 (97.20) 1.0866 (98.20) 1.1655 (96.50)
    φ2 1.3974 (96.10) 1.3998 (95.00) 1.5541 (94.90) 1.4839 (96.50) 1.4778 (96.00)
    η1 1.0534 (98.90) 1.0151 (95.90) 1.1238 (94.30) 1.2290 (96.60) 1.2668 (97.60)
    φ1 2.2295 (97.30) 1.5193 (94.80) 1.3973 (92.00) 1.8172 (95.30) 1.8137 (95.70)
    η2 1.0535 (98.90) 1.0144 (96.00) 1.1244 (94.30) 1.1805 (97.00) 1.2669 (97.10)
    φ2 1.9264 (95.90) 1.5228 (92.10) 1.3896 (91.80) 1.7449 (96.10) 1.8340 (95.90)
    2.00 η1 0.9340 (98.50) 0.8923 (94.30) 1.1622 (97.20) 1.1159 (96.40) 1.1727 (96.80)
    φ1 1.4956 (96.00) 1.3205 (93.10) 0.9641 (86.70) 1.5382 (95.60) 1.6283 (95.60)
    η2 0.9354 (98.50) 0.8925 (96.20) 1.1623 (97.20) 1.0734 (95.90) 1.1433 (96.30)
    φ2 1.5470 (96.00) 1.3208 (92.50) 0.9664 (86.70) 1.5729 (96.10) 1.6037 (95.40)
    η1 0.9685 (97.90) 1.0300 (95.70) 1.0994 (93.60) 1.1367 (96.30) 1.1805 (96.90)
    φ1 1.4941 (96.90) 1.6622 (93.80) 1.4330 (93.80) 1.5063 (96.00) 1.5126 (96.20)
    η2 0.9677 (97.90) 1.0310 (96.10) 1.0993 (93.60) 1.1407 (96.80) 1.2110 (96.30)
    φ2 1.4106 (96.20) 1.6638 (97.00) 1.4312 (93.80) 1.4570 (95.30) 1.5855 (97.10)
    η1 1.0517 (98.70) 1.0346 (97.00) 1.2541 (98.70) 1.2426 (97.90) 1.2616 (95.60)
    φ1 1.7832 (95.60) 1.7497 (92.60) 1.0493 (89.00) 1.7403 (95.40) 1.7656 (96.30)
    η2 1.0519 (98.70) 1.0308 (96.00) 1.2544 (98.70) 1.1528 (97.40) 1.3294 (97.00)
    φ2 1.7359 (95.40) 1.7527 (96.10) 1.0591 (89.10) 1.6374 (95.90) 1.8718 (95.90)

