
Citation: Stephan A. Brinckmann, Nishant Lakhera, Chris M. Laursen, Christopher Yakacki, Carl P. Frick. Characterization of poly(para-phenylene)-MWCNT solvent-cast composites[J]. AIMS Materials Science, 2018, 5(2): 301-319. doi: 10.3934/matersci.2018.2.301
[1] | Sumati Kumari Panda, Abdon Atangana, Juan J. Nieto . Correction: New insights on novel coronavirus 2019-nCoV/SARS-CoV-2 modelling in the aspect of fractional derivatives and fixed points. Mathematical Biosciences and Engineering, 2022, 19(2): 1588-1590. doi: 10.3934/mbe.2022073 |
[2] | Tahir Khan, Roman Ullah, Gul Zaman, Jehad Alzabut . A mathematical model for the dynamics of SARS-CoV-2 virus using the Caputo-Fabrizio operator. Mathematical Biosciences and Engineering, 2021, 18(5): 6095-6116. doi: 10.3934/mbe.2021305 |
[3] | A. D. Al Agha, A. M. Elaiw . Global dynamics of SARS-CoV-2/malaria model with antibody immune response. Mathematical Biosciences and Engineering, 2022, 19(8): 8380-8410. doi: 10.3934/mbe.2022390 |
[4] | Somayeh Fouladi, Mohammad Kohandel, Brydon Eastman . A comparison and calibration of integer and fractional-order models of COVID-19 with stratified public response. Mathematical Biosciences and Engineering, 2022, 19(12): 12792-12813. doi: 10.3934/mbe.2022597 |
[5] | Rahat Zarin, Usa Wannasingha Humphries, Amir Khan, Aeshah A. Raezah . Computational modeling of fractional COVID-19 model by Haar wavelet collocation Methods with real data. Mathematical Biosciences and Engineering, 2023, 20(6): 11281-11312. doi: 10.3934/mbe.2023500 |
[6] | A. M. Elaiw, Raghad S. Alsulami, A. D. Hobiny . Global dynamics of IAV/SARS-CoV-2 coinfection model with eclipse phase and antibody immunity. Mathematical Biosciences and Engineering, 2023, 20(2): 3873-3917. doi: 10.3934/mbe.2023182 |
[7] | Biplab Dhar, Praveen Kumar Gupta, Mohammad Sajid . Solution of a dynamical memory effect COVID-19 infection system with leaky vaccination efficacy by non-singular kernel fractional derivatives. Mathematical Biosciences and Engineering, 2022, 19(5): 4341-4367. doi: 10.3934/mbe.2022201 |
[8] | Adnan Sami, Amir Ali, Ramsha Shafqat, Nuttapol Pakkaranang, Mati ur Rahmamn . Analysis of food chain mathematical model under fractal fractional Caputo derivative. Mathematical Biosciences and Engineering, 2023, 20(2): 2094-2109. doi: 10.3934/mbe.2023097 |
[9] | M. Botros, E. A. A. Ziada, I. L. EL-Kalla . Semi-analytic solutions of nonlinear multidimensional fractional differential equations. Mathematical Biosciences and Engineering, 2022, 19(12): 13306-13320. doi: 10.3934/mbe.2022623 |
[10] | Noura Laksaci, Ahmed Boudaoui, Seham Mahyoub Al-Mekhlafi, Abdon Atangana . Mathematical analysis and numerical simulation for fractal-fractional cancer model. Mathematical Biosciences and Engineering, 2023, 20(10): 18083-18103. doi: 10.3934/mbe.2023803 |
Great progress has been made in the field of statistics and probability theory for interdisciplinary research. New techniques and methods have been developed to meet the challenges of data analysis. Statistical methods are becoming increasingly important in various areas of science. The increasing complexity of scientific problems requires the development of new and suitable statistical methods for interdisciplinary research. Current challenges include, ecology: Quantifying biodiversity; the epidemiology of infectious diseases: Disease outbreak detection; financial mathematics: stock option valuation; industrial engineering: Stochastic optimization; and genomics: Personalized medicine, to name a few.
For a random lifetime T, the conditional inactivity time is defined as Tt=t−T|T≤t, and t>0. An important measure developed based on the conditional inactivity time is the α-quantile inactivity time (α-QIT), which is the α-quantile of Tt. Assuming that the distribution function of T is denoted by F, the α-QIT can be expressed by the following relationship:
qα(t)=t−F−1(−αF(t)),t>0, |
where −α=1−α and F−1(p)=inf{x:F(x)=p} is the inverse function of F. Let T be the event time referring to the instances of a species. Among all instances experienced the event at a time before t, we expect 100α% of these instances to have experienced the event after time t−qα(t). In this sense, a smaller qα(t) means larger T. The α-QIT is a competitor for the mean inactivity time (MIT) function. The MIT has been intensively studied by researchers in the field of reliability theory and survival analysis, e.g., refer to Finkelstein [1] and Kayid and Izadkhah [2]. However, when the moments of the underlying model are infinite or heavily skewed to right, α-QIT is preferred over MIT (see Schmittlein and Morrison [3] for a detailed justification of quantile-based than moment-based measures). The α-QIT concept was formally defined and studied by Unnikrishnan and Vineshkumar [4]. Shafaei [5] showd that how the underlying model can be characterized by α-QIT function. Shafaei and Izadkhah [6] stated some properties of a parallel system in terms of the α-QIT measure. For a sample T1, T2, ..., Tn of iid lifetimes, the α-QIT can be estimated by
qα,n(t)=t−F−1n(−αFn(t)),t≥T(1), |
where Fn(t) is the empirical distribution function, i.e.,
Fn(t)=1n∑ni=1I(Ti≤t), |
and
F−1n(p)=inf{x:Fn(x)≥p}={0p=0,T(1)0<p≤1n,T(2)1n<p≤2n,…T(n)1−1n<p≤1. |
Then, qα,n can be written as in the following.
qα,n(t)={t0≤t<t1,t−T(1)t1≤t<t2,t−T(2)t2≤t<t3,…t−T(n−1)tk−1≤t<tk,t−T(n)t≥tk, | (1) |
where
ti=inf{y:−αFn(y)>i−1n}=inf{y:F−1n(−αFn(y))=T(i)}. |
Note that F−1n(−αFn(ti))=T(i), for every i=1,2,…,k for some k≤n t1=T(1) and ti≥T(i) for i=2…...,k. The expression (1) shows that qα,n(t) consists of line segments with slope 1 on intervals (ti,ti+1), i…,2,...,k−1 and falls at each point ti by T(i)−T(i−1), i=1,2,...,k where T(0)=0. Figure 1 shows a schematic plot of qα,n(t).
For the univariate case, Mahdy [7] proposed the estimator (2) for the α-QIT function and investigated its asymptotic properties. Balmert and Jeong [8] created a nonparametric inference of the median inactivity time function for right-censored data. Balmert et al. [9] applied a log-linear quantile regression model to the inactivity time for right-censored data. Kayid [10] applied the Kaplan-Meiere survival estimator to the α-QIT function for estimation and inference.
We can have two or more dependent events. For example, if successive events of the same person/instance are tracked, the event times depend on each other. Another example is that researchers are interested in determining the effect of a treatment on specific event times related to the eyes, ears, hands or legs. One organ was randomly selected for treatment and the other was a control organ. The events associated with these organs depend on their progression. In such cases, we need to extend the measures in question to bivariate or multivariate settings. In the following section, I refer to the authors who have implemented this idea. Basu [11] and Johnson and Kotz [12] examined the multivariate hazard rate function as a gradient vector. The mean residual lifetime was extended by Nair and Nair [13] to obtain a vector of dependent lifetimes. Shaked and Shanthikumar [14] introduced the dynamic multivariate MRL concept. Kayid [15] developed the multivariate MIT concept. Navarro [16] characterized the basic model by the bivariate hazard rate function. The concept of the α-quantile residual lifetime (α-QRL) was extended to the multivariate context by Shafaei and Kayid [17]. Shafaei et al. [18] discussed the multivariate α-QRL concept in a dynamic way. Buono et al. [19] applied multivariate RHR for discussing reliability attributes of systems. Kayid [20] extended the α-QIT concept to bivariate context and discussed its estimation.
