Research article

On stability of a class of second alpha-order fractal differential equations

  • Received: 03 November 2019 Accepted: 11 February 2020 Published: 26 February 2020
  • MSC : 28A78, 28A80, 35B35, 35B40, 81Q35

  • In this paper, we give a review of fractal calculus which is an expansion of standard calculus. Fractal calculus is applied for functions that are not differentiable or integrable on totally disconnected fractal sets such as middle-μ Cantor sets. Analogues of the Lyapunov functions and their features are given for asymptotic behaviors of fractal differential equations. The stability of fractal differentials in the sense of Lyapunov is defined. For the suggested fractal differential equations, sufficient conditions for the stability and uniform boundedness and convergence of the solutions are presented and proved. We present examples and graphs for more details of the results.

    Citation: Cemil Tunç, Alireza Khalili Golmankhaneh. On stability of a class of second alpha-order fractal differential equations[J]. AIMS Mathematics, 2020, 5(3): 2126-2142. doi: 10.3934/math.2020141

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  • In this paper, we give a review of fractal calculus which is an expansion of standard calculus. Fractal calculus is applied for functions that are not differentiable or integrable on totally disconnected fractal sets such as middle-μ Cantor sets. Analogues of the Lyapunov functions and their features are given for asymptotic behaviors of fractal differential equations. The stability of fractal differentials in the sense of Lyapunov is defined. For the suggested fractal differential equations, sufficient conditions for the stability and uniform boundedness and convergence of the solutions are presented and proved. We present examples and graphs for more details of the results.


    The first COVID-19 infected case was identified in late 2019 in China and then spread around the globe with extraordinary speed. By March 11, 2021, the COVID-19 confirmed cases were registered in 213 countries, and the World Health Organization (WHO) declared this disease a global pandemic; see Ngo et al. [1]. Due to this pandemic, every aspect of life has been disturbed and almost every region around the globe has faced unexpected situations. In every region, among other sectors affected by this pandemic, the health sector is the most affected area; see Pfefferbaum and North [2], Kim et al. [3], Campion et al. [4], Gloster et al. [5], Talevi et al. [6], and Wastnedge et al. [7]. As of December 13, 2021, 09:09 GMT (Greenwich Mean Time), totally confirmed cases (TCC) have touched a figure of 270488249, the total number of deaths (TND) has reached 5324113, and 243235043 infected persons have been recovered. For the latest updates and details about the COVID-19 events; see https://www.worldometers.info/coronavirus/.

    The top fifteen countries with the higher TND, include (ⅰ) America with 817956 deaths, (ⅱ) Brazil with 616941 deaths, (ⅲ) India with 475636 deaths, (ⅳ) Mexico with 296672 deaths, (ⅴ) Russia with 290604 deaths, (ⅵ) Peru with 201,650 deaths, (ⅶ) the United Kingdom with 146439 deaths, (ⅷ) Indonesia with 143936 deaths, (ⅸ) Italy with 134831 deaths, (ⅹ) Iran with 130722 deaths, (xi) Colombia with 129107 deaths, (xii) France with 120431 deaths, (xiii) Argentina with 116771 deaths, (ivx) Germany with 106331 deaths, and (xv) Ukraine with 91215 deaths. For a brief overview of country-wise statistics related to the COVID-19 pandemic, we refer to Bo et al. [8].

    Due to the unprecedented situation of the COVID-19 pandemic, it is necessary to have the best description and efficient modeling of the COVID-19 events. Statistical methodologies are very useful in modeling and predicting lifetime events. Several statistical studies on this pandemic have appeared. For example, Moreau [9] predicted the COVID-19 phenomena in Brazil. Tuli et al. [10] predicted the growth trend of the COVID-19 pandemic. Rahman et al. [11] implemented the Weibull model for the COVID-19 data analysis. Almetwally [12] introduced a new inverted Topp-Leone (NITL) distribution and used it for modeling the COVID-19 mortality rate data.

    These statistical studies are carried out either by implementing the existing models or by proposing new methodologies to update/modify the existing distributions. In the recent era of DT (distribution theory), the development of new methods to introduce new distributions is an important research topic. In this regard, numerous methods to update the distributional flexibility of the existing model have been introduced; see Alizadeh et al. [13] Chipepa et al. [14], Handique et al. [15], Tahir et al. [16], Zaidi et al. [17], Riad et al. [18], and Bakr et al. [19]. For more information about the applicability of statistical models in applied sectors, we refer to Xu et al. [20], and Luo et al. [21].

    In this paper, we further contribute to the literature on DT by proposing a new approach, namely, a new extended exponential (NEExp) family. It can be used to obtain the updated versions of the classical/traditional (such as Weibull, beta, gamma, Gumble, Rayleigh, etc.) or other existing models. The NEExp family is proposed by incorporating the T-X distributions approach of Alzaatreh et al. [22] with the exponential distribution with probability density function (PDF) et, taken as a parent model.

    The novelty and key motivations of the proposed method are the followings:

    ● The method introduced in this paper is new and has not been studied in the literature.

    ● The proposed method is a very simple and convenient approach of adding an extra parameter to obtain the updated versions of the existing models.

    ● The proposed approach helps to improve the flexibility and characteristics of the existing models.

    ● The proposed method provides a close fit to healthcare and other related data sets.

    The reaming work carried out in this paper is organized as follows. In Section 2, we define the proposed family and discuss its special case. Certain mathematical properties of the NEExp family are provided in Section 3. The estimation of the parameters and a simulation study are provided in Section 4. To illustrate the NEExp family, two practical data sets are analyzed in Section 5. To forecast the COVID-19 data sets, the machine learning methods are discussed in Section 6. Finally, some concluding remarks, limitations of the proposed method, and future study plans are discussed in Section 7.

    This section is divided into two subsections. In the very first subsection, we define the proposed NEExp family of distributions. Whereas, the second subsection is devoted to studying a special case of the NEExp family of distributions

    Let V has a NEExp family, if its distribution function (DF) F(v;δ,ϑϑ) is given by

    F(v;δ,ϑϑ)=1δ[1M(v;ϑϑ)]δ+M(v;ϑϑ),vR, (2.1)

    where δ>0 is an additional parameter and ϑϑ is a vector of parameters associated with the baseline DF M(v;ϑϑ).

