This research focuses on a mathematical examination of a path to sliding period doubling and chaotic behaviour for a novel limited discontinuous systems of dimension three separated by a nonlinear hypersurface. The switching system is composed of dissipative subsystems, one of which is a linear systems, and the other is not linked with equilibria. The non-linear sliding surface is designed to improve transient response for these subsystems. A Poincaré return map is created that accounts for the existence of the hypersurface, completely describing each individual sliding period-doubling orbits that route to the sliding chaotic attractor. Through a rigorous analysis, we show that the presence of a nonlinear sliding surface and a set of such hidden trajectories leads to novel bifurcation scenarios. The proposed system exhibits period-m orbits as well as chaos, including partially hidden and sliding trajectories. The results are numerically verified through path-following techniques for discontinuous dynamical systems.
Citation: Hany A. Hosham, Thoraya N. Alharthi. Bifurcation and chaos in simple discontinuous systems separated by a hypersurface[J]. AIMS Mathematics, 2024, 9(7): 17025-17038. doi: 10.3934/math.2024826
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This research focuses on a mathematical examination of a path to sliding period doubling and chaotic behaviour for a novel limited discontinuous systems of dimension three separated by a nonlinear hypersurface. The switching system is composed of dissipative subsystems, one of which is a linear systems, and the other is not linked with equilibria. The non-linear sliding surface is designed to improve transient response for these subsystems. A Poincaré return map is created that accounts for the existence of the hypersurface, completely describing each individual sliding period-doubling orbits that route to the sliding chaotic attractor. Through a rigorous analysis, we show that the presence of a nonlinear sliding surface and a set of such hidden trajectories leads to novel bifurcation scenarios. The proposed system exhibits period-m orbits as well as chaos, including partially hidden and sliding trajectories. The results are numerically verified through path-following techniques for discontinuous dynamical systems.
In probability theory and other related fields, a stochastic process is a mathematical tool generally characterized as a group of random variables. Verifiably, the random variables were related with or listed by a lot of numbers, normally saw as focuses in time, giving the translation of a stochastic process speaking to numerical estimations some system randomly changing over time, for example, the development of a bacterial populace, an electrical flow fluctuating because of thermal noise, or the development of a gas molecule. Stochastic processes are broadly utilized as scientific models of systems that seem to shift in an arbitrary way. They have applications in numerous areas including sciences, for example, biology, chemistry, ecology, neuroscience, and physics as well as technology and engineering fields, for example, picture preparing, signal processing, data theory, PC science, cryptography and telecommunications. Furthermore, apparently arbitrary changes in money related markets have inspired the broad utilization of stochastic processes in fund. For the detailed survey about convex functions, inequality theory and applications, we refer [1,2,3,4] and references therein.
The study of convex stochastic process was initiated by Nikodem in 1980 [5]. He also investigated some regularity properties of convex stochastic process. Later on, some further results on convex stochastic process are derived in 1992 by Skowronski [6]. In recent developments on convex stochastic process, Kotrys [7] investigated Hermite–Hadamard type inequality for convex stochastic process and gave results for strongly convex stochastic process. In [8], the inequality for h-convex stochastic process were derived. The interesting work on stochastic process are [17,18,19,20,21].
The aim of this paper is to introduce the notion of η-convex stochastic process and derive Hermite–Hadamard and Jensen Type inequality for η-convex stochastic process. The main motivation for this paper is the idea of ϕ-convex function and η-convex function [9,10], respectively. For other interesting generalizations, we refer [13,14,15,16,22,23,24,25] to the readers and references therein.
The mapping ξ defined for a σ field Ω to R is F-measurable for each Borel set B∈β(R), if
{ω∈Ω/ξ(ω)∈B}∈F. |
For a probability space (Ω,F,P), the mapping ξ is said to be random variable. The random variable ξ becomes integrable if
∫Ω|ξ|dp<∞. |
If the random variable ξ is integrable, then E(ξ)=∫Ωξdp exists and is called expectation of ξ. The family of integrable random variables ξ:Ω→R is denoted by L′(Ω,F,P).
Now we present the definition and basic properties of mean-square integral [11].