Let F be the distribution function of a random pair T=(T1,T2). Then, the α-QIT vector at point t=(t1,t2) is defined to be (qα,1(t),qα,2(t)). The first element of this vector is
qα,1(t)=sup{x:P(t1−T1>x|T≤t)=−α}=sup{x:F(t1−x,t2)=−αF(t)}=inf{t1−z:F(z,t2)=−αF(t)}=t1−F−11(−αF(t);t2), |
where −α=1−α and
F−11(p;t2)=inf{z:F(z,t2)=p}, |
is the partial inverse of F in terms of the T1. The second element of the α-QIT vector is defined similarly.
qα,2(t)=t2−F−12(−αF(t);t1), |
where F−12(p;t1)=inf{z:F(t1,z)=p} is the partial inverse of F in terms of the second element. The reversed hazard rate vector of T is (r1(t),r2(t)) and
ri(t)=∂∂tilogF(t),i=1,2. |
The RHR satisfies the following relation.
{∂∂t1F(t1,t2)=r1(t1,t2)F(t1,t2),∂∂t2F(t1,t2)=r2(t1,t2)F(t1,t2). |
Kayid [20] showed that if ri(t) is decreasing (increasing) in ti, then qα,i(t) is increasing (decreasing) in ti. It is a surprising fact that for most of the standard bivariate models, ri(t) is decreasing in ti (Finkelstein [1]). For example, bivariate Gumbel, Pareto, normal, and gamma models have decreasing reversed hazard rate functions. This implies that qα,i(t) is increasing in ti. For some examples of such models, refer to Kayid [20]. This motivates me to introduce a new estimator of qα,1(t) and qα,2(t) under the assumption that they are increasing with respect to t1 and t2, respectively. It is expected that applying this knowledge, I have a more accurate estimator than the usual estimator defined by Kayid [20]. Such monotone estimators are defined and studied by Kochar et al. [21], Franco Pereira and Una-Alvarez [22], and Shafaei and Franco Pereira [23].
The rest of this paper is structured as follows. In Section 2, the promised increasing estimator of the bivariate α-QIT function is proposed and its asymptotic properties are discussed. Then, the performance of the new estimator is compared with that of the usual estimator in a simulation study. In Section 4, the proposed estimator is applied to investigate the effect of laser treatment on the time to blindness. In Section 5, I summarize the results.
Let …,...,Tn be an iid random sample from bivariate distribution F. The empirical distribution function is defined by
Fn(t1,t2)=n−1∑ni=1I(T1i≤t1,T2i≤t2), |
and the partial inverse of Fn, with respect to the first and second elements, are as in the following respectively:
F−11,n(p;t2)=inf{x:Fn(x,t2)≥p}, |
and
F−12,n(p;t1)=inf{x:Fn(t1,x)≥p}. |
Kayid [20] proposed the following estimator of the bivariate α-QIT vector.
qα,n(t)=(qα,1,n(t),qα,2,n(t)), |
where
{qα,1,n(t)=t1−F−11,n(−αFn(t);t2),qα,2,n(t)=t2−F−12,n(−αFn(t);t1), |
with the knowledge of increasing bivariate α-IQT, we define the natural estimator
iqα,n(t)=(iqα,1,n(t),iqα,2,n(t)), |
where
{iqα,1,n(t)=supy≤t1qα,1,n(y,t2),iqα,2,n(t)=supy≤t2qα,2,n(t1,y), |
Let t2>0 be fixed and define T1[t2]=T1|T2≤t2, then the distribution function of T1[t2] is
F∗1(x;t2)=P(T1[t2]≤x)=F(x,t2)F2(t2), |
where F2(t2)=P(T2≤t2). Denote α-QIT of T1[t2] by q∗α,1(t1;t2), then it can be shown that
q∗α,1(t1;t2)=qα,1(t1,t2). | (2) |
Similarly, for every fixed t1>0, we define T2[t1]=T2|T1≤t1 following distribution F∗2(.;t1). Let q∗α,2(t2;t1) be the α-QIT of T2[t1], then we can investigate that
q∗α,2(t2;t1)=qα,2(t1,t2). | (3) |
Given a bivariate iid random sample (T1i,T2i), i=1,2,…,n from distribution F, and for every fixed t2, consider the following univariate random sample which follows from F∗1(.;t2).
χ(1,t2)={T1ij: whenT2ij≤t2,j=1…...,k1(t2)}. |
I can apply this sample to estimate q∗α,1(t1;t2), as in the following.
q∗α,1,n(t1;t2)=t1−F∗−11,n(−αF∗1,n(t1;t2)), |
where
F∗1,n(t1;t2)=#(T1ij≤t1)k1(t2), |
and
F∗−11,n(p)=inf{x:F∗1,n(x;t2)≥p}. |
Applying the knowledge of increasing q∗α,1(t1;t2) in terms of t1, it is natural to use the following estimator.
iq∗α,1,n(t1;t2)=supy≤t1 q∗α,1,n(y;t2). |
Again, for a bivariate iid random sample (T1i,T2i), i…,2,...,n from distribution F, and for every fixed t1, consider the following sample.
χ(2,t1)={T2ij: whenT1ij≤t1⋯=1,2,...,k2(t1)}, |
which follows from F∗2(.;t1). Then, the estimator of q∗α,2(t2;t1) is defined by
q∗α,2,n(t2;t1)=t2−F∗−12,n(−αF∗2,n(t2;t1)), |
where
F∗2,n(t2;t1)=#(T2ij≤t2)k2(t1), |
and
F∗−12,n(p)=inf{x:F∗2,n(x;t1)≥p}. |
In an increasing context,
iq∗α,2,n(t2;t1)=supy≤t2 q∗α,2,n(y;t1). |
It is clear that
{iqα,1,n(t)=iq∗α,1,n(t1;t2),iqα,2,n(t)=iq∗α,2,n(t2;t1). | (4) |
Theorem 1. Let us assume that the following two conditions are fulfilled.
(C1). F(t1,t2) be twice differentiable with respect each element.
(C2). ∂∂t1F(t) and ∂∂t2F(t) are bounded from zero on the intervals (0,F−11(−α;t2)) and (0,F−12(−α;t1)), respectively, for every t1>0 and t2>0.
Then, (iqα,1,n(t),iqα,2,n(t)) is consistent for (iqα,1(t),iqα,2(t)).
Proof. By Theorem 7 from Kayid [24], we have
|iq∗α,1,n(t1;t2)−iq∗α,1(t1;t2)|→0, almost every where, |
and
|iq∗α,2,n(t2;t1)−iq∗α,2(t2;t1)|→0, almost every where. |
Thus, the result follows from (2)–(4).
To state the next theorem, I need two following conditions.
(C3) ∂∂t1qα,1(t) and ∂∂t2qα,2(t) exist and there are c1>0 and c2>0 such that ∂∂t1qα,1(t)>c1 and ∂∂t2qα,2(t)>c2 for all 0<t1<b1 and 0<t2<b2 for some positive b1 and b2.
(C4) ∂2∂t1∂t1qα,1(t) and ∂2∂t2∂t2qα,2(t) exist and
sup0<t1<b1|∂2∂t1∂t1qα,1(t)|≤c3<∞andsup0<t2<b2|∂2∂t2∂t2qα,2(t)|≤c4<∞. |
Theorem 2. Assume that C1–C4 are satisfied. Then, we have
√n|(iqα,1,n(t),iqα,2,n(t))−(qα,1,n(t),qα,2,n(t))|→0, in probability. |
Proof. By Theorem 5 from Kayid [21], we have
sup0<t<b1|iq∗α,1,n(t1;t2)−q∗α,1,n(t1;t2)|→0, inprobability, |
and
sup0<t<b2|iq∗α,2,n(t2;t1)−q∗α,2,n(t2;t1)|→0, inprobability. |
Thus, the result follows from relations (2)–(4) and the concept of convergence in probability in bivariate setting.
The following lemma, which is the result of the well-known Slutsky theorem, is used in the proof of the next theorem (see Van der Vaart [25] for Slutsky's theorem and related results).
Lemma 1. If √n(Xn−Yn)→0 in probability and √nXn converges, in distribution, to a random variable X with distribution F, then √nYn converges, in distribution, to a random variable Y with the same distribution F.
Theorem 3. Under the conditions C1–C4, we have
√n|(iqα,1,n(t),iqα,2,n(t))−(qα,1(t),qα,2(t))|→N(0,CΣC), in distribution, |
where
C=−[∂∂pF−11(p;t2)|p=−αF(t)00∂∂pF−12(p;t1)|p=−αF(t)], |
and elements of Σ are
σ11=σ22=α−αF(t), |
and
σ12=σ21=F(F−11(−αF(t);t2),F−12(−αF(t);t1))−−α2F(t). |
Proof. Theorem 7 of Kayid [20] states that under some mild conditions:
√n|(qα,1,n(t),qα,2,n(t))−(qα,1(t),qα,2(t))|→N(0,CΣC), in distribution, |
where C and Σ are defined in this theorem. Thus, applying Lemma 1, the result follows immediately.
