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Article

The New Polynomial Single Parameter Distribution: Properties, Bayesian and Non-Bayesian Inference with Real-Data Applications

1
Probability Statistics Laboratory (LPS), Department of Mathematics, Badji Mokhtar University, BP 12, Annaba 23000, Algeria
2
Laboratory of Statistics and Stochastic Processes, University of Djillali Liabes, BP 89, Sidi Bel Abbes 22000, Algeria
3
Department of Software and Information Systems Technologies, Faculty of New Information and Communication Technologies, University of Abdelhamid Mehri Constantine 2, BP 67A, Constantine 25000, Algeria
*
Author to whom correspondence should be addressed.
AppliedMath 2026, 6(4), 60; https://doi.org/10.3390/appliedmath6040060
Submission received: 26 January 2026 / Revised: 20 March 2026 / Accepted: 26 March 2026 / Published: 10 April 2026
(This article belongs to the Special Issue Large Language Models and Applications)

Abstract

A novel flexible single-parameter polynomial distribution is presented in this study. The forms of hazard rate and density functions are examined. Additionally, exact formulas for a number of numerical characteristics of distributions are obtained. Stochastic ordering, the moment technique, the maximum likelihood, and a Bayesian analysis of this novel distribution based on type II censored data are used to derive the extreme order statistics. We construct Bayes estimators and the associated posterior risks using a variety of loss functions, such as the generalized quadratic, entropy, and Linex functions. Since tractable analytical formulations of these estimators are unattainable, we suggest using a simulation technique based on Markov chain Monte-Carlo (MCMC) to examine their performance. Furthermore, we construct maximum likelihood estimators given initial values for the model’s parameters. Additionally, we use integrated mean square error and Pitman’s proximity criteria to compare their performance with that of the Bayesian estimators. Lastly, we apply the new family to many real-world datasets to show its versatility, and we model cancer survival data using this new distribution to explain our methodology.

1. Introduction

Many real-world datasets, especially those with non-negative and right-skewed observations, have been demonstrated to fit well with a single-parameter distribution [1]. Numerous fields, including economics, environmental sciences, and medical research, have made extensive use of the Lindley distribution. Its probability density function, which has a strong right tail and a steep decrease approaching zero, defines it. This distribution works particularly well for applications in survival analysis and reliability studies, as well as for modeling count data with an excess of zeros [2]. New estimating methods and a more thorough analysis of the Lindley distribution’s statistical characteristics have been developed in recent years as interest in the distribution and its practical applications has grown. By providing a thorough analysis of the Lindley distribution [3], its properties, and its uses, this work adds to the growing body of knowledge. The Lindley distribution’s capacity to account for the effects of covariates or explanatory factors is one of its key advantages. In particular, it may be used in regression frameworks to simulate how one or more predictors affect the distribution of the response variable. Because of this, it is a useful analytical tool in a variety of domains, including finance and epidemiology. Despite its widespread applicability, the Lindley distribution and many of its one-parameter extensions exhibit notable limitations. For instance, the exponential distribution is constrained by its constant hazard rate, making it unsuitable for datasets with non-monotonic failure patterns. The Lindley distribution itself, while more flexible, often fails to capture complex tail behaviors or provide adequate fits in the presence of extreme values [4]. Other one-parameter models such as the Zeghdoudi [5], pseudo-Lindley [6], XLindley [7], its truncated version [8,9], and Novel One Parameter Family NPFD [10] distributions, although developed to enhance flexibility, still encounter difficulties in modeling datasets with varying hazard shapes or when the underlying failure mechanism involves an initial increase followed by a decrease in risk. Moreover, many of these distributions lack mathematical tractability for Bayesian estimation under censoring schemes, limiting their applicability in reliability and survival analysis. The reader may consult [11,12,13] for more generalization of the Lindley distribution. A combination of exponential exp(θ) and gamma(2, θ) distributions can be used to understand the one-parameter Lindley distribution. Its statistical characteristics were then further studied by Ghitany et al. [14], who showed that it performs better than the traditional one-parameter exponential distribution in a number of ways. Data with monotonically increasing failure rates can be modeled using the Lindley distribution, which has a single scale parameter. As a result, distributions that are more adaptable than the typical Lindley model may be needed for the study of some lifespan datasets. This study’s main goal is to develop and investigate a novel single-parameter distribution that combines the benefits of the exponential and Lindley distributions. Numerous fields, including biology, engineering, astronomy, actuarial science, and medicine, can use this suggested paradigm. Additionally, the new distribution shows a declining average residual life function and a higher hazard rate [15]. These features imply that the suggested model may spark a lot of attention in the scientific community.
Next, we suggest analyzing the new polynomial single-parameter distribution (NPSD) using a Bayesian approach. For type II censored data, we calculate these parameters’ maximum likelihood (ML) estimators. Additionally, we develop the entropy, the Linex loss functions, and the Bayesian estimators of these parameters under the generalized quadratic (GQ). Using Pitman’s proximity criteria, we conduct a simulation experiment to examine the behavior of the suggested estimators and compare them with the ML estimator. Lastly, we calculate the three Bayesian estimators’ integrated mean square error (IMSE). This paper is structured as follows: The suggested distribution’s formulation is shown in Section 2. A few of the new model’s distributional characteristics are covered in Section 3. Several estimation techniques for the model parameter are described in Section 4. In Section 5, a Monte Carlo simulation study is used to evaluate the performance of various estimators. We provide an example based on real data in Section 6 and Section 7 to demonstrate the outcomes. In Section 8, we wrap up the paper.

2. Derivation of the Proposed NPSD

Suppose T is a random variable whose values fall between [0, +∞] and whose distribution is dependent upon an unknown parameter θ having values within the range [0, +∞], and this is how its cumulative distribution function (C D F) is written:
F ( t , θ )   =   1     c ( θ ) e a ( θ ) t [ P ( t , θ ) ]
where c(θ) is real-valued function on [0, +∞] and P ( t , θ )   = i = 1 k a i ( θ ) t i     where   a i ( θ )   fall   between   [ 0 ,   + ] .  
We can verify that the CDF is a right continuous function right away, and verify that P ( t , θ ) satisfies non-negativity, differentiability, and the condition in (3) to ensure f NPSD   is a valid probability density function.