Suppose that ξ1:I×Ω→R is a stochastic process with E[ξ1(t)2]<∞ for all t∈I and [a,b]∈I, a=t0<t1<t2<⋯<tn=b is a partition of [a,b] and Θk∈[tk−1,tk] for all k=1,⋯,n. Further, suppose that ξ2:I×Ω→R be a random variable. Then, it is said to be mean-square integral of the process ξ1 on [a,b], if for each normal sequence of partitions of the interval [a,b] and for each Θk∈[tk−1,tk], k=1,⋯,n, we have
limn→∞E[(n∑k=1ξ1(Θk)·(tk−tk−1)−ξ2)2]=0. |
Then, we can write
ξ2(.)=∫baξ1(s,.)ds(a.e.). | (1.1) |
The monotonicity of the mean square integral will be used frequently throughout the paper. If ξ1(t,.)≤ξ2(t,.) (a.e.) for the interval [a,b], then
∫baξ1(t,.)dt≤∫baξ2(t,.)dt(a.e.) | (1.2) |
The inequality (1.2) is the immediate consequence of the definition of the mean-square integral.
Lemma 1.1. If X:I×Ω→R is a stochastic process of the form X(t,.)=A(.)t+B(.), where A,B:Ω→R are random variables such that E[A2]<∞,E[B2]<∞ and [a,b]⊂I, then
∫baX(t,.)dt=A(.)b2−a22+B(.)(b−a)(a.e.). | (1.3) |
Now, we present the definition of η-convex stochastic process.
Definition 1.2. Let (Ω,A,P) be a probability space and I⊆R be an interval, then ξ:I×Ω→R is an η-convex stochastic process, if
ξ(λb1+(1−λ)b2,.)≤ξ(b2,.)+λη(ξ(b1,.),ξ(b2,.))(a.e) | (1.4) |
for all b1,b2∈I and λ∈[0,1].
In (1.4), if we take η(b1,b2)=b1−b2, we obtain convex stochastic process. By taking ξ(b1,.)=ξ(b2,.) in (1.4) we get
λη(ξ(b1,.),ξ(b1,.))≥0 |
for any b1∈I and t∈[0,1]. Which implies that
η(ξ(b1,.),ξ(b1,.))≥0 |
for any b1∈I.
Also, if we take λ=1 in (1.4), we get
ξ(b1,.)−ξ(b2,.)≤η(ξ(b1,.),ξ(b2,.)) |
for any b1,b2∈I. The second condition implies the first one, so if we want to define η convex stochastic process on an interval I of real numbers, we should assume that
η(b1,b2)≥b1−b2 | (1.5) |
for any b1,b2∈I.
One can observe that, if ξ:I→R is convex stochastic process and η:ξ(I)×ξ(I)→R is an arbitrary bi-function that satisfies the condition (1.5), then for any b1,b2∈I and t∈[0,1], we have
ξ(tb1+(1−t)b2,.)≤ξ(b2,.)+λ(ξ(b1,.)−ξ(b2,.))≤ξ(b2,.)+λη(η(b1,.),η(b2,.)), |
which tells that ξ is η convex stochastic process.
Definition 1.3. (η Quasi-convex stochastic process) A stochastic Process ξ:I×Ω→R is said to be η quasi-convex stochastic process if
ξ(tb1+(1−t)b2,.)≤max{ξ(b2,.),ξ(b2,.)+η(ξ(b1,.),ξ(b2,.))(a.e.) |
Definition 1.4. (η-affine) A stochastic process ξ:I×Ω→R is said to be η-affine if
ξ(tb1+(1−t)b2,.)=ξ(b2,.)+tη(ξ(b1,.),ξ(b2,.))(a.e.) |
for all b1,b2∈I and t∈[0,1]
Definition 1.5. (Non-Negatively Homogeneous) A function η:A×B→R is said to be non-negatively homogenous if
η(γb1,γb2)=γη(b1,b2) | (1.6) |
for all b1,b2∈R and γ≥0.
Definition 1.6. (Additive) A function η is said to be additive if
η(x1,y1)+η(x2,y2)=η(x1+x2,y1+y2) | (1.7) |
for all x1,x2,y1,y2∈R.
Definition 1.7. (Non-negatively linear function) A function η is said to be non-negatively linear, if it satisfy (1.6) and (1.7).
Definition 1.8. (Non-decreasing in first variable) A function η is said to be non-decreasing in first variable if b1≤b2 implies η(b1,b3)≤η(b2,b3) for all b1,b2,b3∈R.
Definition 1.9. (Non-negatively sub-linear in first variable) A function η is said to be non-negatively sub-linear in first variable if
η(γ(b1+b2),b3)≤γη(b1,b3)+γη(b2,b3) |
for all b1,b2,b3∈R and γ≥0.