    Furthermore, in link to F(v;δ,ϑϑ), the PDF f(v;δ,ϑϑ) of the NEExp family is

    f(v;δ,ϑϑ)=δ(δ+1)m(v;ϑϑ)[δ+M(v;ϑϑ)]2,vR. (2.2)

    For vR, the survival function (SF) S(v;δ,ϑϑ)=1F(v;δ,ϑϑ), and hazard function (HF) h(v;δ,ϑϑ)=f(v;δ,ϑϑ)1F(v;δ,ϑϑ) of the NEExp family are given by

    S(v;δ,ϑϑ)=δ[1M(v;ϑϑ)]δ+M(v;ϑϑ),

    and

    h(v;δ,ϑϑ)=(δ+1)m(v;ϑϑ)[1M(v;ϑϑ)][δ+M(v;ϑϑ)],

    respectively.

    A special member of the NEExp family called, a new extended exponential Weibull (NEExp-Weibull) model is discussed in the next subsection. The NEExp-Weibull model is introduced by using the DF of the Weibull model in Eq (2.1). The DF M(v;ϑϑ) of the Weibull model is given by

    M(v;ϑϑ)=1eφ2vφ1,v0,φ1>0,φ2>0, (2.3)

    with PDF m(v;ϑϑ) given by

    m(v;ϑϑ)=φ1φ2vφ11eφ2vφ1,v>0,φ1>0,φ2>0,

    where ϑϑ=(φ1,φ2). By incorporating Eq (2.3) in Eq (2.1), we reach at the DF of the NEExp-Weibull model; see Subsection 2.2.

    A random variable V has the NEExp-Weibull model with parameters φ1>0,φ2>0, and δ>0, if its DF F(v;δ,ϑϑ) and PDF F(v;δ,ϑϑ), are given by

    F(v;δ,ϑϑ)=1δeφ2vφ1δ+1eφ2vφ1,v0, (2.4)

    and

    f(v;δ,ϑϑ)=δ(δ+1)φ1φ2vφ11eφ2vφ1[δ+1eφ2vφ1]2,v>0, (2.5)

    respectively.

    For the NEExp-Weibull model with DF in Eq (2.4) and PDF in Eq (2.5), the SF ˉF(v;δ,ϑϑ)=1F(v;δ,ϑϑ), HF h(v;δ,ϑϑ)=f(v;δ,ϑϑ)ˉF(v;δ,ϑϑ), and CHF H(v;δ,ϑϑ)=log(ˉF(v;δ,ϑϑ)) are given by

    ˉF(v;δ,ϑϑ)=δeφ2vφ1δ+1eφ2vφ1,v>0,
    h(v;δ,ϑϑ)=(δ+1)φ1φ2vφ11[δ+1eφ2vφ1],v>0,

    and

    H(v;δ,ϑϑ)=log(δeφ2vφ1δ+1eφ2vφ1),v>0,

    respectively.

    A visual behavior of f(v;δ,ϑϑ) for (i) φ1=5.5,φ2=0.2,δ=9.5 (red curve) (ii) φ1=4.5,φ2=0.6,δ=2.5, (green curve) (iii) φ1=0.5,φ2=1.6,δ=1.5, (blue curve) and (iv) φ1=1.9,φ2=2.6,δ=2.5, (gold curve) is provided in Figure 1.

    Figure 1.  A visual behavior of f(v;δ,ϑϑ) for different values of φ1,φ2, and δ.

    From the visual illustration in Figure 1, we can see that f(v;δ,ϑϑ) possess different behaviors. For example, it takes (i) the left-skewed form (red curve), (ii) the symmetrical shape (green curve), (iii) the reverse-J shape (blue curve), and (iv) the right-skewed (gold curve).

    Here, we obtain different mathematical properties of the NEExp family with PDF f(v;δ,ϑϑ). These properties include QF (quantile function) expressed by Q(u), rth moment denoted by μ/r, MGF (moment generating function) represented by MV(t), RL (residual life), and RRL (reverse residual life) functions.

    The QF of the NEExp family can be obtained by inverting Eq (2.1). Let V have the NEExp family with DF F(v;δ,ϑϑ), then, its QF is given by

    vq=Q(u)=F1(δuδ+1u),

    where u(0,1).

    Suppose V follows the NEExp family of distributions, then the rth moment of the NEExp distributions is derived as

    μ/r=Ωvrδ(δ+1)m(v;ϑϑ)[δ+M(v;ϑϑ)]2dv,μ/r=(δ+1)δΩvrm(v;ϑϑ)[1+M(v;ϑϑ)δ]2dv. (3.1)

    Consider the series

    1(1+k)2=a=1(1)a1aka1. (3.2)

    By implementing Eq (3.2) with k=M(v;ϑϑ)δ, we have

    1(1+[M(v;ϑϑ)δ])2=a=1(1)a1a(M(v;ϑϑ)δ)a1. (3.3)

    Using Eq (3.3) in Eq (3.1), we get

    μ/r=(δ+1)δaa=1(1)a1aΩvrm(v;ϑϑ)M(v;ϑϑ)a1dv,μ/r=(δ+1)δaa=1(1)a1Ωvrka(v;ϑϑ)dv, (3.4)

    where ka(v;ϑϑ)=am(v;ϑϑ)M(v;ϑϑ)a1 is the exponentiated PDF, and a is a power parameter. We can also write Eq (3.4), as follows

    μ/r=(δ+1)δaa=1(1)a1λa,r, (3.5)

    where

    λa,r=Ωvrka(v;ϑϑ)dv. (3.6)

    Using the DF and PDF of the Weibull model in Eq (3.6), we get

    λa,r=0vrφ1φ2vφ11eφ2vφ1(1eφ2vφ1)a1dv. (3.7)

    On solving Eq (3.7), we get

    λa,r=a1k=0(1)k(a1k)0vrφ1φ2vφ11eφ2(k+1)vφ1dv,λa,r=a1k=0(1)k(a1k)Γ(rφ1+1)(φ2)rφ1(k+1)rφ1+1. (3.8)

    Using Eq (3.8) in Eq (3.5), we get the rth moment of the NEExp-Weibull model, given by

    μ/r=(δ+1)δaa=1a1k=0(1)a+k1(a1k)Γ(rφ1+1)(φ2)rφ1(k+1)rφ1+1. (3.9)

    Using r=1, in Eq (3.9), we get the first rth moment of the NEExp-Weibull model, given by

    μ/1=(δ+1)δaa=1a1k=0(1)a+k1(a1k)Γ(1φ1+1)(φ2)1φ1(k+1)1φ1+1.

    Using r=2, in Eq (3.9), we obtain the second rth moment of the NEExp-Weibull model, given by

    μ/2=(δ+1)δaa=1a1k=0(1)a+k1(a1k)Γ(2φ1+1)(φ2)2φ1(k+1)2φ1+1.

    Using r=3, in Eq (3.9), we obtain the third rth moment of the NEExp-Weibull model, given by

    μ/3=(δ+1)δaa=1a1k=0(1)a+k1(a1k)Γ(3φ1+1)(φ2)3φ1(k+1)3φ1+1.

