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Research article Special Issues

Analytical insight into fractional Fornberg-Whitham equations using novel transform methods

  • Received: 10 February 2025 Revised: 27 March 2025 Accepted: 29 March 2025 Published: 09 April 2025
  • MSC : 34G20, 35A20, 35A22, 35R11

  • This work addressed one of the most essential evolutionary equations that was widely used in describing various nonlinear wave propagation and dispersive phenomena in various scientific and engineering applications, which was called the nonlinear fractional Fornberg-Whitham (FFW). Due to the importance of this equation, we examined it by employing two highly effective techniques: the residual power series method (RPSM) and the new iterative approach (NIM), both distinguished by their efficacy in solving more complicated nonlinear fractional evolutionary equations. Moreover, we integrated the Elzaki transform with both approaches to create Elzaki RPSM (ERPSM) and Elzaki NIM (ENIM) to ease the calculations. The ERPSM effectively combined the power series approach with residual error analysis to generate highly accurate series solutions, while ENIM provided alternative frameworks for handling nonlinearities and achieving rapid convergence. Comparative studies of the obtained solutions highlighted these methods' efficiency, accuracy, and reliability in solving fractional-order differential equations. The results underscored the potential of these analytical techniques for modeling and solving complex fractional wave equations, contributing to the advancement of mathematical physics and computational fluid dynamics.

    Citation: Safyan Mukhtar, Wedad Albalawi, Faisal Haroon, Samir A. El-Tantawy. Analytical insight into fractional Fornberg-Whitham equations using novel transform methods[J]. AIMS Mathematics, 2025, 10(4): 8165-8190. doi: 10.3934/math.2025375

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  • This work addressed one of the most essential evolutionary equations that was widely used in describing various nonlinear wave propagation and dispersive phenomena in various scientific and engineering applications, which was called the nonlinear fractional Fornberg-Whitham (FFW). Due to the importance of this equation, we examined it by employing two highly effective techniques: the residual power series method (RPSM) and the new iterative approach (NIM), both distinguished by their efficacy in solving more complicated nonlinear fractional evolutionary equations. Moreover, we integrated the Elzaki transform with both approaches to create Elzaki RPSM (ERPSM) and Elzaki NIM (ENIM) to ease the calculations. The ERPSM effectively combined the power series approach with residual error analysis to generate highly accurate series solutions, while ENIM provided alternative frameworks for handling nonlinearities and achieving rapid convergence. Comparative studies of the obtained solutions highlighted these methods' efficiency, accuracy, and reliability in solving fractional-order differential equations. The results underscored the potential of these analytical techniques for modeling and solving complex fractional wave equations, contributing to the advancement of mathematical physics and computational fluid dynamics.



    Let {X,Xn;n1} be a sequence of independent and identically distributed (i.i.d.) random variables. Complete convergence first established by Hsu and Robbins [1] (for the sufficiency) and Erdős [2,3] (for the necessity) proceeds as follows:

    n=1P(|Sn|ϵn)<,foranyϵ>0,

    if and only if EX=0 and EX2<. Baum and Katz [4] extended the above result and obtained the following theorem:

    n=1nr/p2P(|Sn|ϵn1/p)<,for0<p<2,rp,anyϵ>0, (1.1)

    if and only if E|X|r<, and when r1, EX=0.

    There are several extensions of the research on complete convergence. One of them is the study of the convergence rate of complete convergence. The first work was the convergence rate, achieved by Heyde [5]. He got the result of limϵ0ϵ2n=1P(|Sn|ϵn)=EX2 under the conditions EX=0 and EX2<. For more results on the convergence rate, see Chen [6], Sp˘ataru [7], Gut and Sp˘ataru [8], Sp˘atarut and Gut [9], Gut and Steinebach [10], He and Xie [11], Kong and Dai [12], etc.

    But (1.1) does not hold for p=2. However, by replacing n1/p by nlnn and nlnlnn, Gut and Sp˘ataru [8] and Sp˘atarut and Gut [9] established the following results called the convergence rate of the law of the (iterated) logarithm. Supposing that {X,Xn;n1} is a sequence of i.i.d. random variables with EX=0 and EX2=σ2<, Gut and Sp˘ataru [8] and Sp˘atarut and Gut [9] obtained the following results respectively:

    limϵ0ϵ2+2δn=1lnδnnP(|Sn|ϵnlnn)=E|N|2+2δσ2+2δδ+1,0δ1, (1.2)

    where N is the standard normal distribution, and

    limϵ0ϵ2n=31nlnnP(|Sn|ϵnlnlnn)=σ2. (1.3)

    Motivated by the above results, the purpose of this paper is to extend (1.2) and (1.3) to sub-linear expectation space (to be introduced in Section 2), which was introduced by Peng [13,14], and to study the necessary conditions of (1.2).