     | Show Table
    DownLoad: CSV
    Table 6.  The length of the difference intervals and CPs for the Type-Ⅰ APHCS under various censoring schemes at (η1=0.5,φ1=1.5,η2=0.75,φ2=2), and (n,m)=(200,60).
    τ Scheme Parm. MLE HPD- MCMC
    Asy-CI Boot-P Boot-T IP Non-IP
    1.00 η1 0.7658 (97.90) 0.8187 (95.00) 1.0470 (97.40) 0.9474 (96.20) 0.9559 (96.60)
    φ1 1.0346 (95.30) 1.0814 (96.10) 1.0539 (92.90) 1.1977 (96.50) 1.2560 (97.50)
    η2 0.7659 (97.90) 0.8188 (94.50) 1.0493 (97.40) 0.9166 (96.40) 0.9751 (96.40)
    φ2 1.0419 (95.40) 1.0809 (91.30) 1.0555 (92.90) 1.2261 (96.40) 1.2357 (96.70)
    η1 0.8115 (98.40) 0.8265 (96.10) 1.0135 (95.70) 0.9517 (96.10) 1.0283 (97.40)
    φ1 1.1207 (97.00) 1.0671 (93.90) 1.0063 (93.20) 1.2138 (97.10) 1.2599 (96.50)
    η2 0.8120 (98.40) 0.8262 (95.80) 1.0131 (95.70) 1.0011 (97.10) 1.0698 (97.00)
    φ2 1.1338 (97.10) 1.0674 (92.10) 1.0068 (93.20) 1.2096 (95.60) 1.2587 (97.00)
    η1 0.9324 (98.20) 0.9190 (95.50) 1.1624 (97.50) 1.0811 (96.60) 1.1634 (96.70)
    φ1 1.3076 (95.40) 1.3266 (96.30) 1.1696 (91.60) 1.3732 (96.40) 1.4417 (96.60)
    η2 0.9344 (98.20) 0.9229 (97.50) 1.1622 (97.50) 1.0477 (96.90) 1.1408 (96.50)
    φ2 1.3227 (95.40) 1.3388 (94.00) 1.1832 (92.10) 1.4185 (97.10) 1.4638 (96.60)
    1.50 η1 0.7372 (98.20) 0.7715 (94.00) 0.9491 (96.50) 0.9273 (97.70) 0.9691 (98.20)
    φ1 1.0248 (95.40) 1.0706 (97.10) 0.8938 (92.70) 1.2035 (96.30) 1.2415 (95.90)
    η2 0.7371 (98.20) 0.7719 (96.30) 0.9397 (96.50) 0.9062 (96.60) 0.9551 (97.30)
    φ2 1.0246 (95.40) 1.0706 (92.80) 0.8936 (92.70) 1.1956 (95.70) 1.2517 (95.90)
    η1 0.8343 (97.80) 0.7860 (96.60) 0.8472 (93.90) 1.0631 (96.70) 1.1022 (96.60)
    φ1 1.1153 (95.70) 1.0089 (95.50) 1.5410 (98.10) 1.2906 (95.80) 1.3245 (95.70)
    η2 0.8343 (97.80) 0.7860 (95.20) 0.8275 (93.60) 1.0027 (95.80) 1.0705 (96.50)
    φ2 1.1156 (95.70) 1.0084 (97.00) 1.5044 (97.90) 1.3146 (95.60) 1.3287 (95.70)
    η1 0.9343 (97.70) 0.8947 (97.30) 1.0984 (95.30) 1.0897 (95.50) 1.2016 (95.70)
    φ1 1.2786 (95.10) 1.2631 (96.20) 1.2981 (93.20) 1.3852 (96.80) 1.4450 (96.10)
    η2 0.9356 (97.70) 0.8938 (96.10) 1.0992 (95.40) 1.0585 (95.90) 1.1586 (95.60)
    φ2 1.2895 (95.00) 1.2589 (97.00) 1.2993 (93.20) 1.3527 (95.40) 1.4743 (96.70)
    2.00 η1 0.7505 (97.80) 0.7604 (95.40) 0.8829 (95.20) 0.9468 (96.20) 0.9254 (96.90)
    φ1 1.0300 (95.00) 1.0169 (92.10) 0.7994 (90.70) 1.2518 (97.50) 1.2283 (96.70)
    η2 0.7506 (97.80) 0.7601 (94.00) 0.8824 (95.20) 0.9339 (96.70) 0.9392 (97.00)
    φ2 1.0301 (95.00) 1.0170 (92.00) 0.7988 (90.70) 1.1913 (97.10) 1.2624 (96.50)
    η1 0.8182 (98.20) 0.8085 (94.30) 0.6973 (92.90) 1.0066 (97.10) 1.0384 (97.10)
    φ1 1.0643 (95.70) 0.9421 (95.50) 1.0770 (95.40) 1.2278 (96.00) 1.3069 (95.60)
    η2 0.8185 (98.20) 0.8085 (95.20) 0.6978 (93.00) 0.9937 (96.70) 1.0914 (97.90)
    φ2 1.0669 (95.70) 0.9424 (96.20) 1.0773 (95.40) 1.2683 (96.80) 1.2406 (95.80)
    η1 0.9439 (98.20) 0.9225 (95.80) 1.2227 (97.60) 1.1371 (96.80) 1.1902 (96.80)
    φ1 1.3328 (95.70) 1.1781 (94.20) 0.9708 (89.70) 1.4559 (96.10) 1.4882 (96.50)
    η2 0.9453 (98.20) 0.9225 (93.10) 1.2228 (97.50) 1.0421 (96.10) 1.1436 (96.90)
    φ2 1.3803 (96.10) 1.1806 (92.00) 0.9620 (89.70) 1.4121 (97.60) 1.4809 (97.40)