    Using r=4, in Eq (3.9), we obtain the second rth moment of the NEExp-Weibull model, given by

    μ/4=(δ+1)δaa=1a1k=0(1)a+k1(a1k)Γ(4φ1+1)(φ2)4φ1(k+1)4φ1+1.

    Furthermore, the MGF of the NEExp-Weibull model is given by

    MV(t)=(δ+1)δaa=1a1k=0r=0(1)a+k1trr!(a1k)Γ(rφ1+1)(φ2)rφ1(k+1)rφ1+1.

    The RL of the NEExp-Weibull model represented by Rt(v), is given by

    Rt(v)=δeφ2(v+t)φ1δ+1eφ2(v+t)φ1×δ+1eφ2vφ1δeφ2vφ1.

    Furthermore, the RRL of the NEExp-Weibull model represented by ˉRt(v), is given by

    ˉRt(v)=δeφ2(vt)φ1δ+1eφ2(vt)φ1×δ+1eφ2vφ1δeφ2vφ1.

    In this section, we obtain the estimators (^φ1,^φ2,ˆδ) of the parameters (φ1,φ2,δ) by implementing the maximum likelihood estimation approach. Furthermore, for the evaluation of ^φ1,^φ2, and ˆδ, a simulation is also provided.

    Let V1,V2,...,Vp be a sample of size p observed from the PDF f(v;δ,ϑϑ). In link to f(v;δ,ϑϑ), the likelihood function (LH) λ(δ,ϑϑ|v1,v2,...,vp) is given by

    λ(δ,ϑϑ|v1,v2,...,vp)=pa=1f(va;δ,ϑϑ). (4.1)

    Using Eq (2.5) in Eq (4.1), we get

    λ(δ,ϑϑ|v1,v2,...,vp)=pa=1δ(δ+1)φ1φ2vφ11aeφ2vφ1a[δ+1eφ2vφ1a]2. (4.2)

    Corresponding to λ(φ1,φ2,δ|v1,v2,...,vp), the log LH π(δ,ϑϑ|v1,v2,...,vp) is given by

    π(δ,ϑϑ|v1,v2,...,vp)=plogδ+plog(δ+1)+plogφ1+plogφ2+(φ11)pa=1logvapa=1φ2vφ1a2pa=1log(δ+1eφ2vφ1a).

    The partial derivatives of π(δ,ϑϑ|v1,v2,...,vp) are given by

    φ1π(δ,ϑϑ|v1,v2,...,vp)=pφ1+pa=1logvaφ2pa=1(logva)vφ1a2φ2pa=1(logva)vφ1aeφ2vφ1a(δ+1eφ2vφ1a),
    φ2π(δ,ϑϑ|v1,v2,...,vp)=pφ2pa=1vφ1a2pa=1vφ1aeφ2vφ1a(δ+1eφ2vφ1a),

    and

    δπ(δ,ϑϑ|v1,v2,...,vp)=pδ+p(δ+1)2pa=11(δ+1eφ2vφ1a),

    respectively.

    On solving φ1π(δ,ϑϑ|v1,v2,...,vp)=0, φ2π(δ,ϑϑ|v1,v2,...,vp)=0, and δπ(δ,ϑϑ|v1,v2,...,vp), we get the estimators ^φ1,^φ2, and ˆδ, respectively.

    Now, we evaluate the performances of ^φ1,^φ1, and ˆφ by conducting a SiSt (simulation study). The SiSt is performed by adopting the following steps

    ● To carry out the SiSt, the RNs (random numbers) from the NEExp-Weibull model are generated using the inverse DF, given by

    vq=Q(u)=F1(δuδ+1u).

    ● The SiSt is performed for two different combination sets of φ1,φ2, and δ, such as (a) φ1=0.7,φ2=0.9,δ=1.4, and (b) φ1=1.5,φ2=1.4,δ=1.25.

    ● For both two sets of φ1, φ2, and δ, RNs of sizes p=25,50,75,...,500 are generated using the inverse DF method.

    ● The numerical values of the maximum likelihood estimators (MLEs) (^φ1,^φ2,ˆδ) of the parameters (φ1,φ2,δ) are obtained.

    ● Two statistical quantities/measures such as (i) mean square errors (MSEs) and (ii) Bias, are selected for assessing ^φ1, ^φ2, and ˆδ. The values of these quantities are given by

    MSE(ˆϕˆϕ)=1500500a=1(ˆϕˆϕaϕϕ)2,

    and

    Bias(ˆϕˆϕ)=1500500a=1(ˆϕˆϕaϕϕ),

    respectively, where ϕϕ=(φ1,φ2,δ).

    All the numerical and simulation results are obtained using optim() R-function with the argument method="L-BFGS-B". The results of the SiSt of the NEExp-Weibull distribution are reported in Tables 1 and 2, and presented visually in Figures 2 and 3.

    Table 1.  The results of the SiSt of the NEExp-Weibull model for φ1=0.7,δ=1.4,φ2=0.9.
    n Parameters MLEs MSEs Biases
    φ1 0.7439555 0.01816230 0.043955486
    20 δ 2.5224710 4.62452592 1.122470958
    φ2 0.9819897 0.08933255 0.081989688
    φ1 0.7261523 0.00675241 0.026152290
    40 δ 2.2436960 3.50148162 0.843695947
    φ2 0.9475541 0.04503070 0.047554140
    φ1 0.7174831 0.00469112 0.017483127
    60 δ 2.1504600 3.14461417 0.750459996
    φ2 0.9382455 0.03002095 0.038245459
    φ1 0.7139450 0.00303585 0.013945008
    80 δ 2.0166510 2.71268772 0.616651319
    φ2 0.9172897 0.02141037 0.017289700
    φ1 0.7118858 0.00250170 0.011885794
    100 δ 1.9587070 2.39162374 0.558707085
    φ2 0.9215668 0.01819720 0.021566823
    φ1 0.7071069 0.00095725 0.007106915
    200 δ 1.6315320 1.20339825 0.231531527
    φ2 0.8963361 0.00907772 -0.003663932
    φ1 0.7059804 0.00056999 0.005980353
    300 δ 1.4947460 0.59116842 0.094745813
    φ2 0.8942843 0.00510254 -0.005715678
    φ1 0.7046970 0.00042009 0.004696986
    400 δ 1.4758080 0.42345175 0.075807616
    φ2 0.8949554 0.00295727 -0.005044638
    φ1 0.7026197 0.00015114 0.002619658
    500 δ 1.4191470 0.17256813 0.019147385
    φ2 0.8958860 0.00155967 -0.004113986
    φ1 0.7021186 0.00011673 0.002118624
    600 δ 1.3973690 0.05930217 -0.002630857
    φ2 0.8964089 0.00084446 -0.003591110