    Under the theoretical framework of the traditional probability space, in order to infer the model, all statistical models must assume that the error (and thus the response variable) is subject to a certain uniquely determined probability distribution, that is, the distribution of the model is deterministic. Classical statistical modeling and statistical inference are based on such distribution certainty or model certainty. "Distribution certainty" modeling has yielded a set of mature theories and methods. However, the real complex data in economic, financial and other fields often have essential and non negligible probability and distribution uncertainty. The probability distribution of the response variable to be studied is uncertain and does not meet the assumptions of classical statistical modeling. Therefore, classical probability statistical modeling methods cannot be used for this type of data modeling. Driven by uncertainty issues, Peng [14,15] established a theoretical framework for sub-linear expectation spaces from the perspective of expectations. Sub-linear expectation has a wide range of application backgrounds and prospects. In recent years, a series of research achievements on limit theory in sub-linear expectation spaces has been established. See Peng [14,15], Zhang [16,17,18], Hu [19], Wu and Jiang [20,21], Wu et al. [22], Wu and Lu [23], etc. Wu [24], Liu and Zhang [25], Ding [26] and Liu and Zhang [27] obtained the convergence rate for complete moment convergence. However, the convergence rate results for the (iterative) logarithmic law have not been reported yet. The main difficulty in studying it is that the sub-linear expectation and capacity are not additive, which makes many traditional probability space tools and methods no longer effective; thus, it is much more complex and difficult to study it.

    In Section 2, we will provide the relevant definitions of sub-linear expectation space, the basic properties and the lemmas that need to be used in this paper.

    Let (Ω,F) be a measurable space and let H be a linear space of random variables on (Ω,F) such that if X1,,XnH then φ(X1,,Xn)H for each φCl,Lip(Rn), where Cl,Lip(Rn) denotes the set of local Lipschitz functions on Rn. In this case, for XH, X is called a random variable.

    Definition 2.1. A sub-linear expectation ˆE on H is a function: HR satisfying the following for all X,YH:

    (a) Monotonicity: If XY then ˆEXˆEY;

    (b) Constant preservation: ˆEc=c;

    (c) Sub-additivity: ˆE(X+Y)ˆEX+ˆEY;

    (d) Positive homogeneity: ˆE(λX)=λˆEX,λ0.

    The triple (Ω,H,ˆE) is called a sub-linear expectation space. The conjugate expectation ˆε of ˆE is defined by

    ˆεX:=ˆE(X),XH.

    Let GF. A function V:G[0,1] is called a capacity if

    V()=0,V(Ω)=1andV(A)V(B)forAB,A,BG.

    The upper and lower capacities (V,ν) corresponding to (Ω,H,ˆE) are respectively defined as

    V(A):=inf{ˆEξ;I(A)ξ,ξH},ν(A):=1V(Ac),AF,Ac:=ΩA.

    The Choquet integrals is defined by

    CV(X):=0V(X>x)dx+0(V(X>x)1)dx.

    From all of the definitions above, it is easy to obtain the following Proposition 2.1.

    Proposition 2.1. Let X,YH and A,BF.

    (i) ˆεXˆEX,ˆE(X+a)=ˆEX+a,aR;

    (ii) |ˆE(XY)|ˆE|XY|,ˆE(XY)ˆEXˆEY;

    (iii) ν(A)V(A),V(AB)V(A)+V(B),ν(AB)ν(A)+V(B);

    (iv) If fI(A)g,f,gH, then

    ˆEfV(A)ˆEg,ˆεfν(A)ˆεg. (2.1)

    (v)(Lemma 4.5 (iii) in Zhang [16]) For any c>0,

    ˆE(|X|c)c0V(|X|>x)dxCV(|X|), (2.2)

    where, here and hereafter, ab:=min(a,b), and ab:=max(a,b) for any a,bR.

    (vi)Markov inequality: V(|X|x)ˆE(|X|p)/xp,x>0,p>0;

    Jensen inequality: (ˆE(|X|r))1/r(ˆE(|X|s))1/sfor0<rs.