We shall begin with few preliminary proposition for η-convex function.
Proposition 1. Consider two η convex stochastic process ξ1,ξ2:I×Ω→R, such that
1.If η is additive then ξ1+ξ2:I→R is η convex stochastic process.
2. If η is non-negatively homogenous, then for any γ≥0, γξ1:I×Ω→R is η- convex stochastic process.
Proof. The proof of the proposition is straight forward.
Proposition 2. If ξ:[b1,b2]→R is η convex stochastic process, then
maxx∈[b1,b2]ξ(x,.)≤max{ξ(b2,.),ξ(b2,.)+η(ξ(b1,.),ξ(b2,.))}. |
Proof. Consider x=αb1+(1−α)b2 for arbitrarily x∈[b1,b2] and some α∈[0,1]. We can write
ξ(x,.)=ξ(αb1+(1−α)b2,.). |
Since ξ is η convex stochastic process, so by definition
ξ(x,.)≤ξ(b2,.)+αη(ξ(b1,.),ξ(b2,.)) | (1.8) |
and
ξ(b2,.)+αη(ξ(b1,.),ξ(b2,.))≤max{ξ(b2,.),ξ(b2,.)+η(ξ(b1,.),ξ(b2,.)). | (1.9) |
Since x is arbitrary, so from (1.8) and (1.9), we get our desired result.
Theorem 1.10. A random variable ξ:I×Ω→R is η convex stochastic process if and only if for any c1,c2,c3∈I with c1≤c2≤c3, we have
det((c3−c2)ξ(c2,.)−ξ(c3,.)(c3−c1)η(ξ(c1,.),ξ(c3,.)))≥0. |
Proof. Suppose that ξ is an η-convex stochastic process and c1,c2,c3∈I such that c1≤c2≤c3. Then, their exits α1∈(0,1), such that
c2=α1c1+(1−α1)c3 |
where α1=c2−c3c1−c3.
By definition of η convex stochastic process, we have
ξ(c2,.)=ξ(α1c1+(1−α1)c3,.)≤ξ(c3,.)+(c2−c3c1−c3)η(ξ(c1,.),ξ(c3,.))so0≤ξ(c3,.)−ξ(c2,.)+(c2−c3)(c1−c3)η(ξ(c1,.),ξ(c3,.))0≤(ξ(c3,.)−ξ(c2,.))(c3−c1)+(c3−c2)η(ξ(c1,.),ξ(c3,.)). |
Hence
det((c3−c2)ξ(c2,.)−ξ(c3,.)(c3−c1)η(ξ(c1,.),ξ(c3,.)))≥0. |
For the reverse inequality, take y1,y2∈I with y1≤y2. Choose any α1∈(0,1), then, we have
y1≤α1y1+(1−α1)y2≤y2. |
So, the above determinant is;
0≤[y2−[α1y1+(1−α1)y2]]η(ξ(y1,.),ξ(y2,.))−(y2−y1)(ξ(α1y1+(1−α1)y2,.)−ξ(y2,.) |
implies
(ξ(α1y1+(1−α1)y2,.)≤ξ(y2,.)+α1(y2−y1)(y2−y1)η(ξ(y1,.),ξ(y2,.))≤ξ(y2,.)+α1η(ξ(y1,.),ξ(y2,.)). |
Which is as required.
We will use the following relation to prove the Jesen type inequality for η-convex stochastic process. Let ξ:I×Ω→R be an η-convex stochastic process. For x1,x2∈ I and α1+α2 = 1, we have
ξ(α1x1+α2x2,.)≤ξ(x2,.)+α1η(ξ(x1,.),ξ(x2,.)). |
Also, when n>2 for x1,x2,...,xn∈I,n∑i=1αi=1 and Ti=i∑j=1αj, we have
ξ(n∑i=1αixi,.)=ξ(Tn−1n−1∑i=1αiTn−1xi+αnxn,.)≤ξ(xn,.)+Tn−1η(ξ(n−1∑i=1αiTn−1xi,.),ξ(xn,.)) | (2.1) |
Theorem 2.1. Let ξ:I×Ω→R be an η-convex stochastic process and η:A×B→R be the non-decreasing non-negatively sub-linear in first variable. If Ti=i∑j=1αj for i=1,2,...,n such that Tn=1, then
ξ(n∑i=1αixi,.)≤ξ(xn,.)+n−1∑i=1Tiηξ(xi,xi+1,...,xn) | (2.2) |
where ηξ(xi,xi+1,...,xn)=η(ηξ(xi,xi+1,...,xn−1,.),ξ(xn,.)) and ηξ(x,.)=ξ(x,.) for all x∈I.