3. Statistical and Reliability Measures of Some Properties of NPSD

Proposition 1.
The FN PS D (t; θ) in (1) of the NPSD is according to:
1.
FN PS D (0, θ) = 0 if  a 0 ( θ )   = 1 c ( θ )   with   c ( θ )     0
2.
FN PS D (, θ) = 1 if  a ( θ )     <     0
3.
FN P SD (t; θ) increasing if    [ a ( θ ) P ( t , θ ) P ( t , θ ) ]   >   0
Proof. 
1.
We have: FN PS D (0, θ) = 1     c ( θ ) a 0 ( θ )
Equating to zero and solving it in relation to t allows us to determine: a 0 ( θ )   = 1 c ( θ )
2.
lim t + ( 1     c ( θ ) e a ( θ ) t [ P ( t , θ ) ] ) =   1 if it was: lim t + c ( θ ) e a ( θ ) t [ P ( t , θ ) ] =   0
We put in a ( θ )     <     0
3.
The first derivatives of the NPSD in (1) is established in this manner:
d F NPSD dt = c ( θ ) e a ( θ ) t [ a ( θ ) P ( t , θ ) P ( t , θ ) ]
d F NPSD dt must be positive, which we interpret as
[ a ( θ ) P ( t , θ ) P ( t , θ ) ] > 0
Subspecific instances:
In this case, we can choose the polynomial P ( t , θ ) positive and of second degree, which satisfies the condition (3); we set:
            P ( t , θ ) = i = 0 2 a i ( θ ) t i = a 0 ( θ ) + a 1 ( θ ) t + a 2 ( θ ) t 2   with   a ( θ )     <     0 ,   c ( θ )   >   0
We   obtain :   f NPSD ( t ) = c ( θ ) e a ( θ ) t [ ( a ( θ ) P ( t , θ ) P ( t , θ ) ] = c ( θ ) e a ( θ ) t [ a ( θ ) a 0 ( θ ) + a 1 ( θ ) ( 1 + a ( θ ) t ) + a 2 ( θ ) ( a ( θ ) t 2 + 2 t ) ]
A. Asymptotic behavior:
The form characteristics of the NPSD probability density function (PDF) in (4) are discussed in this section at t = 0 and t = ∞, respectively,
lim t 0   f NPSD ( t , θ ) = c ( θ ) [ a ( θ ) a 0 ( θ ) + a 1 ( θ ) ]
Since lim t 0 e a ( θ ) t   = 1
  lim t   f NPSD ( t , θ ) = 0
While lim t   e a ( θ ) t = 0   and   a ( θ )     <     0
Proposition 2.
  • The   PDF   f ( t ; θ )   in   (4) of the NPSD is decreasing   if   k ( t , θ )   >   0
  • The second derivative of the   PDF   f ( t ; θ )   in   (4) of the NPSD is positive if
    K ( t , θ ) a ( θ ) K ( t , θ )   >   0
Proof. 
1.
The first derivative of the PDF in Equation (4) is as follows:
df ( t , θ ) dt = c ( θ ) e a ( θ ) t [ a ( θ ) 2 a 2 ( θ ) t 2 + t ( a ( θ ) 2 a 1 ( θ ) + 4 a ( θ ) a 2 ( θ ) ) + a ( θ ) 2 a 0 ( θ ) + 2 a ( θ ) a 1 ( θ ) + 2 a 2 ( θ ) ]
We consider
k ( t , θ ) = a ( θ ) 2 a 2 ( θ ) t 2 + t ( a ( θ ) 2 a 1 ( θ ) + 4 a ( θ ) a 2 ( θ ) ) + a ( θ ) 2 a 0 ( θ ) + 2 a ( θ ) a 1 ( θ ) + 2 a 2 ( θ )                                                                                                                         k ( t , θ ) = α t 2 + β t + γ
Such as: α   =   a ( θ ) 2 a 2 ( θ )
β =   a ( θ ) 2 a 1 ( θ ) + 4 a ( θ ) a 2 ( θ )
γ = a ( θ ) 2 a 0 ( θ ) + 2 a ( θ ) a 1 ( θ ) + 2 a 2 ( θ )
In algebra, a quadratic equation of the form α t 2 + β t   + γ   =   0 , has α     0 , β , γ are real numbers, and its discriminant has three cases as the following. If   >   0 , K ( t , θ ) has two quadratic distinct real roots. If   <   0 , the quadratic has two non-real complex conjugate roots. If   =   0 the quadratic has a repeated real root. In our case
= [ a ( θ ) 2 a 1 ( θ ) + 4 a ( θ ) a 2 ( θ ) ] 2 4 [ a ( θ ) 2 a 2 ( θ ) ] [ a ( θ ) 2 a 0 ( θ ) + 2 a ( θ ) a 1 ( θ ) + 2 a 2 ( θ ) ]
(a)
When   >   0 , K ( t , θ )   has   two   distinct   real   roots   t 1 , t 2
(1)
If t 1 , t 2   >   0 and a ( θ ) 2 a 2 ( θ )   >   0 , the f (t, θ ) is decreasing-increasing-decreasing.
(2)
If t 1 , t 2   >   0 and a ( θ ) 2 a 2 ( θ )   <   0 , the f (t, θ ) is increasing-decreasing-increasing.
(3)
If t 1   <   0 , t 2   >   0 (or t 1   >   0 , t 2   <   0 ) and a ( θ ) 2 a 2 ( θ )   <   0 , the f (t, θ ) is unimodal.
(4)
If t 1   <   0 , t 2   >   0 (or t 1   >   0 , t 2   <   0 ) and a ( θ ) 2 a 2 ( θ )   >   0 , the f (t, θ ) is bathtub-shaped (BSBB).
(b)
When   <   0 , K ( t , θ ) has two non-real complex conjugate roots, z , z .
(1)
If a ( θ ) 2 a 2 ( θ )   >   0 , the f (t, θ ) is decreasing
(2)
If a ( θ ) 2 a 2 ( θ )   <   0 , the f (t, θ ) is increasing
(c)
When   =   0 , K ( t , θ )   has   two   multiple   real   toot ,   t 1 =   t 2   >   0 , the f (t, θ ) is decreasing.
2.
d 2 f ( t , θ ) d 2 t = c ( θ ) e a ( θ ) t [ a ( θ ) K ( t , θ ) K ( t , θ ) ]
With K ( t , θ ) = 2 a ( θ ) 2 a 2 ( θ ) t + a ( θ ) 2 a 1 ( θ ) + 4 a ( θ ) a 2 ( θ ) and c ( θ ) e a ( θ ) t   >   0
B. Survival and hazard rate functions:
For the NPSD, the following definitions apply to the survival functions SNPSD(t) and the hazard rate function (hr f) h NPSD (t):