In the real world, lifetime random pairs T1,T2,...,Tn may be censored by a random censorship Ci, in the sense that the observations are T1i=T1i∧Ci, T2i=T2i∧Ci, δ1i=I(T1i>Ci) and δ2i=I(T2i>Ci). Note that a∧b=min{a,b}. Let censorship random variable Ci be independent from desired lifetimes and follows from distribution G and the reliability function −G=1−G, i.e., −G(t)=P(Ci>t). Also, let R(t1,t2)=P( T1i>t1, T2i>t2) and R(t1,t2)=P(T1i>t1,T2i>t2). Then, we have
R(t1,t2)= R(t1,t2)−G(t1∨t2), |
where t1∨t2=max{t1,t2}. So, we can estimate the reliability function R by
Rn(t1,t2)=1n∑ni=1I( T1i>t1, T2i>t2)−Gn(t1∨t2). |
Under this censoring scheme, Lin and Ying [26] showed that Rn(t1,t2) is strongly consistent and weakly converges to a Gaussian process. Thus, when we have such censored data, the empirical distribution function could be replaced by the following estimate:
Fn(t1,t2)=1−Rn(t1,0)−Rn(0,t2)+Rn(t1,t2). |
To investigate the performance of the proposed (increasing) estimator and comparing it with the usual estimator, a simulation study is conducted. The bivariate Gumbel and Pareto distributions with respectively the following reliability functions are selected for the baseline models:
−F(t1,t2)=exp{−t1−t2−βt1t2},β>0,t1≥0,t2≥0, |
and
−F(t1,t2)=(t1+t2−1)−c,c>0,t1≥1,t2≥1. |
Both models are important from practical and theoretical points of view. The Gumbel distribution was introduced by Gumbel [27], and the Pareto model was used by Jupp and Mardia [28] to analyze income data for consecutive years. Some proper values for β and c were selected. In each simulation run, r=1000 replicates of bivariate samples of size n were generated, where n was set to 25, 50 or 100. For each sample, q0.5,1,n() and its increasing version, iq0.5,1,n(), are calculated at four appropriate time points t1, t2, t3 and t4 according to the following rules: Let F1 be the marginal distribution of the first element and ti=(t1i,t2i). The equations F1(t11)=0.25, F1(t12)=0.40, F1(t13)=0.50 and F1(t14)=0.75 are solved to find t11 to t14 and given them, the equations F(t11,t21)=0.2, F(t12,t22)=0.3, F(t13,t23)=0.4, and F(t14,t24)=0.6 are solved for t21 to t24. After calculating the objective functions for r replicates, the bias (B) and mean squared error (MSE) were calculated and are shown in Tables 1 and 2 for the Gumbel and Pareto models, respectively. All simulations and calculations were performed in R (statistical programming language). The results show small values for B and MSE for both the conventional estimator and the proposed increasing estimator. As expected, the MSE increases with F(t) (see Theorem 3). The MSE values for the increasing estimator are smaller in all cases, indicating that the increasing estimator performs better than the conventional estimator. See Figures 2 and 3 for a graphicall representaion of the ratio of MSE values related to the ususal to the increasing estimator.
β | ||||||||
0.8 | 1 | 1.4 | ||||||
Estimator | n | point | B | MSE | B | MSE | B | MSE |
Usual | 25 | t1 | 0.0133 | 0.0036 | 0.0120 | 0.0037 | 0.0115 | 0.0035 |
t2 | 0.0146 | 0.0075 | 0.0096 | 0.0075 | 0.0144 | 0.0074 | ||
t3 | 0.0113 | 0.0105 | 0.0086 | 0.0099 | 0.0157 | 0.0100 | ||
t4 | 0.0118 | 0.0242 | 0.0150 | 0.0212 | 0.0203 | 0.0232 | ||
50 | t1 | 0.0071 | 0.0019 | 0.0068 | 0.0019 | 0.0062 | 0.0018 | |
t2 | 0.0093 | 0.0040 | 0.0074 | 0.0039 | 0.0071 | 0.0039 | ||
t3 | 0.0055 | 0.0053 | 0.0069 | 0.0055 | 0.0050 | 0.0054 | ||
t4 | 0.0070 | 0.0110 | 0.0050 | 0.0115 | 0.0059 | 0.0118 | ||
100 | t1 | 0.0057 | 0.0010 | 0.0049 | 0.0009 | 0.0043 | 0.0010 | |
t2 | 0.0033 | 0.0021 | 0.0035 | 0.0022 | 0.0035 | 0.0020 | ||
t3 | 0.0017 | 0.0028 | 0.0058 | 0.0027 | 0.0022 | 0.0028 | ||
t4 | -0.0010 | 0.0064 | 0.0027 | 0.0059 | 0.0009 | 0.0058 | ||
Increasing | 25 | t1 | 0.0395 | 0.0032 | 0.0388 | 0.0031 | 0.0386 | 0.0030 |
t2 | 0.0480 | 0.0064 | 0.0466 | 0.0065 | 0.0503 | 0.0065 | ||
t3 | 0.0440 | 0.0082 | 0.0435 | 0.0079 | 0.0473 | 0.0086 | ||
t4 | 0.0370 | 0.0204 | 0.0392 | 0.0182 | 0.0455 | 0.0196 | ||
50 | t1 | 0.0224 | 0.0016 | 0.0232 | 0.0016 | 0.0238 | 0.0017 | |
t2 | 0.0286 | 0.0035 | 0.0282 | 0.0034 | 0.0268 | 0.0033 | ||
t3 | 0.0244 | 0.0043 | 0.0252 | 0.0047 | 0.0238 | 0.0045 | ||
t4 | 0.0192 | 0.0105 | 0.0175 | 0.0108 | 0.0163 | 0.0110 | ||
100 | t1 | 0.0145 | 0.0009 | 0.0141 | 0.0008 | 0.0139 | 0.0009 | |
t2 | 0.0140 | 0.0019 | 0.0141 | 0.0019 | 0.0148 | 0.0019 | ||
t3 | 0.0103 | 0.0026 | 0.0137 | 0.0026 | 0.0115 | 0.0025 | ||
t4 | 0.0063 | 0.0060 | 0.0058 | 0.0057 | 0.0082 | 0.0055 |
c | ||||||||
0.5 | 0.7 | 1.1 | ||||||
Estimator | n | point | B | MSE | B | MSE | B | MSE |
Usual | 25 | t1 | -0.0040 | 0.1866 | 0.0149 | 0.0686 | 0.0018 | 0.0242 |
t2 | 0.0030 | 0.2704 | -0.0067 | 0.1025 | -0.0042 | 0.0346 | ||
t3 | -0.0412 | 0.4076 | -0.0285 | 0.1508 | -0.0082 | 0.0469 | ||
t4 | -0.0591 | 0.5858 | -0.0349 | 0.2085 | -0.0156 | 0.0620 | ||
50 | t1 | 0.0017 | 0.0903 | -0.0100 | 0.0407 | 0.0040 | 0.0113 | |
t2 | -0.0152 | 0.1273 | -0.0178 | 0.0554 | 0.0005 | 0.0159 | ||
t3 | -0.0312 | 0.1913 | -0.0296 | 0.0816 | -0.0025 | 0.0221 | ||
t4 | -0.0534 | 0.3003 | -0.0345 | 0.1103 | -0.0004 | 0.0273 | ||
100 | t1 | -0.0086 | 0.0461 | -0.0017 | 0.0172 | 0.0008 | 0.0057 | |
t2 | -0.0089 | 0.0577 | -0.0030 | 0.0253 | -0.0010 | 0.0080 | ||
t3 | -0.0137 | 0.0823 | -0.0057 | 0.0343 | -0.0037 | 0.0107 | ||
t4 | -0.0222 | 0.1243 | -0.0086 | 0.0495 | -0.0035 | 0.0141 | ||
Increasing | 25 | t1 | 0.0004 | 0.1832 | 0.0271 | 0.0603 | 0.1125 | 0.0197 |
t2 | 0.0032 | 0.2702 | -0.0018 | 0.1008 | 0.0049 | 0.0304 | ||
t3 | -0.0411 | 0.4076 | -0.0285 | 0.1508 | -0.0043 | 0.0438 | ||
t4 | -0.0591 | 0.5858 | -0.0349 | 0.2085 | -0.0155 | 0.0620 | ||
50 | t1 | 0.0057 | 0.0897 | 0.0009 | 0.0373 | 0.0830 | 0.0087 | |
t2 | -0.0135 | 0.1261 | -0.0142 | 0.0539 | 0.0048 | 0.0151 | ||
t3 | -0.0307 | 0.1906 | -0.0286 | 0.0802 | -0.0012 | 0.0218 | ||
t4 | -0.0534 | 0.3002 | -0.0343 | 0.1103 | -0.0004 | 0.0273 | ||
100 | t1 | -0.0046 | 0.0447 | 0.0014 | 0.0166 | 0.0631 | 0.0046 | |
t2 | -0.0072 | 0.0570 | -0.0017 | 0.0252 | 0.0008 | 0.0077 | ||
t3 | -0.0137 | 0.0823 | -0.0042 | 0.0339 | -0.0029 | 0.0105 | ||
t4 | -0.0222 | 0.1243 | -0.0085 | 0.0495 | -0.0033 | 0.0140 |
In a study that began in 1971, researchers were interested in the effect of laser photocoagulation on delaying blindness in patients with DR. Patients with visual acuity ≥ 20/100 in both eyes were selected for the study. One eye of each patient was randomly selected for laser photocoagulation (treatment) and the other eye was observed without treatment (control). The time from the start of treatment to blindness is given in months. Blindness means that visual acuity fell below 5/200 on two consecutive visits. The data for this study is available in the "diabetic" dataset in the "survival" package in R. Table 3 shows part of the dataset relating to adolescents (under 20 years of age). For patient i, T1i and T2iindicate the observed time to blindness in the control and treated eyes, respectively.