    Definition 2.2. (Peng [14,15])

    (ⅰ) (Identical distribution) Let X1 and X2 be two random variables on (Ω,H,ˆE). They are called identically distributed, denoted by X1d=X2, if

    ˆE(φ(X1))=ˆE(φ(X2)),forallφCl,Lip(Rn).

    A sequence {Xn;n1} of random variables is said to be identically distributed if for each i1, Xid=X1.

    (ⅱ) (Independence) In a sub-linear expectation space (Ω,H,ˆE), a random vector Y=(Y1,,Yn), YiH is said to be independent of another random vector X=(X1,,Xm),XiH under ˆE if for each φCl,Lip(Rm×Rn), there is ˆE(φ(X,Y))=ˆE[ˆE(φ(x,Y))|x=X].

    (ⅲ) (Independent and identically distributed) A sequence {Xn;n1} of random variables is said to be i.i.d., if Xi+1 is independent of (X1,,Xi) and Xid=X1 for each i1.

    From Definition 2.2 (ⅱ), it can be verified that if Y is independent of X, and X0,ˆEY0, then ˆE(XY)=ˆE(X)ˆE(Y). Further, if Y is independent of X and X,Y0, then

    ˆE(XY)=ˆE(X)ˆE(Y),ˆε(XY)=ˆε(X)ˆε(Y). (2.3)

    For convenience, in all subsequent parts of this article, let {X,Xn;n1} be a sequence of random variables in (Ω,H,ˆE), and Sn=ni=1Xi. For any XH and c>0, set X(c):=(c)Xc. The symbol c represents a positive constant that does not depend on n. Let axbx denote limxax/bx=1, axbx denote that there exists a constant c>0 such that axcbx for sufficiently large x, [x] denote the largest integer not exceeding x, and I() denote an indicator function.

    To prove the main results of this article, the following three lemmas are required.

    Lemma 2.1. (Theorem 3.1 (a) and Corollary 3.2 (b) in Zhang [16]) Let {Xk;k1} be a sequence of independent random variables in (Ω,H,ˆE).

    (i) If ˆEXk0, then for any x,y>0,

    V(Snx)V(max1knXk>y)+exp(x22(xy+Bn){1+23ln(1+xyBn)});

    (ii) If ˆεXk0, then there exists a constant c>0 such that for any x>0,

    ν(Snx)cBnx2,

    where Bn=nk=1ˆEX2k.

    Here we give the notations of a G-normal distribution which was introduced by Peng [14].

    Definition 2.3. (G-normal random variable) For 0σ_2ˉσ2<, a random variable ξ in (Ω,H,ˆE) is called a G-normal N(0,[σ_2,ˉσ2]) distributed random variable (write ξN(0,[σ_2,ˉσ2]) under ˆE), if for any φCl,Lip(R), the function u(x,t)=ˆE(φ(x+tξ)) (xR,t0) is the unique viscosity solution of the following heat equation:

    tuG(2xxu)=0,u(0,x)=φ(x),

    where G(α)=(ˉσ2α+σ_2α)/2.

    From Peng [14], if ξN(0,[σ_2,ˉσ2]) under ˆE, then for each convex function φ,

    ˆE(φ(ξ))=12πφ(ˉσx)ex2/2dx. (2.4)

    If σ=ˉσ=σ_, then N(0,[σ_2,ˉσ2])=N(0,σ2) which is a classical normal distribution.

    In particular, notice that φ(x)=|x|p,p1 is a convex function, taking φ(x)=|x|p,p1 in (2.4), we get

    ˆE(|ξ|p)=2ˉσp2π0xpex2/2dx<. (2.5)

    Equation (2.5) implies that

    CV(|ξ|p)=0V(|ξ|p>x)dx1+1ˆE(|ξ|2p)x2dx<,foranyp1/2.

    Lemma 2.2. (Theorem 4.2 in Zhang [17], Corollary 2.1 in Zhang [18]) Let {X,Xn;n1} be a sequence of i.i.d. random variables in (Ω,H,ˆE). Suppose that

    (i)limcˆE(X2c) is finite;

    (ii)x2V(|X|x)0 as x;

    (iii)limcˆE(X(c))=limcˆE((X)(c))=0.