     | Show Table
    DownLoad: CSV
    Table 2.  The results of the SiSt of the NEExp-Weibull model for φ1=0.6,δ=1.5,φ2=0.8.
    n Parameters MLEs MSEs Biases
    φ1 0.6538964 1.61446e-02 0.053896399
    20 δ 2.3444560 3.753281849 0.844456065
    φ2 0.8422871 0.074129355 0.042287133
    φ1 0.6335936 6.57586e-03 0.033593572
    40 δ 2.0966990 2.835106550 0.596698837
    φ2 0.8114326 0.027465620 0.011432631
    φ1 0.6207884 3.08374e-03 0.020788424
    60 δ 1.9743140 2.393837599 0.474313588
    φ2 0.8107312 0.022889902 0.010731190
    φ1 0.6195547 2.83132e-03 0.019554745
    80 δ 1.8076620 1.762573786 0.307661602
    φ2 0.7912179 0.016246953 -0.008782086
    φ1 0.6135883 1.52055e-03 0.013588293
    100 δ 1.7689760 1.451201967 0.268976369
    φ2 0.7923297 0.011392565 -0.007670316
    φ1 0.6062087 4.83673e-04 0.006208661
    200 δ 1.5338360 0.437971185 0.033836372
    φ2 0.7870588 0.003783507 -0.012941210
    φ1 0.6050252 2.87229e-04 0.005025202
    300 δ 1.4799110 0.134430960 -0.020089413
    φ2 0.7911718 0.001925689 -0.008828233
    φ1 0.6021233 1.08930e-04 0.002123257
    400 δ 1.5034740 0.104238258 0.003473527
    φ2 0.7954403 0.000832362 -0.004559674
    φ1 0.6014035 6.62443e-05 0.001403539
    500 δ 1.4982590 0.048978064 -0.001741474
    φ2 0.7974116 0.000411811 -0.002588439
    φ1 0.6009386 3.77904e-05 0.000938590
    600 δ 1.4899270 0.005002637 -0.010072511
    φ2 0.7976296 0.000242969 -0.002370384

     | Show Table
    DownLoad: CSV
    Figure 2.  A visual display of the SiSt for φ1=0.7,δ=1.4,φ2=0.9.
    Figure 3.  A visual display of the SiSt for φ1=0.6, δ=1.5, φ2=0.8.

    The primary aim of the introduction of the proposed distribution is its implementation for data analysis in the health and other related sectors. This section illustrates the respective fact by analyzing two data sets. The first data set (Data 1) represents the mortality rates of the COVID-19 infected persons in Mexico. Whereas, the second illustration is based on taking another COVID-19 data from Holland.

    By analyzing these two COVID-19 data sets, the numerical results of the proposed model is compared with the

    ● Weibull model with SF given by

    S(v;φ1,φ2)=eφ2vφ1,v,φ1,φ2>0,

    ● Logarithmic Weibull (L-Weibull) model with SF given by

    S(v;φ1,φ2,θ,σ)=(1σ[1eφ2vφ1]σ[log(1eφ2vφ1)])α,v,φ1,φ2,α,σ>0,

    ● Novel exponent power-Weibull (NEP-Weibull) model with SF given by

    S(v;φ1,φ2,θ)=(11eφ2vφ1eeφ2vφ1)θ,v,φ1,φ2,θ>0,

    and

    ● New modified Weibull (NM-Weibull) model with SF given by

    S(v;φ1,φ2,σ)=1(1eφ2vφ1)σ[σeφ2vφ1],v,φ1,φ2,σ1,σ1.

    To figure out the best competitive model for the COVID-19 data, certain statistical tests such as the (i) AD (Anderson-Darling) test statistic given by AD=p1ppa=1(2a1)[logM(va)+log{1M(vpa+1)}], (ii) CM (Cramer-von Mises) test statistic expressed by CM=112p+pa=1[2a12pM(va)]2, and (iii) KS (Kolmogorov-Smirnov (KS) test statistic derived by KS=supv[Mp(v)M(v)], are considered.

    Here, we analyze the mortality rates of the patients infected by the COVID-19 pandemic in Mexico; see https://covid19.wh. It is also studied by Almongy et al. [23] using a new extension of the Rayleigh distribution. This data set consists of 106 observations and is recorded from March 4, 2020, to July 20, 2020. The data set is given by: 4.4130, 3.0525, 4.6955, 7.4810, 5.1915, 3.6335, 6.6100, 8.2490, 5.8325, 3.0075, 5.4275, 3.0610, 3.3280, 1.7200, 2.9270, 5.3425, 5.0175, 2.6210, 2.1720, 2.5715, 3.8150, 7.3020, 3.9515, 3.1850, 1.7685, 3.1635, 2.3650, 1.6075, 4.6420, 6.4390, 4.4065, 5.0215, 3.6300, 2.9925, 3.2060, 1.6975, 2.2120, 4.9675, 3.9200, 4.7750, 1.7495, 1.8755, 3.4840, 1.6430, 5.0790, 4.0540, 3.3485, 3.5755, 3.2800, 1.0385, 1.8890, 1.4940, 1.6680, 3.4070, 4.1625, 3.9270, 4.2755, 1.6140, 3.7430, 3.3125, 3.0700, 2.4545, 2.3305, 2.6960, 6.0210, 4.3480, 0.9075, 1.6635, 2.7030, 3.0910, 0.5205, 0.9000, 2.4745, 2.0445, 1.6795, 1.0350, 1.6490, 2.6585, 2.7210, 2.2785, 2.1460, 1.2500, 3.2675, 2.3240, 2.3485, 2.7295, 2.0600, 1.9610, 1.6095, 0.7010, 1.2190, 1.6285, 1.8160, 1.6165, 1.5135, 1.1760, 0.6025, 1.6090, 1.4630, 1.3005, 1.0325, 1.5145, 1.0290, 1.1630, 1.2530, 0.9615.

    Corresponding to the COVID-19 data (mortality rate of the COVID-19 infected persons) of Mexico, the summary measures are: minimum = 0.5205, 1st quartile = 1.6445, median = 2.6397, mean = 2.9112, 3rd quartile = 3.7970, maximum = 8.2490, variance = 2.640433, range = 7.7285, standard deviation = 1.624941, skewness = 0.9732453, and kurtosis = 3.666136.

    Corresponding to the mortality rate of the COVID-19 infected persons in Mexico, some basic plots are presented in Figure 4. The plots in Figure 4, show that the first data set is right-skewed and possesses the increasing failure rate behavior.