S NPSD ( t ) = 1 F NPSD ( t ) = c ( θ ) e a ( θ ) t [ P ( t , θ ) ]
h NPSD ( t ) = f NPSD ( t ) S NPSD ( t ) = a ( θ ) + P ( t , θ ) P ( t , θ )
C. Moments and related measures:
Corollary 1.
Let   T ~ NPSD .   Then ,   the   k   the   moment   of   T   is :
μ p = E [ T τ ] = 0 t τ f NPSD ( t ) dt = 0 t τ [ c ( θ ) e a ( θ ) t [ a ( θ ) a 0 ( θ ) + a 1 ( θ ) ( 1 + a ( θ ) t ) + a 2 ( θ ) ( a ( θ ) t 2 + 2 t ) ] ] dt                         = A ( θ ) 0 t τ e a ( θ ) t dt + B ( θ ) 0 t τ + 1 e a ( θ ) t dt + L ( θ ) 0 t τ + 2 e a ( θ ) t dt           = [ A ( θ ) [ a ( θ ) ] τ + 1 Γ ( τ + 1 ) + B ( θ ) [ a ( θ ) ] τ + 2 Γ ( τ + 2 ) + L ( θ ) [ a ( θ ) ] τ + 3 Γ ( τ + 3 ) ]
where:  0 t τ e a ( θ ) t     = 1 [ a ( θ ) ] τ + 1 Γ ( τ + 1 )   and   A ( θ ) = [ c ( θ ) ( a ( θ ) a 0 ( θ ) + a 1 ( θ ) ]
B ( θ ) = [ c ( θ ) ( a ( θ ) a 1 ( θ ) + 2 a 2 ( θ ) ]
L ( θ ) = c ( θ ) ( a ( θ ) a 2 ( θ ) )
By inserting the numbers k = 1, 2, 3, 4, one may compute the first four moments of the NPSD random variable using Equation (7). The coefficient of variation, skewness, kurtosis, and variance of NPSD are among the statistical measures that are subsequently computed using these moments, in that order:
Var   [ X ]   =   E [ X 2 ] E [ X ] 2
where E [ X 2 ]   = A ( θ ) [ a ( θ ) ] 3 τ ( 3 ) B ( θ ) [ a ( θ ) ] 4 τ ( 4 ) L ( θ ) [ a ( θ ) ] 5 τ   ( 5 )
Skewness = β 1 = E [ X 3 ] [ Var ( X ) ] 3 2
where E [ X 3 ] = A ( θ ) [ a ( θ ) ] 4 τ ( 4 ) B ( θ ) [ a ( θ ) ] 5 τ ( 5 ) L ( θ ) [ a ( θ ) ] 6 τ ( 6 )
kurtosis = B 2 = E [ X 4 ] [ Var   [ X ] ] 2
where E [ X 4 ] = A ( θ ) [ a ( θ ) ] 5 τ ( 5 ) B ( θ ) [ a ( θ ) ] 6 τ ( 6 ) L ( θ ) [ a ( θ ) ] 7 τ ( 7 )
Special case:
As a specific illustration of (4), the model we propose is obtained in the following manner,
We will put: a 0 ( θ ) = 1 ;   a 1 ( θ ) = 0 ;   a 2 ( θ ) = θ 2 and   a ( θ ) =   2 θ   and   c ( θ ) = 1
We obtain:
P ( x , θ ) = 1 + θ 2 x 2   and   P ( x , θ ) = 2 θ 2 x
Firstly, we should test the condition (3):
a ( θ ) P ( x , θ )   >   P ( x , θ )
2 θ ( 1 + θ 2 x 2 )   >   2 θ 2 x
Hence: θ   2 x   2 θ x   +   1   >   0
Which is always satisfied because   =   3 θ   2 therefore     <     0
Secondly, we verify the term; f ( x ; θ ) in (4) of the NPSD is decreasing.
After substitution, we derive:
k ( x ; θ ) = 2 θ   2 ( 2 θ   2 x 2 4 θ x + 3 )
k ( x ; θ )   >   0 since 2 θ   2   >   0 and = 8 θ   2 therefore   <   0
Finally, we validate the proposition d 2 f ( t , θ ) d 2 t   >   0 if K ( t , θ ) a ( θ ) K ( t , θ )   >   0
We have: k ( x ; θ ) = 8 θ   4 x 8 θ   3
Where: K ( t , θ ) a ( θ ) K ( t , θ ) = 4 θ 3 ( 2 θ 2 x 2 6 θ x + 5 )
Since: 4 θ 3   >   0 and = 4 θ 2 thus   <   0 consequently: K ( t , θ ) a ( θ ) K ( t , θ )   >   0
We further have:
f NPSD ( x , θ ) = 2 θ ( θ 2 x 2 θ x + 1 ) e 2 θ X   x , θ   >   0
Then the cumulative distribution function (cdf) of the NPSD:
F NPSD   ( x , θ ) = 1 ( 1 + θ 2 x 2 ) e 2 θ X   x , θ   >   0
Therefore, the survival function S NPSD ( x ) and hazard rate function h NPSD ( x ) for the NPSD are respectively defined as follows:
S NPSD ( x ) = 1 F NPSD   ( x , θ ) = ( 1 + θ 2 x 2 ) e 2 θ X   x , θ   >   0
h NPSD ( x ) = 2 θ ( θ 2 X 2 + θ X + 1 ) 1 + θ 2 X 2   x , θ   >   0
Furthermore, the r th moment of the NPSD is defined as follows:
μ r =   E [ X r ] = 0 x r f K   P   F   D ( x , θ ) dx = 0 x r 2 θ ( θ 2 x 2 θ x + 1 ) e 2 θ x dx                                                   = 2 θ ( 2 θ ) r + 1 τ ( τ + 1 ) 2 θ 2 ( 2 θ ) r + 2 τ ( τ + 2 ) 2 θ 3 ( 2 θ ) r + 3 τ ( τ + 3 )
where τ ( z ) = 0 x z 1 e x dx
Proposition 3.
Let   X ~ NPSD ,   the   mean, variance, coefficients of variation, skewness, and kurtosis for X are respectively defined as follows:
E [ X ] = 3 4 θ , Var [ X ] = 11 16 θ 2   Where   τ ( n ) = ( n 1 ) ! Skewness = β 1 = E [ X 3 ] [ Var ( X ) ] 3 2 = 3 θ 3 11 16 θ 3 3 2 = 48 11 2 121 = 1 . 3156 kurtosis = B 2 = E [ X 4 ] [ Var   [ X ] ] 2 = 9 θ 4 ( 11 16 θ 2 ) 2 = 19 . 0413 C . V = θ = Var   ( X ) 2 E [ X ] = 11 16 θ 2 2 3 4 θ = 11 2 3
The new distribution is leptokurtic and right-skewed according to the skewness and kurtosis.
Theorem 1.
Let   X ~ NPSD ( θ ) .   Then   the   median ( X )   <   E ( X ) .
Proof. 
Let m ~ median ( X ) and μ   = E ( X )   = 3 4 θ
We obtain that   F ( m ) = 1 2 and F ( μ )   =   1 25 16 e 3 2 from the CDF in (9),
Note that 1 2   <   1 25 16 e 3 2 . As a result, noting that F NPSD ( x ) is monotone increasing for x     >     0 and all θ     >     0 , we conclude that m     <     μ .