    Then for any bounded continuous function φ,

    limnˆE(φ(Snn))=ˆE(φ(ξ)),

    and if F(x):=V(|ξ|x), then

    limnV(|Sn|>xn)=F(x),ifxisacontinuouspointofF, (2.6)

    where ξN(0,[σ_2,ˉσ2]) under ˆE, ˉσ2=limcˆE(X2c) and σ_2=limcˆε(X2c).

    Lemma 2.3. (Lemma 2.1 in Zhang [17]) Let {Xn;n1} be a sequence of independent random variables in (Ω,H,ˆE), and 0<α<1 be a real number. If there exist real constants βn,k such that

    V(|SnSk|βn,k+ϵ)α,forallϵ>0kn,

    then

    (1α)V(maxkn(|Sk|βn,k)>x+ϵ)V(|Sn|>x),forallx>0,ϵ>0.

    The results of this article are as follows.

    Theorem 3.1. Let {X,Xn;n1} be a sequence of i.i.d. random variables in (Ω,H,ˆE). Suppose that

    CV(X2)<,limcˆE(X(c))=limcˆE((X)(c))=0. (3.1)

    Then for 0δ1,

    limϵ0ϵ2+2δn=2lnδnnV(|Sn|ϵnlnn)=CV(|ξ|2δ+2)δ+1, (3.2)

    where, here and hereafter, ξN(0,[σ_2,ˉσ2]) under ˆE, ˉσ2=limcˆE(X2c) and σ_2=limcˆε(X2c).

    Conversely, if (3.2) holds for δ=1, then (3.1) holds.

    Theorem 3.2. Under the conditions of Theorem 3.1,

    limϵ0ϵ2n=31nlnnV(|Sn|ϵnlnlnn)=CV(ξ2). (3.3)

    Remark 3.1. Theorems 3.1 and 3.2 not only extend Theorem 3 in [8] and Theorem 2 in [9], respectively, from the probability space to sub-linear expectation space, but they also study and obtain necessary conditions for Theorem 3.1.

    Remark 3.2. Under the condition limcˆE(|X|c)+=0 (limcˆE(X2c)+=0limcˆE(|X|c)+=0), it is easy to verify that ˆE(±X)=limcˆE((±X)(c)). So, Corollary 3.9 in Ding [26] has two more conditions than Theorem 3.2: ˆE is continuous and limcˆE(X2c)+=0. Therefore, Corollary 3.9 in Ding [26] and Theorem 3.2 cannot be inferred from each other.

    Proof of the direct part of Theorem 3.1.. Note that

    ϵ2+2δn=2lnδnnV(|Sn|ϵnlnn)=ϵ2+2δn=2lnδnnV(|ξ|ϵlnn)+ϵ2+2δn=2lnδnn(V(|Sn|ϵnlnn)V(|ξ|ϵlnn)):=I1(ϵ)+I2(ϵ).

    Hence, in order to establish (3.2), it suffices to prove that

    limϵ0I1(ϵ)=CV(|ξ|2δ+2)δ+1 (3.4)

    and

    limϵ0I2(ϵ)=0. (3.5)

    Given that lnδnn and V(|ξ|εlnn) is monotonically decreasing with respect to n, it holds that

    I1(ϵ)=ϵ2+2δn=2lnδnnV(|ξ|ϵlnn)=ϵ2+2δlnδ22V(|ξ|ϵln2)+ϵ2+2δn=3nn1lnδnnV(|ξ|ϵlnn)dxϵ2+2δlnδ22+ϵ2+2δn=3nn1lnδxxV(|ξ|ϵlnx)dx=ϵ2+2δlnδ22+ϵ2+2δ2lnδxxV(|ξ|ϵlnx)dx,

    and

    I1(ϵ)=ϵ2+2δn=2lnδnnV(|ξ|ϵlnn)=ϵ2+2δn=2n+1nlnδnnV(|ξ|ϵlnn)dxϵ2+2δn=2n+1nlnδxxV(|ξ|ϵlnx)dx=ϵ2+2δ2lnδxxV(|ξ|ϵlnx)dx.

    Therefore, (3.4) follows from

    limϵ0I1(ϵ)=limϵ0ϵ2+2δ2lnδxxV(|ξ|ϵlnx)dx=limϵ0εln22y2δ+1V(|ξ|y)dy(lety=εlnx)=02y2δ+1V(|ξ|y)dy=CV(|ξ|2+2δ)δ+1.