    Figure 4.  Basic plots of the Mexico data.

    Corresponding to the Mexico data, the values of ^φ1, ^φ2, and ˆδ are presented in Table 3. The standard errors (SEs) (numerical values in the parentheses) of ^φ1, ^φ2, and ˆδ are also presented in Table 3.

    Table 3.  The numerical values of ^φ1,^φ2,ˆδ,ˆα,ˆσ, and ˆθ using the mortality rate data.
    Model ^φ1 ^φ2 ˆδ ˆα ˆσ ˆθ
    NEExp-Weibull 2.53401 (0.31876) 0.01723 (0.01562) 0.26201 (0.24135) - - -
    Weibull 1.92738 (0.14019) 0.09976 (0.02220) - - - -
    L-Weibull 1.57117 (0.01001) 1.20372 (0.00879) - 0.16022 (0.01580) 0.45036 (0.01773) -
    NEP-Weibull 1.71906 (0.03634) 0.95340 (0.03634) - - - 0.15201 (0.01503)
    NM-Weibull 1.89237 (0.15734) 0.11004 (0.03088) - - 12.06058 (20.5532) -

     | Show Table
    DownLoad: CSV

    For the Mexico data, the values of the selected tests CM, AD, and KS of the fitted models are reported in Table 4. The associated p-value of fitted models is also provided in Table 4. From the numerical illustration in Table 4, we can see that the proposed model has the smallest values of CM, AD, and KS, and the largest p-value. These facts show that the proposed model is the best competitor. Besides the numerical illustration, a visual display of the performances of the proposed model is also provided in Figure 5.

    Table 4.  The analytical measures of the fitted models using Data 1.
    Model CM AD KS p-value
    NEExp-Weibull 0.05834 0.33674 0.06266 0.79940
    Weibull 0.10264 0.66004 0.07147 0.65100
    L-Weibull 0.06002 0.36130 0.07091 0.66060
    NEP-Weibull 0.07017 0.43993 0.07862 0.52880
    NM-Weibull 0.10723 0.68969 0.07024 0.67240

     | Show Table
    DownLoad: CSV
    Figure 5.  For the first data, the plots of the fitted DFs of the proposed and all the fitted models.

    Here, we provide a second illustration of the proposed model by analyzing another COVID-19 data taken from Holland; see Almongy et al. [23]. This data set consists of 30 observations and is recorded between March 31, 2020, and April 30, 2020. The second data set is given by: 7.4590, 3.7490, 3.4700, 5.3280, 1.4285, 1.1270, 6.1370, 5.1445, 5.4160, 3.5495, 1.7305, 1.8235, 2.9640, 6.6055, 3.9840, 3.7920, 2.6535, 2.5240, 2.7155, 2.7775, 3.0135, 2.0485, 1.8055, 2.4800, 2.2310, 1.9415, 0.9870, 0.6365, 0.7080, 2.1175.

    The summary measures of the mortality rate of the COVID-19 infected persons in Holland are: minimum = 0.6365, 1st quartile = 1.8530, median = 2.6845, mean = 3.0783, 3rd quartile = 3.7812, maximum = 7.4590, variance = 3.121073, range = 6.8225, standard deviation = 1.766656, skewness = 0.8339708, and kurtosis = 2.953478.

    In link to the mortality rate of the COVID-19 infected persons in Holland, some basic plots are sketched in Figure 6. From the plots in Figure 6, it is obvious that the second data set, related to the mortality rate of the COVID-19 infected persons, is skewed to the right and has increasing failure rate behavior.

    Figure 6.  Basic plots of the Holland data.

    Based on the Holland's COVID-19 data, the numerical values of estimators ^φ1,^φ2, and ˆδ are obtained in Table 5. Furthermore, the SEs of these estimators are also reported in Table 5.

    Table 5.  The numerical values of ^φ1,^φ2,ˆδ,ˆα,ˆσ, and ˆθ using the mortality rate data.
    Model ^φ1 ^φ2 ˆδ ˆα ˆσ ˆθ
    NEExp-Weibull 2.20197 (0.48765) 0.03704 (0.04876) 0.75896 (0.10983) - - -
    Weibull 1.92738 (0.14019) 0.09976 (0.02220) - - - -
    L-Weibull 1.42252 (0.51193) 0.12239 (0.05844) - 2.85548 (0.97654) 0.89686 (2.15028) -
    NEP-Weibull 1.77603 (0.07305) 1.03756 (0.07304) - - - 0.11297 (0.02890)
    NM-Weibull 2.00489 (0.28946) 0.06377 (0.04170) - - -2.41345 (3.47713)

     | Show Table
    DownLoad: CSV

    Corresponding to the Holland data, the p-value and values of CM, AD, and KS are reported in Table 6. From the numerical comparison of the fitted models in Table 6, it is obvious that the proposed model performs better than the other competitors as it has the largest p-value and smallest CM, AD, and KS values. In support of Table 6, the performances of the proposed model are also illustrated visually by plotting the estimated DF, PP, PDF, QQ, and SF; see Figure 7.

    Table 6.  The analytical measures of the fitted models using Data 2.
    Model CM AD KS p-value
    NEExp-Weibull 0.03088 0.20437 0.08557 0.96710
    Weibull 0.04794 0.29434 0.10236 0.88030
    L-Weibull 0.05165 0.31630 0.10144 0.88660
    NEP-Weibull 0.03423 0.22143 0.10418 0.86740
    NM-Weibull 0.03926 0.24960 0.08981 0.95100

     | Show Table
    DownLoad: CSV
    Figure 7.  For the first data, the plots of the fitted DFs of the proposed and all the fitted models.

    In this section, we implement three different machine learning algorithms, namely, SVR, NNAR, and RF to forecast the data set analyzed in Section 5. Before modeling, we split the data set into two parts; 80 percent as training data and 20 percent as testing data, followed by Qi and Zhang [24]. We apply all the models to training data and compare their forecasting performances using the testing data. To assess the out-of-sample (also known as post-sample) prediction accuracy, multistep ahead forecasts with RMSE and MAE are calculated.

    The SVR is a popular ML approach, which is used for regression as well as classification problems. The SVR was first developed by Cortes and Vapnik [25], and to date, it is one of the most widely used supervised learning methods that is based on structured risk minimization rule and statistical theory. The structured risk minimization rule maximizes prediction accuracy and mitigates the likelihood of over fitting.