Patient (i) | 1 | 2 | 3 | 4 | 5 | 6 | 7 | 8 | 9 |
T1i | 6.9 | 1.63 | 13.83 | 35.53 | 14.8 | 6.2 | 22 | 1.7 | 43.03 |
T2i | 20.17 | 10.27 | 5.67 | 5.90 | 33.9 | 1.73 | 30.2 | 1.7 | 1.77 |
Patient (i) | 10 | 11 | 12 | 13 | 14 | 15 | 16 | 17 | 18 |
T1i | 6.53 | 42.17 | 48.43 | 9.6 | 7.6 | 1.8 | 9.9 | 13.77 | 0.83 |
T2i | 18.7 | 42.17 | 14.3 | 13.33 | 14.27 | 34.57 | 21.57 | 13.77 | 10.33 |
Patient (i) | 19 | 20 | 21 | 22 | 23 | 24 | |||
T1i | 1.97 | 11.3 | 30.4 | 19 | 5.43 | 46.63 | |||
T2i | 11.07 | 2.1 | 13.97 | 13.80 | 13.57 | 42.43 |
Figures 4 and 5 draw the bivariate median inactivity time functions and their increasing versions, iqn,0.5,1(t) and iqn,0.5,2(t), respectively.
The comparison of the proposed increasing median inactivity time functions iqn,0.5,1(t) and iqn,0.5,2(t) at different points is informative in investigating the treatment effect. To provide a simple and powerful statistics, we can consider the points on the identity line and use the following statistics
dn(t)=iqn,0.5,1(t,t)−iqn,0.5,2(t,t),t≥0. | (5) |
If I assume that the treatment dose not effect the time length to blindness, dn(t) should be positive or negitive values near zero, reflecting some random errors. However, if the treatment causes longer time to blindness, I expect relatively larger values for iqn,0.5,1(t,t) than iqn,0.5,2(t,t), i.e., positive values for dn(t). Figure 6 plots dn(t) in all points of the observed T1 or T2. The plot shows positive values that increase with t and indicates that the treatment causes longer time to blindness. The effect of treatment also increases with time. The bivariate median inactivity functions are on the right side of Figure 6 to provide a better comparison of these functions.
Assuming an increasing α-QIT function, I define a new estimator for this function. It is proven that the proposed estimator is consistent. It is asymptotically close to the usual estimator in the sense that the difference to the usual estimator converges to zero with high probability. It is also shown that the proposed estimator converges weakly to a Gaussian process when normalized. Interestingly, none of the asymptotic results assume that the true α-QIT function increases, which increases the applicability of the estimator in general. The simulation results show that the MSE for the proposed increasing estimator is smaller than that of the conventional estimator. When using the proposed estimator, it was found that the laser treatment causes a delay in glare.
The author thanks the two anonymous reviewers for their careful reading of our manuscript and their many insightful comments and suggestions.
This work was supported by Researchers Supporting Project number (RSP2024R392), King Saud University, Riyadh, Saudi Arabia.
The data for this study is available in the "diabetic" dataset in the "survival" package in R.
The author declares that there is no conflict of interest.
[1] |
Nunes JP, Silva JF, Velosa JC, et al. (2009) New thermoplastic matrix composites for demanding applications. Plast Rubber Compos 38: 167–172. doi: 10.1179/174328909X387946
![]() |
[2] | Dean D, Husband M, Trimmer M (1998) Time–temperature-dependent behavior of a substituted poly(paraphenylene): Tensile, creep, and dynamic mechanical properties in the glassy state. J Polym Sci Pol Phys 36: 2971–2979. |
[3] |
Friedrich K, Burkhart T, Almajid AA, et al. (2010) Poly-Para-Phenylene-Copolymer (PPP): A High-Strength Polymer with Interesting Mechanical and Tribological Properties. Int J Polym Mater Po 59: 680–692. doi: 10.1080/00914037.2010.483211
![]() |
[4] |
Frick CP, DiRienzo AL, Hoyt AJ, et al. (2014) High-strength poly(para-phenylene) as an orthopedic biomaterial. J Biomed Mater Res A 102: 3122–3129. doi: 10.1002/jbm.a.34982
![]() |
[5] |
Hoyt AJ, Yakacki CM, Fertig III RS, et al. (2015) Monotonic and cyclic loading behavior of porous scaffolds made from poly(para-phenylene) for orthopedic applications. J Mech Behav Biomed 41: 136–148. doi: 10.1016/j.jmbbm.2014.10.004
![]() |
[6] |
DiRienzo AL, Yakacki CM, Frensemeier M, et al. (2014) Porous poly(para-phenylene) scaffolds for load-bearing orthopedic applications. J Mech Behav Biomed 30: 347–357. doi: 10.1016/j.jmbbm.2013.10.012
![]() |
[7] | Collins DA, Yakacki CM, Lightbody D, et al. (2016) Shape-memory behavior of high-strength amorphous thermoplastic poly(para-phenylene). J Appl Polym Sci 133: 1–10. |
[8] |
Almajid A, Friedrich K, Noll A, et al. (2013) Poly-para-phenylene-copolymers (PPP) for extrusion and injection moulding Part 1——molecular and rheological differences. Plast Rubber Compos 42: 123–128. doi: 10.1179/1743289812Y.0000000045
![]() |
[9] | Pei X, Friedrich K (2012) Sliding wear properties of PEEK, PBI and PPP. Wear 274–275: 452–455. |
[10] |
Ma Y, Cong P, Chen H, et al. (2015) Mechanical and Tribological Properties of Self-Reinforced Polyphenylene Sulfide Composites. J Macromol Sci B 54: 1169–1182. doi: 10.1080/00222348.2015.1061845
![]() |
[11] |
Ribeiro B, Pipes RB, Costa ML, et al. (2017) Electrical and rheological percolation behavior of multiwalled carbon nanotube-reinforced poly(phenylene sulfide) composites. J Compos Mater 51: 199–208. doi: 10.1177/0021998316644848
![]() |
[12] |
Mahat KB, Alarifi I, Alharbi A, et al. (2016) Effects of UV Light on Mechanical Properties of Carbon Fiber Reinforced PPS Thermoplastic Composites. Macromol Symp 365: 157–168. doi: 10.1002/masy.201650015
![]() |
[13] |
Kuo MC, Huang JC, Chen M, et al. (2003) Fabrication of High Performance Magnesium/Carbon-Fiber/PEEK Laminated Composites. Mater Trans 44: 1613–1619. doi: 10.2320/matertrans.44.1613
![]() |
[14] |
Martin AC, Lakhera N, DiRienzo AL, et al. (2013) Amorphous-to-crystalline transition of Polyetheretherketone-carbon nanotube composites via resistive heating. Compos Sci Technol 89: 110–119. doi: 10.1016/j.compscitech.2013.09.012