    Let M40; write AM,ϵ:=exp(Mϵ2).

    |I2(ϵ)|ϵ2+2δ2n[AM,ϵ]lnδnn|V(|Sn|nϵlnn)V(|ξ|ϵlnn)|+ϵ2+2δn>[AM,ϵ]lnδnnV(|Sn|ϵnlnn)+ϵ2+2δn>[AM,ϵ]lnδnnV(|ξ|ϵlnn):=I21(ϵ)+I22(ϵ)+I23(ϵ). (3.6)

    Let us first estimate I21(ϵ). For any β>ϵ2,

    I21(ϵ)ϵ2+2δAM,ϵ2lnδxx|V(|S[x]|[x]ϵlnx)V(|ξ|ϵlnx)|dxϵ2+2δAβ,ϵ22lnδxxdx+ϵ2+2δAM,ϵAβ,ϵlnδxxsupnAβ,ϵ|V(|Sn|nϵlnx)V(|ξ|ϵlnx)|dx2β1+δ+M02y1+2δsupnAβ,ϵ|V(|Sn|ny)F(y)|dy. (3.7)

    By (2.2), ˆE(X2c)c0V(X2x)dx; also, notice that V(X2x) is a decreasing function of x. So, CV(X2)=0V(X2x)dx< implies that limcˆE(X2c) is finite and limxx2V(|X|x)=limxxV(X2x)=0. Therefore, (3.1) implies the conditions of Lemma 2.2. From (2.6),

    limϵ0supnAβ,ϵ|V(|Sn|ny)F(y)|=0,ifyisacontinuouspointofF. (3.8)

    Note that F(y) is a monotonically decreasing function, so its discontinuous points are countable. Hence (3.8) holds for each y, except on a set with the null Lebesgue measure. Combining y2δ+1supnAβ,ϵ|V(|Sn|ny)F(y)|2Mδ+1/2 for any 0yM, by the Lebesgue bounded convergence theorem, (3.8) leads to the following:

    limϵ0M0y2δ+1supnAβ,ϵ|V(|Sn|ny)F(y)|dy=0. (3.9)

    Let ϵ0 first, then let β0; from (3.7) and (3.9), we get

    limϵ0I21(ϵ)=0. (3.10)

    Next, we estimate that I22(ϵ). For 0<μ<1, let φμ(x)Cl,Lip(R) be an even function such that 0φμ(x)1 for all x and φμ(x)=0 if |x|μ and φμ(x)=1 if |x|>1. Then

    I(|x|1)φμ(x)I(|x|μ). (3.11)

    Given (2.1) and (3.11), and that X,Xi are identically distributed, for any x>0 and 0<μ<1, we get

    V(|Xi|x)ˆE[φμ(Xix)]=ˆE[φμ(Xx)]V(|X|μx). (3.12)

    Without loss of generality, we assume that ˉσ=1. For nexp(Mϵ2)exp(40ϵ2), set bn:=ϵnlnn/20; from Proposition 2.1 (ii) and the condition that limcˆE(X(c))=0,

    ni=1|ˆEX(bn)i|=n|limcˆE(X(c))ˆEX(bn)|nlimcˆE|X(c)X(bn)|=nlimcˆE(|X|cbn)+nlimcˆE(|X|c)2bn=nˉσ2bn=20nϵlnnϵ2nlnn,forM40,nexp(Mϵ2).

    Using Lemma 2.1 for {X(bn)iˆEX(bn)i;1in}, and taking x=ϵnlnn/2 and y=2bn=ϵnlnn/10 in Lemma 2.1 (ⅰ), by Proposition 2.1 (ⅰ), ˆE(X(bn)iˆEX(bn)i)=0, and noting that |X(bn)iˆEX(bn)i|y, Bn=ni=1ˆE(X(bn)iˆEX(bn)i)24nˆE(X(bn)i)24n; combining this with (3.12) we get

    V(Snϵnlnn)V(ni=1(X(bn)iˆEX(bn)i)ϵnlnn/2)+ni=1V(|Xi|bn)exp(ϵ2nlnn4(ϵ2nlnn/20+4n){1+23lnϵ2nlnn80n})+nV(|X|μbn)c(ϵ2lnn)3+nV(|X|μϵnlnn/20)

    from ϵ2nlnn4(ϵ2nlnn/20+4n){1+23ln(1+ϵ2lnn80)}3ln(ϵ2lnn80).