    In practice, it can effectively approximate linear and nonlinear problems and work well for numerous problems. The SVR uses various kernel functions to figure out the similarity between two data points to tackle the non-linear situations. The main advantage of SVR lies in its potential to capture the predictors' nonlinearity and then utilize it to enhance forecasting accuracy. In our case, the set of predictors contains the lagged values. The SVR assists to detect the margin of error which is bearable in the model; see Ribeiro et al. [26] and Bibi et al. [27]. The SVR equation with kernel function can be expressed as

    Ft=hk=1(λkλk)N(ck,c)+μ, (6.1)

    where Ft is the outcome variable. The kernel function, N(ck,c) denotes the inner product, while μ is accommodated within the kernel function. In the literature, several kernel functions have been developed. Among them, the radial basis function (RBF) is the most popular, which can be illustrated as

    N(ck,c)=exp{||ckcN||22τ2}, (6.2)

    where the Euclidean distance between the two predictors squared vectors is represented by ||ckcN||2 and τ2 is basically the width of RBF; see Lu et al. [28]. Hence, in this study, we focus on the RBF kernel function for the SVR. Tuning the SVR model enable us to arrive at optimal parameters.

    Another ML approach is RF which is also known as the random decision forest. It falls within the supervised learning category. The RF is a very effective algorithm that is used for both regression and classification problems as proposed by Breiman [29]. Dietterich [30] argued that RF is considered the most efficient ensemble technique appearing in ML and fulfills good forecasting properties. The RF approach is employed in different areas, including stock trading, finance, e-commerce, and health care. It provides a forest out of a collection of decision trees that are usually estimated (trained) by employing the bagging approach.

    The RF approach discovers the output based on the decision trees' forecasts. The forecasts are computed by averaging the output of several trees. The improvement is achieved in prediction by expanding the number of trees. In other words, as the number of trees in the forest grows, a more accurate forecast is obtained and circumvents the issue of over fitting as well. To estimate the RF, we use three hyper parameters i.e., the number of trees, number of nodes, and sample repetition. The number of nodes and trees are utilized as 3 and 500, respectively.

    In general, neural networks (NNs) are basically a network or circuit of neurons. The artificial neural network (ANNs) is composed of nodes or artificial neurons. NNs are highly flexible computing frameworks for analyzing a wide range of nonlinear problems. A key advantage of such networks is that they have not required prior information regarding the functional form in the model establishing process, rather highly determined by the characteristics of data; see Peng et al. [31].

    A feedback NN is established with lagged realization as predictors and hidden layer(s) with dimension nodes. The neural network autoregression (NNAR) contains three layers such as (i) the input layer, (ii) the hidden layer, and (iii) the output layer. The NNAR model is fitted to forecast a time series by utilizing its past information as inputs Ft,Ft1,...,Ftm, the entire process refers to feedback delay, where t indicates the time delay parameter. The NNAR (m, n) entails that the hidden layer consists of m delayed inputs and n nodes. The mathematical form of NNAR can be illustrated as

    Ft=ω0+mc=1θωc(c+zn=1cnFti)+μ, (6.3)

    where cn(c=1,2,3,...,m,n=1,2,3,...,z) and ωc(c=1,2,3,...,m) are the weights of interconnection, and z is the length of input layers, and m is the length of hidden layers.

    The prediction accuracy of all ML techniques is quantified by using two statistical accuracy criteria computed from a testing data set. Statistically, the forecast errors are more appropriate criteria to evaluate the predictive power and to finalize the best approach. In general, the most popular measures are MAE and RMSE. Hence, we compare the forecasting performance of ML techniques using these two measures in our study. Their mathematical expressions are given by

    MAE=mean(|Ft^Ft|),

    and

    RMSE=mean(Ft^Ft)2,

    respectively.

    This subsection is further divided into two parts. In the first part, we deal with the mortality rates of the patients infected by the COVID-19 pandemic in Mexico. In the second part, we deal with the death rates of the patients infected by the COVID-19 pandemic in Holland.

    From Figure 8, it can be observed that the entire trajectory of the mortality rate has experienced many ups and downs in the last few months, but the trend of data is decreasing over time. The mortality rate series is plotted in Figure 8, where the vertical blue dotted line splits the estimation and post-sample forecasting periods. The histogram plot and box plot are also provided in Figure 8, which reveal that the underlying time series is right skewed.

    Figure 8.  A virtual display of the mortality rate data in Mexico.

    The two statistical accuracy measures for the Mexico data set are given in Table 7. The MAE and RMSE are calculated for ML algorithms such as SVR, RF, and NNAR. It is inferred that the RF outperformed the other competitor counterparts. For the RF method, the RMSE and MAE values are given by 0.066 and 0.039, respectively. Whereas, for the SVR, the values of the RMSE and MAE are given by 0.073 and 0.043, respectively. On the other hand, the RMSE and MAE values for the NNAR are, respectively, given by 0.198 and 0.149. From the values of the RMSE and MAE for the NNAR approach, it is clear that the values of NNAR are higher than the values of the RMSE and MAE computed for RF and SVR.

    Table 7.  The error metrics.
    Criteria SVR RF NNAR
    RMSE 0.073 0.066 0.198
    MAE 0.043 0.039 0.149

     | Show Table
    DownLoad: CSV

    Furthermore, the visual illustration of forecast errors is porvided in Figure 9. The plots in Figure 9 show that the ML algorithms, specifically, the RF remained an efficient tool in forecasting the mortality rates of COVID-19 patients.

    Figure 9.  The schematic representation of forecast errors for the mortality rate data in Mexico.

    We also plot the prediction curves for COVID-19 deaths under the three machine learning algorithms to get a more intuitive picture of the prediction accuracy and results. In this regard, the line chart has been constructed, for the representation of predicted and actual values; see Figure 10. Some predicted values of the NNAR approach are very close, but few are substantially far away from the actual data. On the other hand, SVR prediction is highly stable over time and therefore beat the rival algorithms in predictive modeling.

    Figure 10.  Forecasting performance of ML algorithms for the mortality rate data in Mexico.

    Here, we estimate and predict the daily death data of COVID-19 for Holland. It can be observed from Figure 11 that the entire trajectory of mortality rate has experienced numerous episodes in several months, but the times series is declining over time. The mortality rate series is plotted in Figure 11, where the vertical blue dotted line represents the estimation and post-sample forecasting periods. The histogram plot and box plot are also presented in Figure 10, which demonstrates that the underlying series is right skewed.

    Figure 11.  A virtual display of the mortality rate data in Holland.

    The two considered statistical accuracy measures for the Holland data set are reported in Table 8. The MAE and RMSE are computed for ML algorithms, namely SVR, RF, and NNAR. From Table 8, we can observe that the SVR showed superior forecast performance as compared to the rival counterparts. For the SVR method, the RMSE and MAE values are 0.16 and 0.118, respectively. On the other hand, for the RF approach, these values are given by 0.191 and 0.139, respectively. Whereas, the forecast errors (RMSE and MAE) of NNAR are given by 0.444 and 0.398, respectively. From the above discussion, it is obvious that the forecast errors of the NNAR approach are substantially higher than the forecast errors of RF and SVR.