![]() |
[15] |
Garcia-Gonzalez D, Rusinek A, Jankowiak T, et al. (2015) Mechanical impact behavior of polyether-ether-ketone (PEEK). Compos Struct 124: 88–99. doi: 10.1016/j.compstruct.2014.12.061
![]() |
[16] |
Bishop MT, Karasz FE, Russo PS, et al. (1985) Solubility and Properties of a Poly(aryl ether ketone) in Strong Acids. Macromolecules 18: 86–93. doi: 10.1021/ma00143a014
![]() |
[17] | Shukla D, Negi YS, Kumar V (2013) Modification of Poly(ether ether ketone) Polymer for Fuel Cell Application. J Appl Chem 2013. |
[18] |
Wang X, Li Z, Zhang M, et al. (2017) Preparation of a polyphenylene sulfide membrane from a ternary polymer/solvent/non-solvent system by thermally induced phase separation. RSC Adv 7: 10503–10516. doi: 10.1039/C6RA28762J
![]() |
[19] |
Natori I, Natori S, Sekikawa H, et al. (2008) Synthesis of soluble poly(para-phenylene) with a long polymer chain: Characteristics of regioregular poly(1,4-phenylene). J Polym Sci Pol Chem 46: 5223–5231. doi: 10.1002/pola.22851
![]() |
[20] |
Marvel CS, Hartzell GE (1959) Preparation and Aromatization of Poly-1,3-cyclohexadiene1. J Am Chem Soc 81: 448–452. doi: 10.1021/ja01511a047
![]() |
[21] | Cochet M, Maser WK, Benito AM, et al. (2001) Synthesis of a new polyaniline/nanotube composite: "in-situ" polymerisation and charge transfer through site-selective interaction. Chem Commun 1450–1451. |
[22] |
Olifirov LK, Kaloshkin SD, Zhang D (2017) Study of thermal conductivity and stress-strain compression behavior of epoxy composites highly filled with Al and Al/f-MWCNT obtained by high-energy ball milling. Compos Part A-Appl S 101: 344–352. doi: 10.1016/j.compositesa.2017.06.027
![]() |
[23] |
Overney G, Zhong W, Tomanek D (1993) Structural rigidity and low frequency vibrational modes of long carbon tubules. Z Phys D-Atoms, Molecules and Clusters 27: 93–96. doi: 10.1007/BF01436769
![]() |
[24] |
Spitalsky Z, Tasis D, Papagelis K, et al. (2010) Carbon nanotube-polymer composites: Chemistry, processing, mechanical and electrical properties. Prog Polym Sci 35: 357–401. doi: 10.1016/j.progpolymsci.2009.09.003
![]() |
[25] | Khare R, Bose S (2005) Carbon Nanotube Based Composites——A Review. J Min Mater Charact Eng 4: 31–46. |
[26] |
Schadler LS, Giannaris SC, Ajayan PM (1998) Load transfer in carbon nanotube epoxy composites. Appl Phys Lett 73: 3842–3844. doi: 10.1063/1.122911
![]() |
[27] |
Frankland SJV, Caglar A, Brenner DW, et al. (2002) Molecular simulation of the influence of chemical cross-links on the shear strength of carbon nanotube-polymer interfaces. J Phys Chem B 106: 3046–3048. doi: 10.1021/jp015591+
![]() |
[28] |
Tsuda T, Ogasawara T, Deng F, et al. (2011) Direct measurements of interfacial shear strength of multi-walled carbon nanotube/PEEK composite using a nano-pullout method. Compos Sci Technol 71: 1295–1300. doi: 10.1016/j.compscitech.2011.04.014
![]() |
[29] |
Calvert P (1999) Nanotube Composites: A recipe for strength. Nature 399: 210–211. doi: 10.1038/20326
![]() |
[30] |
Tasis D, Tagmatarchis N, Bianco A, et al. (2006) Chemistry of carbon nanotubes. Chem Rev 106: 1105–1136. doi: 10.1021/cr050569o
![]() |
[31] |
Ma PC, Siddiqui NA, Marom G, et al. (2010) Dispersion and functionalization of carbon nanotubes for polymer-based nanocomposites: A review. Compos Part A-Appl S 41: 1345–1367. doi: 10.1016/j.compositesa.2010.07.003
![]() |
[32] |
Grady BP (2010) Recent developments concerning the dispersion of carbon nanotubes in polymers. Macromol Rapid Comm 31: 247–257. doi: 10.1002/marc.200900514
![]() |
[33] |
Jyoti J, Babal AS, Sharma S, et al. (2018) Significant improvement in static and dynamic mechanical properties of graphene oxide-carbon nanotube acrylonitrile butadiene styrene hybrid composites. J Mater Sci 53: 2520–2536. doi: 10.1007/s10853-017-1592-6
![]() |
[34] |
Song YS, Youn JR (2005) Influence of dispersion states of carbon nanotubes on physical properties of epoxy nanocomposites. Carbon 43: 1378–1385. doi: 10.1016/j.carbon.2005.01.007
![]() |
[35] |
Shi DL, Feng XQ, Huang YY, et al. (2004) The effect of nanotube waviness and agglomeration on the elastic property of carbon nanotube-reinforced composites. J Eng Mater-T ASME 126: 250–257. doi: 10.1115/1.1751182
![]() |
[36] |
Fiedler B, Gojny FH, Wichmann MHG, et al. (2006) Fundamental aspects of nano-reinforced composites. Compos Sci Technol 66: 3115–3125. doi: 10.1016/j.compscitech.2005.01.014
![]() |
[37] |
Strano MS, Dyke CA, Usrey ML, et al. (2003) Electronic structure control of single-walled carbon nanotube functionalization. Science 301: 1519–1522. doi: 10.1126/science.1087691
![]() |
[38] |
Banerjee S, Kahn MGC, Wong SS (2003) Rational chemical strategies for carbon nanotube functionalization. Chem-Eur J 9: 1898–1908. doi: 10.1002/chem.200204618
![]() |
[39] |
Yang K, Gu M, Guo Y, et al. (2009) Effects of carbon nanotube functionalization on the mechanical and thermal properties of epoxy composites. Carbon 47: 1723–1737. doi: 10.1016/j.carbon.2009.02.029
![]() |
[40] |
Sahoo NG, Rana S, Cho JW, et al. (2010) Polymer nanocomposites based on functionalized carbon nanotubes. Prog Polym Sci 35: 837–867. doi: 10.1016/j.progpolymsci.2010.03.002
![]() |
[41] |
Silva JF, Nunes JP, Velosa JC, et al. (2010) Thermoplastic matrix towpreg production. Adv Polym Tech 29: 80–85. doi: 10.1002/adv.20174
![]() |
[42] | Vuorinen A (2010) Rigid Rod Polymers Fillers in Acrylic Denture and Dental Adhesive Resin Systems. |
[43] |
Kwok N, Hahn HT (2007) Resistance heating for self-healing composites. J Compos Mater 41: 1635–1654. doi: 10.1177/0021998306069876
![]() |
[44] |
Delzeit L, Nguyen CV, Chen B, et al. (2002) Multiwalled carbon nanotubes by chemical vapor deposition using multilayered metal catalysts. J Phys Chem B 106: 5629–5635. doi: 10.1021/jp0203898