    Since {X,Xi} also satisfies the (3.1), we can replace the {X,Xi} with {X,Xi} in the upper form

    V(Snϵnlnn)c(ϵ2lnn)3+nV(|X|μϵnlnn/20).

    Therefore

    V(|Sn|ϵnlnn)(ϵ2lnn)3+nV(|X|cϵnlnn).

    This implies the following from Markov's inequality and (2.5),

    I22(ϵ)+I23(ϵ)ϵ2+2δnAM,ϵlnδnn(nV(|X|cϵnlnn)+1ϵ6ln3n+ˆE|ξ|6ϵ6ln3n)ϵ2+2δAM,ϵlnδxV(|X|cϵxlnx)dx+cϵ4+2δAM,ϵdxxln3δxϵ2+2δMϵ12δyln1δyV(|X|cϵy)dy+cM2+δϵ2+2δMϵ1yV(|X|ϵy)dy+M2+δϵ2δ0zV(|X|z)dz+M2+δ=ϵ2δCV(X2)/2+M2+δ.

    Let ϵ0 first, then let M; we get

    limϵ0(I22(ϵ)+I23(ϵ))=0.

    Combining this with (3.10) and (3.6), (3.5) is established.

    Proof of the converse part of Theorem 3.1. If (3.2) holds for δ=1, then

    n=2lnnnV(|Sn|ϵnlnn)<foranyϵ>0. (3.13)

    Take ξ as defined by Lemma 2.2 (ˆE|ξ|< from (2.5)) and the bounded continuous function ψ such that I(x>qˆE|ξ|+1)ψ(x)I(x>qˆE|ξ|) for any fixed q>0. Therefore, for any ϵ>0,q>0 and nexp(qˆE|ξ|+1ϵ)2, according to (2.1), Lemma 2.2 and the Markov inequality, one has

    V(|Sn|ϵnlnn)V(|Sn|(qˆE|ξ|+1)n)ˆE(ψ(|Sn|n))ˆE(ψ(|ξ|))V(|ξ|>qˆE|ξ|)ˆE|ξ|qˆE|ξ|=1q.

    From the arbitrariness of q, letting q, we get the following for any ϵ>0,

    V(|Sn|ϵnlnn)0,n. (3.14)

    So, there is an n0 such that V(|Sn|ϵnlnn)<1/4 for nn0. Now for n2n0, if kn/2, then nkn/2n0, and, combining this with (2.1), (3.11) and (3.12), we get that,

    V(|SnSk|2ϵnlnn)ˆE(φ1/2(|SnSk|2ϵnlnn))=ˆE(φ1/2(|Snk|2ϵnlnn))V(|Snk|ϵ(nk)ln(nk))<1/2.

    Also, if n/2<kn, then n,kn/2n0; thus,

    V(|SnSk|2ϵnlnn)V(|Sn|ϵnlnn)+V(|Sk|ϵnlnnϵklnk)<1/2.

    Taking α=1/2,βn,k=0 in Lemma 2.3, for n2n0,

    V(maxkn|Sk|4ϵnlnn)V(|Sn|2ϵnlnn).

    Since maxkn|Xk|2maxkn|Sk|, it follows that for n2n0

    V(maxkn|Xk|8ϵnlnn)V(|Sn|2ϵnlnn). (3.15)

    Let Yk=φ8/9(Xk9ϵnlnn). Then,

    I(maxkn|Xk|8ϵnlnn)=1I(maxkn|Xk|<8ϵnlnn)=1nk=1I(|Xk|<8ϵnlnn)1nk=1(1Yk).

    Since {Xk;k1} is a sequence of i.i.d. random variables, {1Yk;k1} is also a sequence of i.i.d. random variables, and 1Yk0; given (2.1), (2.3) and ˆE(X)=ˆε(X), it can be concluded that,

    V(maxkn|Xk|8ϵnlnn)ˆE(1nk=1(1Yk))=1ˆε(nk=1(1Yk))=1nk=1ˆε(1Yk)=1nk=1(1ˆEYk)1nk=1eˆEYk=1enˆEY1enV(|X|9ϵnlnn)nV(|X|9ϵnlnn).

    Hence, by (3.15) and (3.13)

    n=2lnnV(|X|nlnn)<.

    On the other hand,

    n=2lnnV(|X|nlnn)2lnxV(|X|xlnx)dx2ln22yV(|X|y)dyCV(X2).