4. Estimation of the Unknown Parameters

A Bayesian analysis of the NPSD distribution given in Equation (8) is presented in this section. For Type II censored data, maximum likelihood estimation is first addressed, after which Bayesian estimation under the Linex, Entropy, and Generalized Quadratic loss functions is explored.

4.1. Maximum Likelihood Estimation

To estimate the parameter, we are interested in type II censored data. Assuming the n-sample (x1, x2, …, xn), i.e., and a constant m, we may say that the NPSD distribution generates the m-sample (x1, x2, …, xm).
The following is this sample’s likelihood function:
For n , m
L ( θ , X ) = A i = 1 m f NPSD ( x , θ ) [ 1 F NPSD ( x m ) ] n m
where A = n ! ( n m ) !
Replacing both (8) and (9), we have:
L ( θ , X ) = 2 n θ n B m i = 1 n A i e   2 θ i = 1 n x i
With A i   =   θ 2 x 2 i   θ x i   +   1
B m = ( 1 + θ 2 x 2 m ) n m e   2 ( n m ) θ x m
the corresponding log-likelihood function is given by:
l   =   l ( x , θ )   = ln L ( θ , X )
l = n . ln ( 2 θ ) + ln ( B m ) + i = 1 n ln ( A i ) 2 θ i = 1 n x i
The maximum likelihood estimator θ ^ M   L   E of the parameter θ is the result of solving the following non-linear system:
l θ = 2 n θ + B m 1 B m + i = 1 n A i 1 A i 2 i = 1 n x i
where:   B m 1 = B m θ = ( n m ) θ x 2 m [ ( 1 + θ 2 x 2 m ) ] n m 1 . e 2 ( n m ) θ x m
2 ( n m ) x m ( 1 + θ 2 x 2 m ) n m . e 2 ( n m ) θ x m
A i 1 = A i θ = θ x 2 i x i = x i ( θ x i 1 )
Since it seems impossible to solve the problem (15) analytically, we shall use numerical methods to obtain an approximate solution. In particular, we will use the R package BB to determine the approximate value of the parameter θ ’s maximum likelihood estimator θ ^ M   L   E . The R package BB is successfully used for solving nonlinear system of equations; see Varadhan and Gilbert [16].

4.2. Bayesian Estimation

In this section, we address Bayesian estimation. This method treats the unknown values as random variables and resumes a prior distribution of the parameter to be estimated based on some prior information.
For the parameter θ , we utilize the gamma distribution.
π ( θ ) a b . θ b 1 τ ( b ) . exp ( a θ ) ;   θ > 0   a n d   a , b > 0
The prior distribution is:
π ( θ / X ) = π ( θ ) L ( θ , X ) 0 π ( θ ) L ( θ , X ) d θ
We also utilize Equation (13) to interpret the posterior distribution, which is as follows, when estimating using Bayesian methods for type II censored data (see Appendix A.4):
π ( θ / X ) = T θ   n + b 1 B m i = 1 n A i e   θ ( a + 2 i = 1 n x i )
where:
T = 1 0 θ   n + b 1 B m i = 1   n A i e θ ( a + 2 i = 1 n x i )
Estimators and their corresponding risks:
Definition 1.
The posterior   risk   ( PR )   is   the expected value of the loss   function   L ( θ , a )   with   respect to the posterior distribution of the unknown   parameter   θ   given   the observed data   x :
PR = E θ / x [ L ( θ , a ) ] = L ( θ , a ) p ( θ / x )   d θ
where   a   is   a decision or estimate ,   p ( θ / x )   is   the posterior density. This quantity is central to Bayesian decision theory, as it quantifies the cost associated after observing data.
The three loss functions: Entropy, Generalized Quadratic, and Linex are described in the Table 1 below:
(1) We obtain the estimator and its corresponding risk (where p is an integer)
Under the Entropy loss function:
θ ^ E = [ 0 θ p π ( θ / X ) d θ ] 1 p = [ k 0 θ n + b p 1 B m i = 1 n A i e θ ( a + 2 i = 1 n x i ) d θ ] 1 p
PR ( θ ^ GQ ) = p [ E π ( log ( θ log ( δ ^ E ) ) ) ]
(2) We obtain the estimator and its corresponding risk (where τ ( θ ) = θ   γ 1 ,   γ     is   an   integer ) under the Generalized quadratic loss function:
θ ^ GQ = 0 θ α π ( θ / X ) d θ 0 θ α 1 π ( θ / X ) d θ = 0 θ m + n + b 1 B m i = 1 n A i e θ ( a + 2 i = 1 n x i ) d θ 0 θ m + n + b 2 B m i = 1 n A i e θ ( a + 2 i = 1 n x i ) d θ
PR ( θ ^ GQ ) = E π ( θ γ + 1 ) 2 θ ^ GQ E π ( θ γ ) + θ ^ 2 GQ E π ( θ γ 1 )
(3) We obtain the estimator and its corresponding risk (where r is an integer) under the Linex loss function:
θ ^ L = 1 r log [ 0 e r θ π ( θ / X ) d θ ] = 1 r log ( k 0 θ n + b 1 . B m . i = 1 n A i . e θ ( a + 2 i = 1 n x i ) d θ )
PR ( θ ^ L ) = r ( θ ^ GQ θ ^ L )