![]() |
[45] | Caneba G (2010) Product Materials, In: Free-radical retrograde-precipitation polymerization (FRRPP): novel concept, processes, materials, and energy aspects, Springer Science & Business Media, 199–252. |
[46] | Xu Z, Wan L, Huang X (2009) Surface Modification by Graft Polymerization, In: Surface Engineering of Polymer Membranes. Advanced Topics in Science and Technology in China, Springer, Berlin, Heidelberg, 80–149. |
[47] |
Kubo T, Im J, Wang X, et al. (2014) Solvent induced nanostructure formation in polymer thin films: The impact of oxidation and solvent. Colloid Surface A 444: 217–225. doi: 10.1016/j.colsurfa.2013.12.052
![]() |
[48] |
Ajayan PM, Stephan O, Colliex C, et al. (1994) Aligned carbon nanotube arrays formed by cutting a polymer resin-nanotube composite. Science 265: 1212–1214. doi: 10.1126/science.265.5176.1212
![]() |
[49] |
Haggenmueller R, Gommans HH, Rinzler AG, et al. (2000) Aligned single-wall carbon nanotubes in composites by melt processing methods. Chem Phys Lett 330: 219–225. doi: 10.1016/S0009-2614(00)01013-7
![]() |
[50] |
Puglia D, Valentini L, Kenny JM (2003) Analysis of the cure reaction of carbon nanotubes/epoxy resin composites through thermal analysis and Raman spectroscopy. J Appl Polym Sci 88: 452–458. doi: 10.1002/app.11745
![]() |
[51] |
Park C, Ounaies Z, Watson KA, et al. (2002) Dispersion of single wall carbon nanotubes by in situ polymerization under sonication. Chem Phys Lett 364: 303–308. doi: 10.1016/S0009-2614(02)01326-X
![]() |
[52] |
Qian D, Dickey EC, Andrews R, et al. (2000) Load transfer and deformation mechanisms in carbon nanotube-polystyrene composites. Appl Phys Lett 76: 2868–2870. doi: 10.1063/1.126500
![]() |
[53] |
Allaoui A, Bai S, Cheng HM, et al. (2002) Mechanical and electrical properties of a MWNT/epoxy composite. Compos Sci Technol 62: 1993–1998. doi: 10.1016/S0266-3538(02)00129-X
![]() |
[54] |
Ajayan PM, Schadler LS, Giannaris C, et al. (2000) Single-walled carbon nanotube–polymer composites: strength and weakness. Adv Mater 12: 750–753. doi: 10.1002/(SICI)1521-4095(200005)12:10<750::AID-ADMA750>3.0.CO;2-6
![]() |
[55] |
Li Y, Zhang H, Porwal H, et al. (2017) Mechanical, electrical and thermal properties of in-situ exfoliated graphene/epoxy nanocomposites. Compos Part A-Appl S 95: 229–236. doi: 10.1016/j.compositesa.2017.01.007
![]() |
[56] |
Zhang Y, Park SJ (2017) Enhanced interfacial interaction by grafting carboxylated-macromolecular chains on nanodiamond surfaces for epoxy-based thermosets. J Polym Sci Pol Phys 55: 1890–1898. doi: 10.1002/polb.24522
![]() |
[57] |
Zhang Y, Rhee KY, Park SJ (2017) Nanodiamond nanocluster-decorated graphene oxide/epoxy nanocomposites with enhanced mechanical behavior and thermal stability. Compos Part B-Eng 114: 111–120. doi: 10.1016/j.compositesb.2017.01.051
![]() |
[58] |
Sharmila TKB, Antony JV, Jayakrishnan MP, et al. (2016) Mechanical, thermal and dielectric properties of hybrid composites of epoxy and reduced graphene oxide/iron oxide. Mater Design 90: 66–75. doi: 10.1016/j.matdes.2015.10.055
![]() |
[59] |
Shaffer MSP, Windle AH (1999) Fabrication and characterization of carbon nanotube/poly(vinyl alcohol) composites. Adv Mater 11: 937–941. doi: 10.1002/(SICI)1521-4095(199908)11:11<937::AID-ADMA937>3.0.CO;2-9
![]() |
[60] |
Rizzatti MR, De Araujo MA, Livi RP (1995) Bulk and surface modifications of insulating poly(paraphenylene sulphide) films by ion bombardment. Surf Coat Tech 70: 197–202. doi: 10.1016/0257-8972(94)02275-U
![]() |
[61] |
Liu Y, Gao L (2005) A study of the electrical properties of carbon nanotube-NiFe2O4 composites: Effect of the surface treatment of the carbon nanotubes. Carbon 43: 47–52. doi: 10.1016/j.carbon.2004.08.019
![]() |
[62] |
Park OK, Jeevananda T, Kim NH, et al. (2009) Effects of surface modification on the dispersion and electrical conductivity of carbon nanotube/polyaniline composites. Scripta Mater 60: 551–554. doi: 10.1016/j.scriptamat.2008.12.005
![]() |
1. | Hai-yang Xu, Heng-you Lan, Fan Zhang, General semi-implicit approximations with errors for common fixed points of nonexpansive-type operators and applications to Stampacchia variational inequality, 2022, 41, 2238-3603, 10.1007/s40314-022-01890-7 | |
2. | Yan Wang, Rui Wu, Shanshan Gao, The Existence Theorems of Fractional Differential Equation and Fractional Differential Inclusion with Affine Periodic Boundary Value Conditions, 2023, 15, 2073-8994, 526, 10.3390/sym15020526 | |
3. | Sumati Kumari Panda, Thabet Abdeljawad, Fahd Jarad, Chaotic attractors and fixed point methods in piecewise fractional derivatives and multi-term fractional delay differential equations, 2023, 46, 22113797, 106313, 10.1016/j.rinp.2023.106313 | |
4. | Philip N. A. Akuka, Baba Seidu, C. S. Bornaa, Marko Gosak, Mathematical Analysis of COVID-19 Transmission Dynamics Model in Ghana with Double-Dose Vaccination and Quarantine, 2022, 2022, 1748-6718, 1, 10.1155/2022/7493087 | |
5. | SUMATI KUMARI PANDA, ABDON ATANGANA, THABET ABDELJAWAD, EXISTENCE RESULTS AND NUMERICAL STUDY ON NOVEL CORONAVIRUS 2019-NCOV/ SARS-COV-2 MODEL USING DIFFERENTIAL OPERATORS BASED ON THE GENERALIZED MITTAG-LEFFLER KERNEL AND FIXED POINTS, 2022, 30, 0218-348X, 10.1142/S0218348X22402149 | |
6. | Tahair Rasham, Separate families of fuzzy dominated nonlinear operators with applications, 2024, 70, 1598-5865, 4271, 10.1007/s12190-024-02133-0 | |
7. | Sumati Kumari Panda, Thabet Abdeljawad, A. M. Nagy, On uniform stability and numerical simulations of complex valued neural networks involving generalized Caputo fractional order, 2024, 14, 2045-2322, 10.1038/s41598-024-53670-4 | |