    Hence,

    CV(X2)<. (3.16)

    Next, we prove that limcˆE(X(c))=limcˆE((X)(c))=0. For c1>c2>0, by (2.2) and (3.16),

    |ˆE(±X)(c1)ˆE(±X)(c2)|ˆE|(±X)(c1)(±X)(c2)|=ˆE(|X|c1c2)+ˆE(|X|c1)2c2CV(X2)c21c2.

    This implies that

    limc1>c2|ˆE(±X)(c1)ˆE(±X)(c2)|=0.

    By the Cauchy criterion, limcˆE(X(c)) and limcˆE((X)(c)) exist and are finite. It follows that limcˆE(X(c))=limnˆE(X(n)):=a. So, for any ϵ>0, when n is large enough, |ˆE(X(n))a|<ϵ; by Proposition 2.1 (iii), Lemma 2.1 (ii), ˆE(X(n)k+ˆEX(n)k)24ˆE(X(n)k)24CV(X2) and (3.16),

    ν(Snn<a2ϵ)ν((Snn<a2ϵ,1kn,|Xk|n)(1kn,|Xk|>n))ν(nk=1X(n)k<(a2ϵ)n)+nk=1V(|Xk|>n)=ν(nk=1(X(n)k+ˆEX(n)k)>(2ϵa)n+nEX(n))+nk=1V(|Xk|>n)ν(nk=1(X(n)k+ˆEX(n)k)>ϵn)+nk=1V(|Xk|>n)nk=1ˆE(X(n)k+ˆEX(n)k)2n2+nk=1ˆE(|Xk|n)2n21n0,n.

    It is concluded that,

    limnV(Snna2ϵ)=1foranyϵ>0.

    If a>0, taking ϵ<a/2, then ϵ1:=a2ϵ>0, and

    limnV(|Sn|nϵ1)limnV(Snnϵ1)=1. (3.17)

    On the other hand, by (3.14),

    limnV(|Sn|nϵ1)limnV(|Sn|ϵ1nlnn)=0,

    which contradicts (3.17). It follows that a0. Similarly, we can prove that b:=limcˆE((X)(c))0. From (X)(c)=X(c) and

    0a+b=limc(ˆE(X(c))+ˆE(X(c)))limcˆE(X(c)X(c))=0,

    we conclude that a=b=0, i.e., limcˆE(X(c))=limcˆE((X)(c))=0. This completes the proof of Theorem 3.1.

    Proof of Theorem 3.2. Note that

    ϵ2n=31nlnnV(|Sn|ϵnlnlnn)=ϵ2n=31nlnnV(|ξ|ϵlnlnn)+ϵ2n=31nlnn(V(|Sn|ϵnlnlnn)V(|ξ|ϵlnlnn)):=J1(ϵ)+J2(ϵ).

    Hence, in order to establish (3.3), it suffices to prove that

    limϵ0J1(ϵ)=CV(ξ2) (3.18)

    and

    limϵ0J2(ϵ)=0. (3.19)

    Obviously, (3.18) follows from

    limϵ0J1(ϵ)=limϵ0ϵ231xlnxV(|ξ|ϵlnlnx)dx=limϵ0εlnln32yV(|ξ|y)dy(lety=εlnlnx)=02yV(|ξ|y)dy=CV(ξ2).

    Let M32; write BM,ϵ:=exp(exp(Mϵ2)).

    |J2(ϵ)|ϵ23n[BM,ϵ]1nlnn|V(|Sn|nϵlnlnn)V(|ξ|ϵlnlnn)|+ϵ2n>[BM,ϵ]1nlnnV(|Sn|ϵnlnlnn)+ϵ2n>[BM,ϵ]1nlnnV(|ξ|ϵlnlnn):=J21(ϵ)+J22(ϵ)+J23(ϵ). (3.20)

    Let us first estimate J21(ϵ). For any β>ϵ2,

    I21(ϵ)ϵ2BM,ϵ31xlnx|V(|S[x]|[x]ϵlnlnx)V(|ξ|ϵlnlnx)|dxϵ2Bβ,ϵ32xlnxdx+ϵ2BM,ϵBβ,ϵ1xlnxsupnBβ,ϵ|V(|Sn|nϵlnlnx)V(|ξ|ϵlnlnx)|dx2β+M02ysupnBβ,ϵ|V(|Sn|ny)F(y)|dy.