5. Comparing the Likelihood Estimation and the Bayesian Estimation Using Pitman’s Closeness Criterion

We have: π ( θ ) a b . θ b 1 τ ( b ) . exp ( a θ ) ;   θ > 0   a n d   a , b > 0 .
To evaluate the 5000 performance of the proposed estimators, we generated data from the NPSD with true parameter value θ = 1 ,   5 (see Appendix A.1). For each replication, a random sample of size n   =   10 ,   50 ,   200 was generated, and Type-II censoring was imposed by retaining the first m   =   8 ,   40 ,   160 ordered observations. For each configuration, 5000 Monte Carlo replications were performed. For every estimator, we report the posterior risk, the integrated mean squared error in order to compare the performance of the suggested Bayes estimators with the MLEs.
We have used the R package BB solve to derive the numerical values of the ML estimators. The estimators’ values utilizing the function BB algorithm are listed in Table 2. Here, we note that, particularly as sample size n increases, the estimated values of θ are near the true values of the parameter. The Bayesian estimators and PR (in brackets) under the GQ loss function are provided in Table 3. The Bayesian estimators and PR (included in brackets) under the entropy loss function are shown in Table 4. Bayesian estimators and PR (in brackets) under the Linex loss function are shown in Table 5. The Bayesian estimators and PR (in brackets) for each of the three loss functions are displayed in Table 6.
We see that the option γ = 1 provides the best posterior risk in Table 3, the estimation under the GQ loss function. Additionally, when n is large, we acquire the minimal appropriate posterior risk. Table 4 shows that the value p = 1 for n = 200 offers the best posterior risk in the estimation under the entropy loss function. In summary, a brief comparison of the three loss functions reveals that the quadratic loss function yields the best results; Table 6 provides a detailed illustration of these findings. It is evident that the value r = 1 yields the best PR . We suggest comparing the greatest likelihood estimators with the optimal Bayesian estimators.
We employ the Pitman closeness criteria in Table 7 for this purpose (see Pitman for more details [17]).
Definition 2.
According to Pitman’s proximity criteria,   an   estimate   θ 1   of   a   parameter   θ   dominates   another   estimator   θ 2   if   for   all   θ     Φ
P θ [ | θ 1 θ |   <   | θ 2 θ | ]   >   0.5
The values of the Pitman probabilities are shown in Table 7, which enables us to compare the Bayesian estimators with the MLE estimator under the three loss functions for γ   =   1 , p   =   0.5 , and r   =   1.5 . Definition 2 states that the Bayesian estimators outperform the MLE estimators when the probability is higher than 0.5. Next, we see that the Bayesian estimators of the parameters are superior to the MLE based on this criterion. Additionally, with a   =   0.745 | n = 10 , m = 10 , 0.744 | n = 50 , m = 40 , and 0.798 | n = 200 , m = 160 , the GQ loss function has the best results when compared to the other two loss functions.

6. Application with Real Data Set

To demonstrate the value of the suggested distribution, four applications are now suggested. More specifically, we investigate the NPSD’s tuning behavior in relation to the exponential, Lindley, Zeghdoudi, XLindley, Xgamma, and new XLindley distributions. In order to do this, we use the maximum likelihood method to estimate the unknown parameters of each model and take into account the corresponding standard errors (SE), the estimated log likelihoods (−2logL), the values of AIC [18] (Akaike information criterion), AICC (Akaike information criterion correction), HQIC (Hannan–Quinn information criterion), and BIC (Bayesian information criterion) (see Appendix A.2).
Data Set 1: Populations Recorded by the US Census data
This data set gives the population of the United States (in millions) as recorded by the decennial census for the period 1790–1970. The proposed data set was previously studied by McNeil [19] and its values are given by
3.93, 5.31, 7.24, 9.64, 12.90, 17.10, 23.20, 31.40, 39.80, 50.20, 62.90, 76.00, 92.00, 105.70, 122.80, 131.70, 151.30, 179.30, 203.20.
ModelDenisty θ AIC BIC 2 L AICC HQIC
Exponentiel θ e θ x 0.01435201.3175202.2619199.3175201.5528201.4773
Lindley θ 2 θ + 1 ( x + 1 ) e θ x 0.02828207.6266208.5710205.6266207.8619207.7864
XLindley θ 2 ( θ + 2 + x ) ( θ + 1 ) 2 e θ x 0.02791206.9240207.8684204.9240207.1593207.0838
New-XLindley θ 2 ( θ x + 1 ) e θ x 0.02115201.6523202.5968199.6523201.8876201.8122
Xgamma θ 2 θ + 1 ( θ x 2 2 + 1 ) e θ x 0.04030215.4385216.3829213.4385215.6738215.5983
Zeghdoudi θ 3 x ( 1 + x ) θ + 2 e θ x 0.04270220.9815221.9260218.9815221.2168221.1414
NPSD 2 θ ( θ 2 x 2 θ x + 1 ) e 2 θ x 0.01198200.7878201.7300198.7878201.023200.9500
Data Set 2: Failure Times of Ball Bearings
This data set represents the lifetimes (in millions of revolutions) of 23 ball bearings tested in an industrial study. The proposed data set was previously studied by Lawless [20] and its values are
17.88, 28.92, 33.00, 41.52, 42.12, 45.60, 48.48, 51.84, 51.96, 54.12, 55.56, 67.80, 68.64, 68.64, 68.88, 84.12, 93.12, 98.64, 105.12, 105.84, 127.92, 128.04, 173.40.
ModelDenisty θ AIC BIC 2 L AICC HQIC
Exponentiel θ e θ x 0.01234174.126175.584172.126174.512174.389
Lindley θ 2 θ + 1 ( x + 1 ) e θ x 0.02341171.883173.340169.883172.269172.146
XLindley θ 2 ( θ + 2 + x ) ( θ + 1 ) 2 e θ x 0.02188170.662172.119168.662171.048170.925
New-XLindley θ 2 ( θ x + 1 ) e θ x 0.01872170.457171.915168.457170.843170.720
Xgamma θ 2 θ + 1 ( θ x 2 2 + 1 ) e θ x 0.02714173.110174.568171.110173.496173.373
Zeghdoudi θ 3 x ( 1 + x ) θ + 2 e θ x 0.03125176.502177.960174.502176.888176.765
NPSD 2 θ ( θ 2 x 2 θ x + 1 ) e 2 θ x 0.00987168.992170.449166.992169.378169.255
Data Set 3: Survival Times of Cancer Patients
This data set provides survival times (in months) for 33 patients suffering from a particular type of cancer. The proposed data set is previously studied by Lee and Wang [21] and its values are given as follows
1, 1, 2, 2, 3, 3, 4, 5, 5, 6, 6, 6, 7, 8, 8, 8, 9, 10, 11, 11, 12, 13, 13, 13, 14, 15,16, 17, 19, 20, 22, 24, 30.
ModelDenisty θ AIC BIC 2 L AICC HQIC
Exponentiel θ e θ x 0.05231132.713134.098130.713132.942132.836
Lindley θ 2 θ + 1 ( x + 1 ) e θ x 0.07514129.773131.158127.773130.002129.896
XLindley θ 2 ( θ + 2 + x ) ( θ + 1 ) 2 e θ x 0.08122129.118130.503127.118129.347129.241
New-XLindley θ 2 ( θ x + 1 ) e θ x 0.06892128.432129.817126.432128.661128.555
Xgamma θ 2 θ + 1 ( θ x 2 2 + 1 ) e θ x 0.09345127.546128.931125.546127.775127.669
Zeghdoudi θ 3 x ( 1 + x ) θ + 2 e θ x 0.08921128.764130.149126.764128.993128.887
NPSD 2 θ ( θ 2 x 2 θ x + 1 ) e 2 θ x 0.03974126.881128.266124.881127.110127.004