     | Show Table
    DownLoad: CSV

    From tabulated values, it can be noted that, higher values of n lead to decreasing in MSE depending on the MSEs. With increasing in n and m, the average bias of the estimated values is increasing for the parameters η1, φ2 and decreasing for the parameters η2 and φ1. Also, the average bias of the estimated values of the parameters, φ1 and φ2, of the MLEs is fewer than the BEs (IP and Non-IP) and for parameters, η1 and η2, of the MLEs are higher than the BEs. Furthermore, The BEs under IP for the parameters are better than BEs under Non-IP for the same parameters. Comparing the results in Tables 46, we noted that the HPD intervals under IP perform better than the HPD intervals under Non-IP based on minimum confidence/credible intervals lengths. Also, The AILs of the Asy-CI of the MLEs have the shortest length among the suggested CIs, the AIL decreases in general as n and m increase. In addition, according to the CPs, the MLEs technique has the highest CP among the suggested CPs. Our simulation study's major conclusion is that as the number of steps in a progressive Type-Ⅰ censoring scheme rises over time, the average bias of the estimates and MSEs diminish.

    A real-world data set is used to illustrate the concept and to determine the statistical measures of the MLEs and BEs for IWD under a variety of Type-Ⅰ APHCS using a competing risks model.

    The set of data beneath was first examined by reference [41] and was subsequently examined by reference [21]. The finding was obtained in a laboratory experiment in which male mice were administered a 300-roentgen radiation dosage between the ages of 35 and 42 days (5–6 weeks). For each mouse, the cause of death was identified as reticulum cell sarcoma as 1 (*) and other reasons of death as cause 2 (**), there were n=77 observations remain in the analysis registered below: 40**, 42**, 51**, 62**, 163**, 179**, 206**, 222**, 228**, 249**, 252**, 282**, 317*, 318*, 324**, 333**, 341**, 366**, 385**, 399*, 407**, 420**, 431**, 441**, 461**, 462**, 482**, 495*, 517**, 517**, 524**, 525*, 536*, 549*, 552*, 554*, 557*, 558*, 564**, 567**, 571*, 586*, 586**, 594*, 596*, 605*, 612*, 619**, 620**, 621*, 621**, 622**, 628*, 631*, 636*, 643*, 647*, 647**, 648*, 649*, 651**, 661*, 663*, 666*, 670*, 686**, 695*, 697*, 700*, 705*, 712*, 713*, 738*, 748*, 753*, 761**, 763**.

    From data original, one can create, e.g., five Type-Ⅰ APHC samples with a number of stages m=30 at time censoring τ=400 and removed items Rj (randomly from the surviving items) are assumed to as follows:

    Scheme Ⅰ: R1=nm and R2=...=Rm=0.

    Scheme Ⅱ: R1=...=Rm2=0, R(m2+1)=nm and R(m2+2)=...=Rm=0.

    Scheme Ⅲ: R1=...=Rm1=0 and Rm=nm.

    Scheme Ⅳ: τ=800, R1=nm and R2=...=Rm=03.

    Scheme Ⅴ: τ=800 and R1=R2=...=Rm=0.

    Note that: Scheme Ⅳ can be considered as a progressive Type-Ⅱ censoring scheme, a special case of Type-Ⅰ APHCS. Also, complete sampling can be considered as a special case of Type-Ⅰ APHCS in Scheme Ⅴ when R1=R2=...=Rm=0.

    The MLEs of η1,φ1,η2 and φ2, as well as their related asymptotic CI, two types of bootstrap CI estimates, and AIL for Type-Ⅰ APHC samples under competing risks model with two independent causes of failures as in the given real data set, are shown in Table 7. In addition, BEs were calculated using the MH method with the Non-IP. It is indicated that, while generating samples from the posterior distribution utilizing the MH algorithm, preliminary values of (ηk,φk) are considered as (η(0)k,φ(0)k)=(ˆηk,ˆφk), k=1,2 and (ˆηk,ˆφk) are the MLEs of the parameters(ηk,φk). BEs and HPD intervals were then obtained from the remaining 2000 burn-in samples from the posterior density. Each censoring scheme's relative risk will be calculated.