8. | Sumati Kumari Panda, Kumara Swamy Kalla, A.M. Nagy, Limmaka Priyanka, Numerical simulations and complex valued fractional order neural networks via (ɛ – μ)-uniformly contractive mappings, 2023, 173, 09600779, 113738, 10.1016/j.chaos.2023.113738 | |
9. | Hammed Anuoluwapo Abass, Maggie Aphane, Morufu Oyedunsi Olayiwola, An inertial method for solving systems of generalized mixed equilibrium and fixed point problems in reflexive Banach spaces, 2023, 16, 1793-5571, 10.1142/S1793557123502078 | |
10. | Yassine Adjabi, Fahd Jarad, Mokhtar Bouloudene, Sumati Kumari Panda, Revisiting generalized Caputo derivatives in the context of two-point boundary value problems with the p-Laplacian operator at resonance, 2023, 2023, 1687-2770, 10.1186/s13661-023-01751-0 | |
11. | Nihar Kumar Mahato, Bodigiri Sai Gopinadh, , 2024, Chapter 15, 978-981-99-9545-5, 339, 10.1007/978-981-99-9546-2_15 | |
12. | Sumati Kumari Panda, Velusamy Vijayakumar, Bodigiri Sai Gopinadh, Fahd Jarad, 2024, Chapter 6, 978-981-99-9545-5, 177, 10.1007/978-981-99-9546-2_6 | |
13. | Sumati Kumari Panda, Ilyas Khan, Vijayakumar Velusamy, Shafiullah Niazai, Enhancing automic and optimal control systems through graphical structures, 2024, 14, 2045-2322, 10.1038/s41598-024-53244-4 | |
14. | P K Santra, G S Mahapatra, Sanjoy Basu, Stability analysis of fractional epidemic model for two infected classes incorporating hospitalization impact, 2024, 99, 0031-8949, 065237, 10.1088/1402-4896/ad4692 | |
15. | Anupam Das, Bipan Hazarika, Mohsen Rabbani, 2024, Chapter 10, 978-981-99-9206-5, 165, 10.1007/978-981-99-9207-2_10 | |
16. | Tahair Rasham, Sumati Kumari Panda, Ghada Ali Basendwah, Aftab Hussain, Multivalued nonlinear dominated mappings on a closed ball and associated numerical illustrations with applications to nonlinear integral and fractional operators, 2024, 10, 24058440, e34078, 10.1016/j.heliyon.2024.e34078 | |
17. | Sumati Kumari Panda, Velusamy Vijayakumar, Kottakkaran Sooppy Nisar, Applying periodic and anti-periodic boundary conditions in existence results of fractional differential equations via nonlinear contractive mappings, 2023, 2023, 1687-2770, 10.1186/s13661-023-01778-3 | |
18. | Sumati Kumari Panda, Kottakkaran Sooppy Nisar, Velusamy Vijayakumar, Bipan Hazarika, Solving existence results in multi-term fractional differential equations via fixed points, 2023, 51, 22113797, 106612, 10.1016/j.rinp.2023.106612 | |
19. | Sumati Kumari Panda, Velusamy Vijayakumar, Results on finite time stability of various fractional order systems, 2023, 174, 09600779, 113906, 10.1016/j.chaos.2023.113906 | |
20. | Sumati Kumari Panda, A.M. Nagy, Velusamy Vijayakumar, Bipan Hazarika, Stability analysis for complex-valued neural networks with fractional order, 2023, 175, 09600779, 114045, 10.1016/j.chaos.2023.114045 | |
21. | Mokhtar Bouloudene, Fahd Jarad, Yassine Adjabi, Sumati Kumari Panda, Quasilinear Coupled System in the Frame of Nonsingular ABC-Derivatives with p-Laplacian Operator at Resonance, 2024, 23, 1575-5460, 10.1007/s12346-023-00902-z | |
22. | Sumati Kumari Panda, Vijayakumar Velusamy, Ilyas Khan, Shafiullah Niazai, Computation and convergence of fixed-point with an RLC-electric circuit model in an extended b-suprametric space, 2024, 14, 2045-2322, 10.1038/s41598-024-59859-x |
β | ||||||||
0.8 | 1 | 1.4 | ||||||
Estimator | n | point | B | MSE | B | MSE | B | MSE |
Usual | 25 | t1 | 0.0133 | 0.0036 | 0.0120 | 0.0037 | 0.0115 | 0.0035 |
t2 | 0.0146 | 0.0075 | 0.0096 | 0.0075 | 0.0144 | 0.0074 | ||
t3 | 0.0113 | 0.0105 | 0.0086 | 0.0099 | 0.0157 | 0.0100 | ||
t4 | 0.0118 | 0.0242 | 0.0150 | 0.0212 | 0.0203 | 0.0232 | ||
50 | t1 | 0.0071 | 0.0019 | 0.0068 | 0.0019 | 0.0062 | 0.0018 | |
t2 | 0.0093 | 0.0040 | 0.0074 | 0.0039 | 0.0071 | 0.0039 | ||
t3 | 0.0055 | 0.0053 | 0.0069 | 0.0055 | 0.0050 | 0.0054 | ||
t4 | 0.0070 | 0.0110 | 0.0050 | 0.0115 | 0.0059 | 0.0118 | ||
100 | t1 | 0.0057 | 0.0010 | 0.0049 | 0.0009 | 0.0043 | 0.0010 | |
t2 | 0.0033 | 0.0021 | 0.0035 | 0.0022 | 0.0035 | 0.0020 | ||
t3 | 0.0017 | 0.0028 | 0.0058 | 0.0027 | 0.0022 | 0.0028 | ||
t4 | -0.0010 | 0.0064 | 0.0027 | 0.0059 | 0.0009 | 0.0058 | ||
Increasing | 25 | t1 | 0.0395 | 0.0032 | 0.0388 | 0.0031 | 0.0386 | 0.0030 |
t2 | 0.0480 | 0.0064 | 0.0466 | 0.0065 | 0.0503 | 0.0065 | ||
t3 | 0.0440 | 0.0082 | 0.0435 | 0.0079 | 0.0473 | 0.0086 | ||
t4 | 0.0370 | 0.0204 | 0.0392 | 0.0182 | 0.0455 | 0.0196 | ||
50 | t1 | 0.0224 | 0.0016 | 0.0232 | 0.0016 | 0.0238 | 0.0017 | |
t2 | 0.0286 | 0.0035 | 0.0282 | 0.0034 | 0.0268 | 0.0033 | ||
t3 | 0.0244 | 0.0043 | 0.0252 | 0.0047 | 0.0238 | 0.0045 | ||
t4 | 0.0192 | 0.0105 | 0.0175 | 0.0108 | 0.0163 | 0.0110 | ||
100 | t1 | 0.0145 | 0.0009 | 0.0141 | 0.0008 | 0.0139 | 0.0009 | |
t2 | 0.0140 | 0.0019 | 0.0141 | 0.0019 | 0.0148 | 0.0019 | ||
t3 | 0.0103 | 0.0026 | 0.0137 | 0.0026 | 0.0115 | 0.0025 | ||
t4 | 0.0063 | 0.0060 | 0.0058 | 0.0057 | 0.0082 | 0.0055 |
c | ||||||||
0.5 | 0.7 | 1.1 | ||||||
Estimator | n | point | B | MSE | B | MSE | B | MSE |
Usual | 25 | t1 | -0.0040 | 0.1866 | 0.0149 | 0.0686 | 0.0018 | 0.0242 |
t2 | 0.0030 | 0.2704 | -0.0067 | 0.1025 | -0.0042 | 0.0346 | ||
t3 | -0.0412 | 0.4076 | -0.0285 | 0.1508 | -0.0082 | 0.0469 | ||
t4 | -0.0591 | 0.5858 | -0.0349 | 0.2085 | -0.0156 | 0.0620 | ||
50 | t1 | 0.0017 | 0.0903 | -0.0100 | 0.0407 | 0.0040 | 0.0113 | |
t2 | -0.0152 | 0.1273 | -0.0178 | 0.0554 | 0.0005 | 0.0159 | ||
t3 | -0.0312 | 0.1913 | -0.0296 | 0.0816 | -0.0025 | 0.0221 | ||
t4 | -0.0534 | 0.3003 | -0.0345 | 0.1103 | -0.0004 | 0.0273 | ||
100 | t1 | -0.0086 | 0.0461 | -0.0017 | 0.0172 | 0.0008 | 0.0057 | |
t2 | -0.0089 | 0.0577 | -0.0030 | 0.0253 | -0.0010 | 0.0080 | ||
t3 | -0.0137 | 0.0823 | -0.0057 | 0.0343 | -0.0037 | 0.0107 | ||
t4 | -0.0222 | 0.1243 | -0.0086 | 0.0495 | -0.0035 | 0.0141 | ||