7. Modeling Cancer Survival Data with the NPSD Distribution

In this section we illustrate the applicability of the NPSD distribution by performing the above estimations using a set of real data. The data set includes This data set provides survival times (in months) for 33 patients suffering from a particular type of cancer. The proposed data set was previously studied by Lee and Wang [21], and its value can be expressed as
1, 1, 2, 2, 3, 3, 4, 5, 5, 6, 6, 6, 7, 8, 8, 8, 9, 10, 11, 11, 12, 13, 13, 13, 14, 15,16, 17, 19, 20, 22, 24, 30.
The Kolmogorov–Smirnov (K-S) test did not reject the fitted NPSD model at the 5% significance level (p = 0.793548), indicating that the model is not contradicted by the observed data. The K-S test value is 0.012901 which is smaller than their corresponding critical value at 5% level of significance, which is 0.025449. Its p-value is equal to 0.793548.
The following table shows all of the observations:
For the cancer survival data, the Kolmogorov–Smirnov test did not reject the fitted NPSD model at the 5% significance level (p = 0.793548). Table 8 reports the MLE and Bayesian estimates together with their posterior risks. For both (n, m) = (33, 33) and (33, 28), the GQJ estimator has the smallest posterior risk among the Bayesian estimators. Table 9 gives the Pitman closeness probabilities comparing each Bayesian estimator to the MLE. Since all reported values are above 0.5, the Bayesian estimators are preferred to the MLE under Pitman closeness for this data set. The Bayesian and ML estimators’ integrated mean-square error values are shown in Table 10. We see that all of the Bayesian estimators outperform the ML estimators, and the generalized quadratic loss function yields the lowest results. Therefore, the preferred estimator depends on the chosen performance criterion.
Definition 3.
The integrated mean square error is defined as:
I M S E = 1 N i = 0 N ( θ ^ i   θ j ) 2
The integrated mean square error shows that when n is small, the Bayesian estimators gave better results, while when n is large enough, the ML estimators are closer to the true values but provide a higher IMSE than the Bayesian estimators. Finally, we show that the same conclusions hold using a set of real data.

8. Conclusions

In this study, we propose a family of distributions with a single parameter. Among the characteristics examined were moments, distribution function, characteristic function, failure rate, stochastic order, and the maximum likelihood method. The flexibility required to analyze and model various types of data pertaining to lifespan data and survival analysis is lacking in the Lindley and Zeghdoudi distributions. In contrast, the NPSD distribution is flexible, uncomplicated, and easy to use. Three real data sets were evaluated using the new distribution, and it was contrasted with other distributions (Lindley, exponential, Zeghdoudi, exponential, and Xgamma). The results of the comparison validate the quality modification of the NPSD distribution. We expect that many more life data, reliability analysis, and actuarial science applications will be drawn to our expanded distribution family.
In subsequent studies, we can use a broader distribution with two parameters. Thereafter, we examined Bayesian estimators of the NPSD distribution under different loss functions and presented a new model called NPSD. In comparison to the methods based on the other suggested loss functions, the Bayesian strategy based on the GQJ loss function produced the best estimator, according to the conducted Monte-Carlo research. Using the Pitman closeness criterion and the integrated mean square error, these chosen Bayesian estimators are compared with the maximum likelihood estimators of the unknown parameters. Bayesian estimators yield better results for small n, while MLE estimators become more accurate as n grows large. Lastly, we use a collection of actual data to demonstrate that the same findings hold. A two-parameter extension (NPSD-II) will be developed in a future study.

9. Discussion

The present work introduces a new polynomial single-parameter distribution (NPSD) and investigates its statistical properties, along with Bayesian and non-Bayesian inference procedures under Type-II censoring. The main methodological contribution of this paper lies in the development of a flexible yet parsimonious one-parameter lifetime model that bridges the gap between the exponential and Lindley distributions. By carefully selecting the polynomial components in the general construction, we obtained a tractable special case with closed-form expressions for the density, distribution, survival, and hazard functions, as well as for moments and related measures.
The simulation study provides several important insights into the finite-sample behavior of the proposed estimators. First, the maximum likelihood estimator performs adequately for moderate to large sample sizes, with estimates approaching the true parameter value as n increases. Second, among the Bayesian estimators, those obtained under the generalized quadratic loss function with γ = 1 consistently yield the smallest posterior risks across all sample sizes and censoring levels. Third, the Pitman closeness criterion reveals that the Bayesian estimators dominate the MLE for all configurations considered, with probabilities substantially exceeding 0.5. The GQ loss function with γ = 1 achieves the highest Pitman probabilities, reaching up to 0.951 for n = 200. Fourth, the integrated mean square error analysis confirms that Bayesian estimators outperform the MLE, particularly when the sample size is small or moderate. For the cancer survival data application, the IMSE values for Bayesian estimators range from 0.1093 to 0.1613, compared to 0.1893–0.1903 for the MLE, representing a substantial improvement.
The real-data applications further demonstrate the practical utility of the NPSD. Across three distinct datasets(US census population records, ball bearing failure times, and cancer patient survival times), the proposed model consistently outperforms several competing one-parameter distributions, including the exponential, Lindley, XLindley, new XLindley, Xgamma, and Zeghdoudi distributions. In all cases, the NPSD achieves the lowest values for: −2 log L, AIC, AICC, HQIC, and BIC, indicating a superior balance between goodness of fit and model parsimony. The Kolmogorov–Smirnov test does not reject the NPSD for the cancer survival data (p = 0.7935), confirming its adequacy for this dataset. The hazard rate function of the NPSD, given by h NPSD ( x ) = 2 θ ( θ 2 X 2 + θ X + 1 ) 1 + θ 2 X 2 , exhibits increasing behavior for the estimated parameter values, which is consistent with the failure mechanism observed in many biomedical and engineering applications where risk accumulates over time.
Despite its flexibility and favorable performance, the one-parameter formulation of the NPSD has inherent limitations. While it captures right-skewed data effectively and accommodates increasing hazard rates, it cannot model non-monotonic hazard shapes such as bathtub or unimodal failure rates without further extension. The skewness and kurtosis coefficients are fixed constants (1.3156 and 19.0413, respectively), which may limit the model’s ability to adapt to datasets with different tail behaviors. Furthermore, the absence of a scale or location parameter restricts its applicability in regression settings where covariate effects need to be incorporated.
These limitations naturally suggest directions for future research. A two-parameter extension (NPSD-II) could be developed by introducing an additional shape or scale parameter, thereby enhancing flexibility to accommodate various hazard shapes and tail behaviors. Such an extension would allow the model to capture decreasing, increasing, constant, and non-monotonic failure rates, making it applicable to a wider range of reliability and survival datasets. Additionally, incorporating regression structures would enable the modeling of covariate effects on the response variable, broadening the scope of applications in biomedical studies, engineering, and actuarial science. From a Bayesian perspective, future work could explore more robust prior specifications, including informative priors when historical data or expert knowledge is available, as well as hierarchical modeling frameworks for complex data structures. Finally, the development of diagnostic tools for model adequacy and influence diagnostics would further strengthen the practical utility of the NPSD family.
In summary, the NPSD proposed in this paper represents a valuable addition to the toolkit of one-parameter lifetime distributions, offering a competitive fit for skewed nonnegative data while maintaining mathematical tractability for Bayesian inference under censoring. The simulation and real-data results support its practical relevance, and the identified limitations provide clear motivation for future extensions and refinements.