Proof. Since η is non-decreasing, non-negatively, sub-linear in first variable, so from (2.1)
ξ(n∑i=1αixi,.)≤ξ(xn,.)+Tn−1η(ξ(n−1∑i=1αiTn−1xi),f(xn))=ξ(xn,.)+Tn−1η(ξ(Tn−2Tn−1n−2∑i=1αiTn−2xi,+αn−1Tn−1xn−1,.),ξ(xn,.))≤ξ(xn,.)+Tn−1η(ξ(xn−1,.)+(Tn−2Tn−1)η(ξ(n−2∑i=1αiTn−2xi,ξ(xn−1,.)),ξ(xn,.))≤ξ(xn,.)+Tn−1η(ξ(xn−1,x.),ξ(xn,.))+Tn−2η(η(ξ(n−2∑i=1αiTn−2xi,.),ξ(xn−1,.)),ξ(xn,.))≤…≤(xn)+Tn−1η(ξ(xn−1,.),ξ(xn,.))+Tn−2η(ξ(xn−2,.),ξ(xn−1,.)),ξ(xn,.))+…+T1(η(xi(x1,.),ξ(x2,.)),ξ(x3,.))…,ξ(xn−1,.)),ξ(xn,.))=ξ(xn,.)+n−1∑i=1Tiηξ(xi,xi+1,…,xn,.). |
Hence the proof is complete.
Now, we established new inequality for the η-convex stochastic process that is connected with the Hermite–Hadamard inequality.
Theorem 3.1. Suppose that ξ:[c1,c2]×Ω→R is an η convex stochastic process such that η is bounded above ξ[c1,c2]×ξ[c1,c2], then
ξ(c1+c22)−12Mη≤1c2−c1∫c2c1ξ(y,.)dy≤12[ξ(c1,.)+ξ(c2,.)]+12[η(ξ(c1,.),ξ(c2,.))+η(ξ(c2,.),ξ(c1,.))2]≤12[ξ(c1,.)+ξ(c2,.)]+12Mη | (3.1) |
where Mη is upper bound of η.
Proof. For the right side of inequality, consider an arbitrary point y=α1c1+(1−α1)c2 with α1∈[0,1]. We can write as
ξ(y,.)=ξ((α1c1+(1−α1)c2),.). |
Since ξ is η convex stochastic process, so by definition
ξ(y,.)≤ξ(c2,.)+α1η(ξ(c1,.),ξ(c2,.)) |
with α1=y−c2c1−c2. It follows that
ξ(y,.)≤ξ(c2,.)+(y−c2c1−c2)η(ξ(c1,.),ξ(c2,.)). |
Now, using Lemma 1.1, we get
ξ(y,.)≤1c2−c1[(ξ(c2,.)(c2−c1)+(c2−c1)2η(ξ(c1,.),ξ(c2,.)))]1c2−c1∫c2c1ξ(y,.)dy≤ξ(c2,.)+12η(ξ(c1,.),ξ(c2,.)). |
Also, we have
1c2−c1∫c2c1ξ(y,.)dy≤ξ(c1,.)+12η(ξ(c2,.),ξ(c1,.)). |
Therefore, we get
1c2−c1∫c2c1ξ(y,.)dy≤min{ξ(c2,.)+12η(ξ(c1,.),ξ(c2,.)),ξ(c1,.)+12η(ξ(c2,.),ξ(c1,.))}≤12[ξ(c1,.)+ξ(c2,.)]+[η(ξ(c1,.),ξ(c2,.))+η(ξ(c2,.),ξ(c1,.))]≤12[ξ(c1,.)+ξ(c2,.)]+Mη, |
where Mη=[η(ξ(c1,.),ξ(c2,.))+η(ξ(c2,.),ξ(c1,.))].