    Table 7.  ML, Bayesian, and related interval estimates and SEs for real data set based on the Type-Ⅰ APHCS under various censoring schemes with competing risks model.
    Scheme Parm MLE MCMC Relative risk
    Estimate St.E Asy CI Estimate St.E HPD τ1 τ1
    η1 20.1336 15.4900 (6.6826, 90.0117) 5.2757 0.3444 (4.1937, 6.4285) 08166 0.1834
    φ1 2.8010 1.6213 (0.3511, 6.5381) 0.3132 0.0399 (0.0318, 0.7026)
    η2 3.7969 0.3399 (3.1899, 4.5330) 3.6545 0.0931 (3.0620, 4.2262)
    φ2 0.3541 0.0807 (0.2097, 0.5211) 0.3637 0.0056 (0.2230, 0.5097)
    η1 13.2841 6.1005 (6.3409, 36.1274) 5.4296 0.3074 (4.3746, 6.5555) 0.4475 0.5525
    φ1 1.6071 0.6806 (0.5333, 3.1173) 0.4923 0.0220 (0.2212, 0.7746)
    η2 3.4629 0.2850 (2.9436, 4.0647) 3.3675 0.0737 (2.8536, 3.9011)
    φ2 0.3399 0.0657 (0.2218, 0.4767) 0.3398 0.0040 (0.2210, 0.4687)
    η1 11.8853 4.2466 (6.9693, 27.6577) 6.2115 0.2380 (5.2807, 7.1624) 0.5935 0.4065
    φ1 1.0006 0.5207 (0.2719, 2.2565) 0.2561 0.0095 (0.0721, 0.4292)
    η2 4.9741 0.2947 (4.4365, 5.5965) 4.8244 0.0727 (4.3020, 5.3282)
    φ2 0.2359 0.0484 (0.1503, 0.3386) 0.2311 0.0021 (0.1367, 0.3112)
    η1 81.1868 48.3477 (27.3954, 92.1643) 5.8338 0.3392 (4.7744, 7.0125) 0.7736 0.2264
    φ1 3.2885 0.5401 (2.2939, 4.3669) 1.0294 0.0170 (0.7842, 1.2739)
    η2 3.7650 0.4524 (2.9619, 4.7408) 3.5105 0.1584 (2.7611, 4.2735)
    φ2 0.5533 0.0945 (0.3756, 0.7413) 0.5320 0.0072 (0.3609, 0.6900)
    η1 17.7841 9.9707 (6.7734, 59.4942) 4.8931 0.4678 (3.5849, 6.1881) 0.5721 0.4279
    φ1 3.3324 1.0099 (1.6132, 5.5633) 1.2396 0.1014 (0.6567, 1.8698)
    η2 1.8744 0.2256 (1.4695, 2.3569) 1.8517 0.0483 (1.4259, 2.2873)
    φ2 0.7132 0.0976 (0.5287, 0.9093) 0.7133 0.0086 (0.5369, 0.9036)
    *Asy CI- Asymptotic confidence interval, Parm.-Parameter, St.E-Standard error.

     | Show Table
    DownLoad: CSV

    The convergence of MCMC estimation in case of scheme Ⅱ of Type-Ⅰ APHCS for the cause 1, i.e., (η1,φ1) can be showed in Figure 2 and for the cause 2, i.e., (η2,φ2) can be showed in Figure 3.

    Figure 2.  Convergence of MCMC estimates for η1 and φ1 using MH algorithm.
    Figure 3.  Convergence of MCMC estimates for η2 and φ2 using MH algorithm.

    A competing risks model under Type-Ⅰ APHCS technique was explained in this paper. When a fixed number of failure causes are known. Assuming that the lifetime distributions are IWD. The MLEs have been generated, and different CIs for the parameters of the IWD has been suggested using asymptotic distributions and bootstrap CIs. Also provided are the HPD intervals. Different sample sizes and censoring schemes are used to differentiate between different estimators and CIs in a simulation study. Also, using the MH method, BEs based on squared error loss function under the assumption of independent gamma priors were produced. In terms of minimum MSEs, the simulation results show that BEs, provide the importance sampling technique better than the other estimates. It's also important to note that among the various CIs, the HPD intervals have the shortest lengths. We studied two real data sets to illustrate how the suggested estimators perform in real. According to the real data analysis, the Type-Ⅰ APHCS technique appears to be highly effective when the experimenter's primary concern is time and it is not required to terminate the experiment at a predefined number of failures. Finally, future research may be interested in locating a real-life Type-Ⅰ APHCS situation and using the suggested approaches presented here, as well as comparing the results to other censoring schemes.

    This study was funded by Taif University Researchers Supporting Project number (TURSP-2020/279), Taif University, Taif, Saudi Arabia.

    The authors have no conflict of interest regarding publishing this paper.



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