Author Contributions

Software, M.A.M.; formal analysis, A.S. and M.K.; investigation, M.A.M.; writing—original draft preparation, M.K. and H.T.; writing—review and editing, M.A.M. and A.S. All authors have read and agreed to the published version of the manuscript.

Funding

This research received no external funding.

Data Availability Statement

The original contributions presented in this study are included in the article. Further inquiries can be directed to the corresponding author.

Conflicts of Interest

The authors declare no conflicts of interest.

Appendix A

Appendix A.1. Selection Criterion for the Tuning Constant in Simulation Study ( θ   = 1 . 5 )

Among the tested parameter values, the selected tuning constant is the one minimizing the posterior risk averaged across the simulated scenarios.

Appendix A.2. Interpretation of the Hazard-Rate Behavior, and the Model-Selection Results Based on −2 log L, AIC, AICC, HQIC, and BIC

The size and form of the underlying hazard function directly affect the computed parameter values’ practical significance. A higher estimated parameter value in the context of the suggested model suggests a larger likelihood of failure at early time points by indicating a quicker degradation in survival probability. This is represented in the hazard rate’s behavior, which might represent rising, falling, or steady risk trends over time, depending on the parameter estimate. Understanding the underlying failure mechanism, whether the risk increases with time (e.g., aging effects), decreases (e.g., early failures of faulty components), or stays constant, requires interpreting this hazard trajectory. The negative twice maximized log-likelihood (−2 log L), the Akaike Information Criterion (AIC), the corrected Akaike Information Criterion (AICC), the Hannan–Quinn Information Criterion (HQIC), and the Bayesian Information Criterion (BIC) were among the information criteria taken into consideration in order to evaluate the relative adequacy of the candidate models. A better trade-off between goodness-of-fit and parsimony is shown by lower values, which penalize model complexity in various ways. Strong evidence for a model’s applicability for the given data is provided by consistent rankings across several criteria.

Appendix A.3. Illustration of Proof for Proposition 2: Computing Derivatives

f ( x ) = c ( θ ) e a ( θ ) x [ a ( θ ) a 0 ( θ ) + a 1 ( θ ) ( 1 + a ( θ ) x ) + a 2 ( θ ) ( a ( θ ) x 2 + 2 x ) ] d f ( x ) d x = c ( θ ) e a ( θ ) x [ a ( θ ) a 0 ( θ ) + a 1 ( θ ) ( 1 + a ( θ ) x ) + a 2 ( θ ) ( a ( θ ) x 2 + 2 x ) ] = c ( θ ) e a ( θ ) x [ a 1 ( θ ) a ( θ ) + 2 a 2 ( θ ) a ( θ ) x + 2 a 2 ( θ ) ] = c ( θ ) e a ( θ ) x [ a ( θ ) 2 a 0 ( θ ) + a ( θ ) a 1 ( θ ) ( 1 + a ( θ ) x ) + a ( θ ) a 2 ( θ ) ( a ( θ ) x 2 + 2 x ) + a 1 ( θ ) a ( θ ) + 2 a 2 ( θ ) a ( θ ) x + 2 a 2 ( θ ) ] = c ( θ ) e a ( θ ) x [ a ( θ ) 2 a 0 ( θ ) + a ( θ ) a 1 ( θ ) + a 1 ( θ ) a ( θ ) + 2 a 2 ( θ ) a ( θ ) 2 a 1 ( θ ) x + 2 a ( θ ) a 2 ( θ ) x + 2 a 2 ( θ ) a ( θ ) x + a ( θ ) 2 a 2 ( θ ) x 2 ] = c ( θ ) e a ( θ ) x [ a ( θ ) 2 a 2 ( θ ) x 2 + x ( a ( θ ) 2 a 1 ( θ ) + 4 a ( θ ) a 2 ( θ ) ) + a ( θ ) 2 a 0 ( θ ) + 2 a ( θ ) a 1 ( θ ) + 2 a 2 ( θ ) ) = c ( θ ) e a ( θ ) x   k ( x , θ )
d 2 f ( x ) d 2 x = c ( θ ) a ( θ ) e a ( θ ) x . k ( x , θ ) d k ( x , θ ) d x . c ( θ ) e a ( θ ) x = c ( θ ) a ( θ ) e a ( θ ) x ( a ( θ ) k ( x , θ ) + k ( x , θ ) ) = c ( θ ) a ( θ ) e a ( θ ) x ( k ( x , θ ) a ( θ ) k ( x , θ ) )

Appendix A.4. Posterior Computation in Bayesian Inference

θ ~ g ( a , b )
π ( θ ) = a b . θ b 1 τ ( b ) . exp ( a θ ) ;   θ > 0   a n d   a , b > 0
π ( θ / X ) = L ( X , θ ) π ( θ ) L ( X , θ ) π ( θ ) d θ
π ( θ / X ) = a b .   θ b 1 τ ( b ) e a θ . 2 n θ n . B m .   i = 1 n A i . e 2 θ i = 1 n x i 0 2 n θ n . B m .   i = 1 n A i . e 2 θ i = 1 n x i d θ
π ( θ / X ) = θ n + b 1 . B m . i = 1 n A i . e θ ( a + 2 i = 1 n x i ) 0 θ n + b 1 . B m . i = 1 n A i . e θ ( a + 2 i = 1 n x i ) d θ
We define: T = 1 0 θ n + b 1 . B m . i = 1 n A i . e θ ( a + 2 i = 1 n x i ) d θ .
Hence: π ( θ / X ) = T . θ n + b 1 . B m . i = 1 n A i . e θ ( a + 2 i = 1 n x i ) .