    Table 8.  The error metrics.
    Criteria SVR RF NNAR
    RMSE 0.160 0.191 0.444
    MAE 0.118 0.139 0.398

     | Show Table
    DownLoad: CSV

    The graphical comparison of forecast errors is also depicted in Figure 12. It manifests that the ML algorithms, specifically SVR remained an effective tool in forecasting the post-sample trajectory of the mortality rate of COVID-19 patients.

    Figure 12.  The schematic representation of forecast errors for the mortality rate data in Holland.

    We portray the prediction curves for COVID-19 deaths using these three ML algorithms to get a more clear picture of the models performances. In this regard, we use the line chart for the representation of forecasted and observed data; see Figure 13. From the plots in Figure 13, it can be seen that the observed test series is highly volatile and noisy. Despite this volatility, SVR and RF have shown good results, particularly the RF performance is highly satisfactory.

    Figure 13.  Forecasting Performance of ML algorithms for the mortality rate data in Holland.

    The efforts in this paper added another useful approach to the literature on statistical methodologies by introducing a new family of distributions. The new family was named a NEExp family of distributions. Based on a NEExp family, an updated version of the Weibull model called, a NEExp-Weibull model was studied. The MLEs of the NEExp-Weibull model were obtained. The evaluation of the MLEs of the NEExp-Weibull distribution was carried out through a brief SiSt. The usefulness of the NEExp-Weibull model was shown by analyzing two data sets taken from the healthcare sector. The first data set was representing the mortality rate of COVID-19 patients in Mexico. Whereas, the second data was also related to the COVID-19 events taken from Holland. Using these two COVID-19 data sets, the NEExp-Weibull distribution was compared with the Weibull and three other well-known models such as the L-Weibull, NEP-Weibull, and NM-Weibull distributions. Based on four well-known comparative tools, it is observed that the NEExp-Weibull distribution was the best competitive model as compared to the Weibull and other well-known modified forms of the Weibull distribution. Therefore, based on the numerical results and findings of this study, it is observed that the NEExp-Weibull distribution may be the best suitable choice to use for analyzing the medical and other related data sets. Besides the statistical modeling, for prediction purposes, we further implemented three ML methods including SVR, RF, and NNAR using the same data sets. To compare their forecasting performances, two well-known statistical accuracy quantities such as the RMSE and MAE were computed. We found that the RF algorithm was very efficient in forecasting using the first data. However, for the second data set, the SVR showed superior performance in contrast to other methods.

    Besides the certain advantages of the NEExp-Weibull distribution over the Weibull and other competitive distributions, the NEExp-Weibull distribution has also some certain limitations, for example

    ● The proposed NEExp-Weibull model is a continuous probability distribution, and it is employed to analyze the mortality rates of COVID-19 patients. Therefore, the NEExp-Weibull model could not be implemented to analyze other forms of the COVID-19 data that are discrete in nature, for example, (i) the number of deaths, (ii) the number of confirmed cases, or (iii) the number of recovered cases, etc.

    ● Due to the introduction of the additional parameter, the NEExp-Weibull distribution has a complicated form of its PDF. Therefore, the expressions for the estimators of its parameters are not in explicit forms. Therefore, computer software must be used to obtain the estimated values of the parameters.

    ● Since, the PDF of the NEExp family has a complicated form, therefore, more computational efforts are needed to derive the key mathematical properties.

    In the future, we are motivated to obtain the discrete version of the proposed NEExp-Weibull distribution to counter the discrete data sets. In this work, we only used the maximum likelihood estimation method to estimate the parameters of the NEExp-Weibull distribution. In the future, we are intended to estimate the parameters of the NEExp-Weibull distribution using other classical methods such as ordinary least square, weighted ordinary least square, maximum product spacing methods, etc. Neutrosophic statistics is a generalization of classical statistics and is implemented when the data sets are generated from a complex process. In the future, we are also motivated to study the neutrosophic extension of the NEExp-Weibull distribution.