    Similar to (3.9) we have

    limϵ0M0ysupnBβ,ϵ|V(|Sn|ny)F(y)|dy=0.

    Therefore, let ϵ0 first, then let β0; we get

    limϵ0J21(ϵ)=0. (3.21)

    Next, we estimate that J22(ϵ). Without loss of generality, we still assume that ˉσ=1. For nexp(exp(Mϵ2))exp(exp(32ϵ2)), set an:=ϵnlnlnn/16; from Proposition 2.1 (ii) and the condition that limcˆE(X(c))=0,

    ni=1|ˆEX(an)i|=n|limcˆE(X(c))ˆEX(an)|nlimcˆE|X(c)X(an)|=nlimcˆE(|X|can)+nlimcˆE(|X|c)2an=nˉσ2an=16nϵlnlnnϵ2nlnlnn.

    Using Lemma 2.1 for {X(an)iˆEX(an)i;1in}, and taking x=ϵnlnlnn/2 and y=2an=ϵnlnlnn/8 in Lemma 2.1 (i), if we note that |X(an)iˆEX(an)i|y, and Bn4n, combined with (3.12) we get

    V(Snϵnlnlnn)V(ni=1(X(an)iˆEX(an)i)ϵnlnlnn/2)+ni=1V(|Xi|an)exp(ϵ2nlnlnn4(ϵ2nlnlnn/16+4n){1+23lnϵ2nlnlnn64n})+nV(|X|μan)c(ϵ2lnlnn)2+nV(|X|μϵnlnlnn/16)

    from ϵ2nlnlnn4(ϵ2nlnlnn/16+4n){1+23ln(1+ϵ2lnlnn64)}2ln(ϵ2lnlnn64).

    Since {X,Xi} also satisfies (3.1), we can replace the {X,Xi} with {X,Xi} in the upper form

    V(Snϵnlnlnn)c(ϵ2lnlnn)2+nV(|X|μϵnlnlnn/16).

    Therefore

    V(|Sn|ϵnlnlnn)(ϵ2lnlnn)2+nV(|X|cϵnlnlnn).

    This implies the following from Markov's inequality and (2.5):

    J22(ϵ)+J23(ϵ)ϵ2nBM,ϵ1nlnn(nV(|X|cϵnlnlnn)+1ϵ4(lnlnn)2+ˆE|ξ|4ϵ4(lnlnn)2)ϵ2BM,ϵV(|X|cϵxlnlnx)lnxdx+cϵ2BM,ϵdxxlnx(lnlnx)2ϵ2Mϵ1ylnylnlnyV(|X|cϵy)dy+cM1MzV(|X|z)dz+cM10,M.

    Hence

    limϵ0(J22(ϵ)+J23(ϵ))=0.

    Combining this with (3.20) and (3.21), (3.19) is established.

    Statistical modeling is one of the key and basic topics in statistical theory research and practical application research. Under the theoretical framework of traditional probability space, in order to infer the model, all statistical models must assume that the error (and therefore the response variable) follows a unique and deterministic probability distribution, that is, the distribution of the model is deterministic. However, complex data in the fields of economics, finance, and other fields often have inherent and non negligible probability and distribution uncertainties. The probability distribution of the response variables that need to be studied is uncertain and does not meet the assumptions of classical statistical modeling. Therefore, classical probability statistical modeling methods cannot be used to model these types of data. How to analyze and model uncertain random data has been an unresolved and challenging issue that has long plagued statisticians. Driven by uncertainty issues, Peng [13] established a theoretical framework for the sub-linear expectation space from the perspective of expectations, providing a powerful tool for analyzing uncertainty problems. The sub-linear expectation has a wide range of potential applications. In recent years, the limit theory for sub-linear expectation spaces has attracted much attention from statisticians, and a series of research results have been achieved. This article overcomes the problem of many traditional probability space tools and methods no longer being effective due to the non additivity of sub-linear expectations and capacity; it also demonstrates the development of sufficient and necessary conditions for the rate convergence of logarithmic laws in sub-linear expectation spaces.

    The authors declare that they have not used artificial intelligence tools in the creation of this article.

    This paper was supported by the National Natural Science Foundation of China (12061028) and Guangxi Colleges and Universities Key Laboratory of Applied Statistics.

    Regarding this article, the author claims no conflict of interest.



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