For the left side of inequality, the definition of η-convex stochastic process of ξ implies that
ξ(c1+c22,.)=ξ(c1+c24−α1(c2−c1)4+c1+c24+α1(c2−c1)4,.)=ξ(12c1+c2−α1(c2−c1)2+12c1+c2+α1(c2−c1)2,.)≤ξ(c1+c2+α1(c2−c1)2,.)+(12)η(ξ(c1+c2−α1(c2−c1)2),ξ(12c1+c2−α1(c2−c1)2,.))≤ξ(c1+c2+α1(c2−c1)2,.)+12Mη∀α1∈[0,1]. |
Here
(c1+c2+α1(c2−c1)2,.)≥ξ(c1+c22,.)−12Mη(a.e.) | (3.2) |
and
ξ(c1+c2−α1(c2−c1)2,.)≥ξ(c1+c22,.)−12Mη(a.e.). | (3.3) |
Finally, using change of variable, we have
1c2−c1∫c2c1ξ(y,.)dy=1c2−c1[∫c1+c22c1ξ(y,.)dy+∫c2c1+c22ξ(y,.)dy]=12∫10[ξ(c1+c2−α1(c2−c1)2,.)+ξ(c1+c2+α1(c2−c1)2,.)]dα1. |
From (3.2) and (3.3), we get
1c2−c1∫c2c1ξ(y,.)dy≥12∫10[ξ(c1+c22,.)−12Mη+ξ(c1+c22,.)−12Mη)]dα1≥12∫10[2ξ(c1+c22,.)−22Mη]dα1≥12[2ξ(c1+c22,.)−Mη]≥ξ(c1+c22,.)−12Mη. |
Hence, the proof is completed.
Remark 1. By taking η(x,y)=x−y in (3.1), we get the classical Hermite–Hadamard inequality for convex stochastic process [7].
In order to prove Ostrowski type inequality for η-convex stochastic process, the following Lemma is required.
Lemma 4.1. [12] Let ξ:I×Ω→R be a stochastic process which is mean square differentiable on I∘. If ξ′ is mean square integrable on [c1,c2], where c1,c2∈I with c1<c2, then the following equality holds
ξ(t,.)−1c2−c1∫c2c1ξ(u,.)du=(x−c1)2c2−c1∫10tξ′(tx+(1−t)c1,.)dt−(c2−x)2c2−c1∫10tξ′(tx+(1−t)c2,.)dt,(a.e.), | (4.1) |
for each x∈[c1,c2].
Theorem 4.2. Let ξ:I×Ω→R be a mean square stochastic process such that ξ′ is mean square integrable on [c1,c2], where c1,c2∈I with c1<c2. If |ξ′| is an η- convex stochastic process on I and |ξ′(t,.)|≤M for every t, then
|ξ(t,.)−1c2−c1∫c2c1ξ(u,.)du|≤M2[(t−c1)2+(c2−t)2c2−c1]+(t−c1)23(c2−c1)η(|ξ′(t,.)|,|ξ′(c1,.)|)+(c2−t)23(c2−c1)η(|ξ′(t,.)|,|ξ′(c2,.)|),(a.e.). |
Proof. Since |ξ′| is an η–convex stochastic process, so by (4.1), we have
|ξ(t,.)−1c2−c1∫c2c1ξ(u,.)du|≤(t−c1)2c2−c1∫10y|ξ′(yt+(1−y)c1,.)|dy+(c2−t)2c2−c1∫10y|ξ′(yt+(1−y)c2,.)|dy≤(t−c1)2c2−c1∫10y[|ξ′(c1,.)|+yη(|ξ′(t,.)|,|ξ′(c1,.)|)]dy+(c2−t)2c2−c1∫10y[|ξ′(c2)|+yη(|ξ′(t,.)|,|ξ′(c2,.)|)]dy≤M[(t−c1)2+(c2−t)2c2−c1]∫10ydy+(t−c1)2c2−c1∫10y2η(|ξ′(t,.)|,|ξ′(c1,.)|)dt+(c2−t)2c2−c1∫10y2η(|ξ′(t,.)|,|ξ′(c2,.)|)dy≤M2[(t−c1)2+(c2−t)2c2−c1]+(t−c1)23(c2−c1)η(|ξ′(t,.)|,|ξ′(c1,.)|)+(c2−t)23(c2−c1)η(|ξ′(t,.)|,|ξ′(c2,.)|). |
Hence proof is completed.
There are many applications of Stochastic-processes, for example, Kolmogorov-Smirnoff test on equality of distributions [26,27,28]. The other application includes Sequential Analysis [29,30] and Quickest Detection [31,32]. In this paper, we introduced η-convex Stochastic processes and proved Jensen, Hermite-Hadamard and Fejr type inequalities. Our results are applicable, because the expected value of a random variable is always bounded above by the expected value of the convex function of the random variable.
The authors declare that no competing interests exist.
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