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Table 1. The three loss functions: Entropy, Generalized Quadratic, and Linex.
Table 1. The three loss functions: Entropy, Generalized Quadratic, and Linex.
Loss Function ExpressionBayes EstimatorsPosterior Risk
Entropy: L ( θ , δ ) = ( δ θ ) p p   log ( δ θ ) 1 δ ^ E = E π ( θ   p ) 1 p p [ E π ( log ( θ log ( δ ^ E ) ) ) ]
Generalized quadratic: L ( θ , δ ) = τ ( θ ) ( θ δ ) 2 δ ^ GQ = E π ( τ ( θ ) θ ) E π ( τ ( θ ) ) E π ( τ ( θ ) ( θ δ ) 2 )
Linex: L ( θ , δ ) = exp ( r ( δ θ ) ) r ( δ θ ) 1 δ ^ L = 1 r log ( E π ( exp ( r θ ) ) r ( δ ^ GQ δ ^ L )
Table 2. The MLE of the parameters with quadratic error (in brackets).
Table 2. The MLE of the parameters with quadratic error (in brackets).
N = 5000n = 10n = 50n = 200
m840160
β 0.8654 (0.0013)0.9943 (0.003)0.9985 (0.0043)
Table 3. Bayes estimators and PR (in brackets) under GQ loss function.
Table 3. Bayes estimators and PR (in brackets) under GQ loss function.
N = 5000n = 10n = 50n = 200
m840160
γ  =  2 β 0.6754 (0.0031)1.198 (0.0013)1.1267 (0.0015)
γ  =  1.5 β 0.621 (0.151)1.1209 (0.0112)1.2300 (0.0013)
γ  =  1 β 1.2908 (0.0031)1.3203 (0.0031)1.2421 (0.0085)
γ  =  0.5 β 0.8001 (0.0034)0.6124 (0.0073)0.6787 (0.0054)
γ  = 0.5 β 0.7990 (0.0054)0.6864 (0.0061)0.6147 (0.0010)
γ  = 1 β 0.8998 (0.0437)0.9709 (0.009)0.9891 (0.0001)
γ  = 1.5 β 0.6132 (0.0012)1.2308 (0.0058)1.2012 (0.0020)
γ  = 2 β 1.1247 (0.0054)1.4210 (0.0087)1.2316 (0.0003)
Table 4. Bayes estimators and PR (in brackets) under the entropy loss function.
Table 4. Bayes estimators and PR (in brackets) under the entropy loss function.
N = 5000n = 10n = 50n = 200
m840160
ρ  =  2 β 0.6252 (0.0017)0.6632 (0.0016)0.7743 (0.0004)
ρ  =  1.5 β 0.8510 (0.00915)0.7836 (0.0034)0.8936 (0.0077)
ρ    =  1 β 1.0994 (0.0089)1.028 (0.0070)1.2338 (0.0018)
ρ    =  0.5 β 1.2947 (0.00809)1.888 (0.0043)0.7333 (0.0022)
ρ    = 0.5 β 0.8912 (0.0001)0.9015 (0.0004)0.953 (0.0007)
ρ    = 1 β 0.8101 (0.0091)0.8213 (0.00665)0.8464 (0.0032)
ρ    = 1.5 β 0.7131 (0.0012)0.888 (0.0070)0.7433 (0.0016)
ρ    = 2 β 0.4768 (0.1241)0.6754 (0.1181)0.7903 (0.0033)
Table 5. Bayes estimators and PR (in brackets) under Linex loss function.
Table 5. Bayes estimators and PR (in brackets) under Linex loss function.
N = 5000n = 10n = 50n = 200
m840160
r  = 2 β 0.6185 (0.0699)0.7814 (0.0001)0.7499 (0.0001)
r  = 1.5 β 0.7037 (0.0009)0.2839 (0.009)0.7160 (0.0012)
r  = 1 β 0.7177 (0.0072)0.7633 (0.0073)0.7951 (0.0003)
r  = 0.5 β 0.8124 (0.0072)0.9438 (0.0073)0.8934 (0.0003)
r  = 0.5 β 0.8995 (0.0729)0.8998 (0.0008)0.9814 (0.0001)
r  = 1 β 0.4248 (0.0009)0.4981 (0.0038)0.5100 (0.0733)
r  = 1.5 β 0.92187 (0.0002)0.9159 (0.0005)0.9601 (0.0008)
r  = 2 β 0.6393 (0.0308)0.4176 (0.0661)0.8755 (0.319)
Table 6. Bayes estimators and PR (in brackets) under the three loss function.
Table 6. Bayes estimators and PR (in brackets) under the three loss function.
N = 5000n = 10n = 50n = 200
m840160
GQJ = 1 β 0.8998 (0.0437)0.9709 (0.009)0.9891 (0.0001)
EntropyJp = 0.5 β 0.8912 (0.0001)0.9015 (0.0004)0.953 (0.0007)
Linexj = 1.5 β 0.92187 (0.0002)0.9159 (0.0005)0.9601 (0.0008)
Table 7. Pitman comparison of the estimators.
Table 7. Pitman comparison of the estimators.
N = 5000n = 10n = 50n = 200
m840160
GQJ = 1 β 0.8420.9120.951
EntropyJp = 0.5 β 0.5510.7830.662
Linexj = 1.5 β 0.5630.6110.504
Table 8. Bayesian and likelihood estimate with posterior risk included in brackets for each of the three loss functions.
Table 8. Bayesian and likelihood estimate with posterior risk included in brackets for each of the three loss functions.
nmParameterMLEGQJ = 1EntropyJp = 0.5Linexj = 1.5
3333 θ 1.59871.6051 (0.0009)1.6311 (0.0003)1.6505 (0.0004)
3328 θ 1.64921.6351 (0.0005)1.5905 (0.0012)1.6605 (0.0005)
Table 9. Comparing the estimators of θ using Pitman.
Table 9. Comparing the estimators of θ using Pitman.
nmGQJ = 1EntropyJp = 0.5Linexj = 1.5
33330.56980.58130.6702
33280.67470.69870.6902
Table 10. IMSE of the estimators of θ.
Table 10. IMSE of the estimators of θ.
nmMLEGQJ = 1EntropyJp = 0.5Linexj = 1.5
33330.18930.15910.16130.1603
33280.19030.10930.11900.1133
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Keddali, M.; Talhi, H.; Meraou, M.A.; Slimani, A. The New Polynomial Single Parameter Distribution: Properties, Bayesian and Non-Bayesian Inference with Real-Data Applications. AppliedMath 2026, 6, 60. https://doi.org/10.3390/appliedmath6040060

AMA Style

Keddali M, Talhi H, Meraou MA, Slimani A. The New Polynomial Single Parameter Distribution: Properties, Bayesian and Non-Bayesian Inference with Real-Data Applications. AppliedMath. 2026; 6(4):60. https://doi.org/10.3390/appliedmath6040060

Chicago/Turabian Style

Keddali, Meriem, Hamida Talhi, Mohammed Amine Meraou, and Ali Slimani. 2026. "The New Polynomial Single Parameter Distribution: Properties, Bayesian and Non-Bayesian Inference with Real-Data Applications" AppliedMath 6, no. 4: 60. https://doi.org/10.3390/appliedmath6040060

APA Style

Keddali, M., Talhi, H., Meraou, M. A., & Slimani, A. (2026). The New Polynomial Single Parameter Distribution: Properties, Bayesian and Non-Bayesian Inference with Real-Data Applications. AppliedMath, 6(4), 60. https://doi.org/10.3390/appliedmath6040060

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