Increasing | 25 | t1 | 0.0004 | 0.1832 | 0.0271 | 0.0603 | 0.1125 | 0.0197 |
t2 | 0.0032 | 0.2702 | -0.0018 | 0.1008 | 0.0049 | 0.0304 | ||
t3 | -0.0411 | 0.4076 | -0.0285 | 0.1508 | -0.0043 | 0.0438 | ||
t4 | -0.0591 | 0.5858 | -0.0349 | 0.2085 | -0.0155 | 0.0620 | ||
50 | t1 | 0.0057 | 0.0897 | 0.0009 | 0.0373 | 0.0830 | 0.0087 | |
t2 | -0.0135 | 0.1261 | -0.0142 | 0.0539 | 0.0048 | 0.0151 | ||
t3 | -0.0307 | 0.1906 | -0.0286 | 0.0802 | -0.0012 | 0.0218 | ||
t4 | -0.0534 | 0.3002 | -0.0343 | 0.1103 | -0.0004 | 0.0273 | ||
100 | t1 | -0.0046 | 0.0447 | 0.0014 | 0.0166 | 0.0631 | 0.0046 | |
t2 | -0.0072 | 0.0570 | -0.0017 | 0.0252 | 0.0008 | 0.0077 | ||
t3 | -0.0137 | 0.0823 | -0.0042 | 0.0339 | -0.0029 | 0.0105 | ||
{\boldsymbol{t}}_{4} | -0.0222 | 0.1243 | -0.0085 | 0.0495 | -0.0033 | 0.0140 |
Patient (i) | 1 | 2 | 3 | 4 | 5 | 6 | 7 | 8 | 9 |
{T}_{1i} | 6.9 | 1.63 | 13.83 | 35.53 | 14.8 | 6.2 | 22 | 1.7 | 43.03 |
{T}_{2i} | 20.17 | 10.27 | 5.67 | 5.90 | 33.9 | 1.73 | 30.2 | 1.7 | 1.77 |
Patient (i) | 10 | 11 | 12 | 13 | 14 | 15 | 16 | 17 | 18 |
{T}_{1i} | 6.53 | 42.17 | 48.43 | 9.6 | 7.6 | 1.8 | 9.9 | 13.77 | 0.83 |
{T}_{2i} | 18.7 | 42.17 | 14.3 | 13.33 | 14.27 | 34.57 | 21.57 | 13.77 | 10.33 |
Patient (i) | 19 | 20 | 21 | 22 | 23 | 24 | |||
{T}_{1i} | 1.97 | 11.3 | 30.4 | 19 | 5.43 | 46.63 | |||
{T}_{2i} | 11.07 | 2.1 | 13.97 | 13.80 | 13.57 | 42.43 |
\beta | ||||||||
0.8 | 1 | 1.4 | ||||||
Estimator | n | point | B | MSE | B | MSE | B | MSE |
Usual | 25 | {t}_{1} | 0.0133 | 0.0036 | 0.0120 | 0.0037 | 0.0115 | 0.0035 |
{t}_{2} | 0.0146 | 0.0075 | 0.0096 | 0.0075 | 0.0144 | 0.0074 | ||
{t}_{3} | 0.0113 | 0.0105 | 0.0086 | 0.0099 | 0.0157 | 0.0100 | ||
{t}_{4} | 0.0118 | 0.0242 | 0.0150 | 0.0212 | 0.0203 | 0.0232 | ||
50 | {t}_{1} | 0.0071 | 0.0019 | 0.0068 | 0.0019 | 0.0062 | 0.0018 | |
{t}_{2} | 0.0093 | 0.0040 | 0.0074 | 0.0039 | 0.0071 | 0.0039 | ||
{t}_{3} | 0.0055 | 0.0053 | 0.0069 | 0.0055 | 0.0050 | 0.0054 | ||
{t}_{4} | 0.0070 | 0.0110 | 0.0050 | 0.0115 | 0.0059 | 0.0118 | ||
100 | {t}_{1} | 0.0057 | 0.0010 | 0.0049 | 0.0009 | 0.0043 | 0.0010 | |
{t}_{2} | 0.0033 | 0.0021 | 0.0035 | 0.0022 | 0.0035 | 0.0020 | ||
{t}_{3} | 0.0017 | 0.0028 | 0.0058 | 0.0027 | 0.0022 | 0.0028 | ||
{t}_{4} | -0.0010 | 0.0064 | 0.0027 | 0.0059 | 0.0009 | 0.0058 | ||
Increasing | 25 | {t}_{1} | 0.0395 | 0.0032 | 0.0388 | 0.0031 | 0.0386 | 0.0030 |
{t}_{2} | 0.0480 | 0.0064 | 0.0466 | 0.0065 | 0.0503 | 0.0065 | ||
{t}_{3} | 0.0440 | 0.0082 | 0.0435 | 0.0079 | 0.0473 | 0.0086 | ||
{t}_{4} | 0.0370 | 0.0204 | 0.0392 | 0.0182 | 0.0455 | 0.0196 | ||
50 | {t}_{1} | 0.0224 | 0.0016 | 0.0232 | 0.0016 | 0.0238 | 0.0017 | |
{t}_{2} | 0.0286 | 0.0035 | 0.0282 | 0.0034 | 0.0268 | 0.0033 | ||
{t}_{3} | 0.0244 | 0.0043 | 0.0252 | 0.0047 | 0.0238 | 0.0045 | ||
{t}_{4} | 0.0192 | 0.0105 | 0.0175 | 0.0108 | 0.0163 | 0.0110 | ||
100 | {t}_{1} | 0.0145 | 0.0009 | 0.0141 | 0.0008 | 0.0139 | 0.0009 | |
{t}_{2} | 0.0140 | 0.0019 | 0.0141 | 0.0019 | 0.0148 | 0.0019 | ||
{t}_{3} | 0.0103 | 0.0026 | 0.0137 | 0.0026 | 0.0115 | 0.0025 | ||
{t}_{4} | 0.0063 | 0.0060 | 0.0058 | 0.0057 | 0.0082 | 0.0055 |
c | ||||||||
0.5 | 0.7 | 1.1 | ||||||
Estimator | n | point | B | MSE | B | MSE | B | MSE |
Usual | 25 | {\boldsymbol{t}}_{1} | -0.0040 | 0.1866 | 0.0149 | 0.0686 | 0.0018 | 0.0242 |
{\boldsymbol{t}}_{2} | 0.0030 | 0.2704 | -0.0067 | 0.1025 | -0.0042 | 0.0346 | ||
{\boldsymbol{t}}_{3} | -0.0412 | 0.4076 | -0.0285 | 0.1508 | -0.0082 | 0.0469 | ||
{\boldsymbol{t}}_{4} | -0.0591 | 0.5858 | -0.0349 | 0.2085 | -0.0156 | 0.0620 | ||
50 | {\boldsymbol{t}}_{1} | 0.0017 | 0.0903 | -0.0100 | 0.0407 | 0.0040 | 0.0113 | |
{\boldsymbol{t}}_{2} | -0.0152 | 0.1273 | -0.0178 | 0.0554 | 0.0005 | 0.0159 | ||
{\boldsymbol{t}}_{3} | -0.0312 | 0.1913 | -0.0296 | 0.0816 | -0.0025 | 0.0221 | ||
{\boldsymbol{t}}_{4} | -0.0534 | 0.3003 | -0.0345 | 0.1103 | -0.0004 | 0.0273 | ||
100 | {\boldsymbol{t}}_{1} | -0.0086 | 0.0461 | -0.0017 | 0.0172 | 0.0008 | 0.0057 | |
{\boldsymbol{t}}_{2} | -0.0089 | 0.0577 | -0.0030 | 0.0253 | -0.0010 | 0.0080 | ||
{\boldsymbol{t}}_{3} | -0.0137 | 0.0823 | -0.0057 | 0.0343 | -0.0037 | 0.0107 | ||
{\boldsymbol{t}}_{4} | -0.0222 | 0.1243 | -0.0086 | 0.0495 | -0.0035 | 0.0141 | ||
Increasing | 25 | {\boldsymbol{t}}_{1} | 0.0004 | 0.1832 | 0.0271 | 0.0603 | 0.1125 | 0.0197 |
{\boldsymbol{t}}_{2} | 0.0032 | 0.2702 | -0.0018 | 0.1008 | 0.0049 | 0.0304 | ||
{\boldsymbol{t}}_{3} | -0.0411 | 0.4076 | -0.0285 | 0.1508 | -0.0043 | 0.0438 | ||
{\boldsymbol{t}}_{4} | -0.0591 | 0.5858 | -0.0349 | 0.2085 | -0.0155 | 0.0620 | ||
50 | {\boldsymbol{t}}_{1} | 0.0057 | 0.0897 | 0.0009 | 0.0373 | 0.0830 | 0.0087 | |
{\boldsymbol{t}}_{2} | -0.0135 | 0.1261 | -0.0142 | 0.0539 | 0.0048 | 0.0151 | ||
{\boldsymbol{t}}_{3} | -0.0307 | 0.1906 | -0.0286 | 0.0802 | -0.0012 | 0.0218 | ||
{\boldsymbol{t}}_{4} | -0.0534 | 0.3002 | -0.0343 | 0.1103 | -0.0004 | 0.0273 | ||
100 | {\boldsymbol{t}}_{1} | -0.0046 | 0.0447 | 0.0014 | 0.0166 | 0.0631 | 0.0046 | |
{\boldsymbol{t}}_{2} | -0.0072 | 0.0570 | -0.0017 | 0.0252 | 0.0008 | 0.0077 | ||
{\boldsymbol{t}}_{3} | -0.0137 | 0.0823 | -0.0042 | 0.0339 | -0.0029 | 0.0105 | ||
{\boldsymbol{t}}_{4} | -0.0222 | 0.1243 | -0.0085 | 0.0495 | -0.0033 | 0.0140 |
Patient (i) | 1 | 2 | 3 | 4 | 5 | 6 | 7 | 8 | 9 |
{T}_{1i} | 6.9 | 1.63 | 13.83 | 35.53 | 14.8 | 6.2 | 22 | 1.7 | 43.03 |
{T}_{2i} | 20.17 | 10.27 | 5.67 | 5.90 | 33.9 | 1.73 | 30.2 | 1.7 | 1.77 |
Patient (i) | 10 | 11 | 12 | 13 | 14 | 15 | 16 | 17 | 18 |
{T}_{1i} | 6.53 | 42.17 | 48.43 | 9.6 | 7.6 | 1.8 | 9.9 | 13.77 | 0.83 |
{T}_{2i} | 18.7 | 42.17 | 14.3 | 13.33 | 14.27 | 34.57 | 21.57 | 13.77 | 10.33 |
Patient (i) | 19 | 20 | 21 | 22 | 23 | 24 | |||
{T}_{1i} | 1.97 | 11.3 | 30.4 | 19 | 5.43 | 46.63 | |||
{T}_{2i} | 11.07 | 2.1 | 13.97 | 13.80 | 13.57 | 42.43 |