    [1] B. B. Mandelbrot, The Fractal Geometry of Nature, New York: WH freeman, 1983.
    [2] M. F. Barnsley, Fractals Everywhere, Academic press, 2014.
    [3] C. Cattani, Fractals and hidden symmetries in DNA, Math. Probl. Eng., 2010, 2010.
    [4] S. Kumari, R. Chugh, J. Cao, et al. Multi fractals of generalized multivalued iterated function systems in b-metric spaces with applications, Math., 7 (2019), 967.
    [5] M. S. Tavazoei, M. Haeri, An optimization algorithm based on chaotic behavior and fractal nature, J. Comput. Appl. Math., 206 (2007), 1070-1081. doi: 10.1016/j.cam.2006.09.008
    [6] E. Nakaguchi, M. Efendiev, On a new dimension estimate of the global attractor for chemotaxisgrowth systems, Osaka J. Math., 45 (2008), 273-281.
    [7] M. Efendiev, S. Zelik, Finite- and infinite-dimensional attractors for porous media equations, P. Lond. Math. Soc., 96 (2008), 51-77. doi: 10.1112/plms/pdm026
    [8] I. Chitescu, H. Georgescu, R.Miculescu, Approximation of infinite dimensional fractals generated by integral equations, J. Comput. Appl. Math., 234 (2010), 1417-1425. doi: 10.1016/j.cam.2010.02.017
    [9] S. Ree, L. E. Reichl, Fractal analysis of chaotic classical scattering in a cut-circle billiard with two openings, Phys. Rev. E, 65 (2002), 055205.
    [10] E. de Amo, I. Chitescu, M. D. Carrillo, et al. A new approximation procedure for fractals, J. Comput. Appl. Math., 151 (2003), 355-370. doi: 10.1016/S0377-0427(02)00752-5
    [11] L. Nottale, J. Schneider, Fractals and nonstandard analysis, J. Math. Phys., 25 (1984), 1296-1300. doi: 10.1063/1.526285
    [12] M. Czachor, Waves along fractal coastlines: From fractal arithmetic to wave equations, Acta Phys. Pol. B, 50 (2019), 813-831. doi: 10.5506/APhysPolB.50.813
    [13] M. N. Célérier, L. Nottale, Quantum-classical transition in scale relativity, J. Phys. A: Math. Gen., 37 (2004), 931.
    [14] K. Falconer, Fractal Geometry: Mathematical Foundations and Applications, John Wiley Sons, 2004.
    [15] K. Falconer, Techniques in Fractal Geometry, Chichester (W. Sx.): Wiley, 1997.
    [16] G. Edgar, Measure, Topology, and Fractal Geometry, Springer Science Business Media, 2007.
    [17] J. Kigami, Analysis on Fractals, Cambridge University Press, 2001.
    [18] F. H. Stillinger, Axiomatic Basis for Spaces with Noninteger Dimension, J. Math. Phys., 18 (1977), 1224-1234. doi: 10.1063/1.523395
    [19] V. E. Tarasov, Fractional Dynamics: Applications of Fractional Calculus to Dynamics of Particles, Fields and Media, Springer Science Business Media, 2011.
    [20] M. Zubair, M. J. Mughal, Q. A. Naqvi, Electromagnetic Fields and Waves in Fractional Dimensional Space, Springer Science Business Media, 2012.
    [21] W. Chen Y. Liang, New methodologies in fractional and fractal derivatives modeling, Chaos Soliton. Fract., 102 (2017), 72-77. doi: 10.1016/j.chaos.2017.03.066
    [22] Y. Liang, Q. Y. Allen, W. Chen, et al. A fractal derivative model for the characterization of anomalous diffusion in magnetic resonance imaging, Commun. Nonlinear Sci., 39 (2016), 529-537. doi: 10.1016/j.cnsns.2016.04.006
    [23] H. Richard, Fractional Calculus: an Introduction for Physicists, World Scientific, 2014.
    [24] S. Das, Functional Fractional Calculus, Springer Science Business Media, 2011.
    [25] C. Song, S. Fei, J. Cao, et al. Robust synchronization of fractional-order uncertain chaotic systems based on output feedback sliding mode control, Math., 7 (2019), 599.
    [26] G. Rajchakit, A. Pratap, R. Raja, et al. Hybrid control scheme for projective lag synchronization of Riemann-Liouville sense fractional order memristive BAM neuralnetworks with mixed delays, Math., 7 (2019), 759.
    [27] Y. Wei, L. Yin, X. Long, The coupling integrable couplings of the generalized coupled Burgers equation hierarchy and its Hamiltonian structure, Adv. Differ. Equ., 2019 (2019), 1-17. doi: 10.1186/s13662-018-1939-6
    [28] X. Li, Z. Liu, J. Li, et al. Existence and controllability for nonlinear fractional control systems with damping in Hilbert spaces, Acta Math. Sci., 39 (2019), 229-242. doi: 10.1007/s10473-019-0118-5
    [29] X. Li, Y. Li, Z. Liu, et al. Sensitivity analysis for optimal control problems described by nonlinear fractional evolution inclusions, Fract. Calc. Appl. Anal., 21 (2018), 1439-1470. doi: 10.1515/fca-2018-0076
    [30] K. M. Kolwankar, A. D. Gangal, Fractional differentiability of nowhere differentiable functions and dimensions, Chaos, 6 (1996), 505-513. doi: 10.1063/1.166197
    [31] K. M. Kolwankar, A. D. Gangal, Local fractional Fokker-Planck equation, Phys. Rev. Lett., 80 (1998), 214.
    [32] A. Parvate, A. D. Gangal, Calculus on fractal subsets of real line-I: Formulation, Fract., 17 (2009), 53-148. doi: 10.1142/S0218348X09004181
    [33] A. Parvate, A. D. Gangal, Calculus on fractal subsets of real line-II: Conjugacy with ordinary calculus, Fract., 19 (2011), 271-290. doi: 10.1142/S0218348X11005440
    [34] A. Parvate, S. Satin, A. D. Gangal, Calculus on fractal curves in Rn, Fract., 19 (2011), 15-27. doi: 10.1142/S0218348X1100518X
    [35] A. K. Golmankhaneh, A. Fernandez, A. K. Golmankhaneh, et al. Diffusion on middle-ξ Cantor sets, Entropy, 20 (2018), 1-13.
    [36] A. K. Golmankhaneh, A. S. Balankin, Sub-and super-diffusion on Cantor sets: Beyond the paradox, Phys. Lett. A, 382 (2018), 960-967. doi: 10.1016/j.physleta.2018.02.009
    [37] A. K. Golmankhaneh, U. Branch, Quantum mechanics on the fractal time-space, In: Proceedings of the 8th International Conference on Fractional Differentiation and its Applications, 2016, 677-687.
    [38] A. K. Golmankhaneh, C. Tunç, Sumudu transform in fractal calculus, Appl. Math. Comput., 350 (2019), 386-401.
    [39] A. K. Golmankhaneh, C. Tunç, On the Lipschitz condition in the fractal calculus, Chaos, Soliton Fract., 95 (2017), 140-147. doi: 10.1016/j.chaos.2016.12.001
    [40] C. Tunç, S. A. Mohammed, On the asymptotic analysis of bounded solutions to nonlinear differential equations of second order, Adv. Differ. Equ., 2019 (2019), 1-19. doi: 10.1186/s13662-018-1939-6
    [41] G. C. Wu, D. Baleanu, W. H. Luo, Lyapunov functions for Riemann-Liouville-like fractional difference equations, Appl. Math. Comput., 314 (2017), 228-236.
    [42] M. Rivero, S. V. Rogosin, J. A. T. Machado, et al. Stability of fractional order systems, Math. Probl. Eng., 2013 (2013).
    [43] R. Agarwal, S. Hristova, D. O'Regan, A survey of Lyapunov functions, stability and impulsive Caputo fractional differential equations, Fract. Calc. Appl. Anal., 19 (2016), 290-318.
    [44] A. Q. M. Khaliq, X. Liang, K. M. Furati, A fourth-order implicit-explicit scheme for the space fractional nonlinear Schrödinger equations, Numer. Algorithms, 75 (2016), 147-172.
    [45] C. Tunç, Uniformly stability and boundedness of solutions of second order nonlinear delay differential equations, Appl. Comput. Math., 10 (2011), 449-462.
    [46] C. Tunç, E. Tunç, On the asymptotic behavior of solutions of certain second-order differential equations, J. Franklin I., 344 (2007), 391-398. doi: 10.1016/j.jfranklin.2006.02.011
    [47] T. Yoshizawa, Stability Theory by Liapunov's Second Method, 1966.
    [48] T. Hara, On the asymptotic behavior of the solutions of some third and fourth order nonautonomous differential equations, Publ. Res. I. Math. Sci., 9 (1974), 649-673.
    [49] R. DiMartino, W. Urbina, On Cantor-Like Sets and Cantor-Lebesgue Singular Functions, arXiv preprint arXiv:1403.6554, 2014.
    [50] G. Braden, Fractal Time: The Secret of 2012 and a New World Age, Hay House Inc, 2010.
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