Research article Special Issues

Exploring three periodic point dynamics in 2D spatiotemporal discrete systems

  • Received: 23 October 2024 Revised: 08 January 2025 Accepted: 13 February 2025 Published: 06 March 2025
  • MSC : 47A10, 37G10, 37G35, 37L15

  • This paper explores the dynamics of 2D spatiotemporal discrete systems, focusing on the stability and bifurcations of periodic solutions, particularly 3-cycles. After introducing the concept of a third-order cycle, we discuss both numerical and analytical techniques used to analyze these cycles, defining four types of 3-periodic points and their associated stability conditions. As a specific case, this study examines a spatiotemporal quadratic map, analyzing the existence of 3-cycles and various bifurcation scenarios, such as fold and flip bifurcations, as well as chaotic behavior. In 2D spatiotemporal systems, quadratic maps intrinsically offer better conditions that favor the emergence of chaos, which is characterized by high sensitivity to initial conditions. The findings emphasize the complexity of these systems and the crucial role of bifurcation curves in understanding stability regions. The paper concludes with key insights and suggestions for future research in this field.

    Citation: Mohamed Lamine Sahari, Abdel-Kaddous Taha, Louis Randriamihamison. Exploring three periodic point dynamics in 2D spatiotemporal discrete systems[J]. AIMS Mathematics, 2025, 10(3): 5021-5051. doi: 10.3934/math.2025230

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  • This paper explores the dynamics of 2D spatiotemporal discrete systems, focusing on the stability and bifurcations of periodic solutions, particularly 3-cycles. After introducing the concept of a third-order cycle, we discuss both numerical and analytical techniques used to analyze these cycles, defining four types of 3-periodic points and their associated stability conditions. As a specific case, this study examines a spatiotemporal quadratic map, analyzing the existence of 3-cycles and various bifurcation scenarios, such as fold and flip bifurcations, as well as chaotic behavior. In 2D spatiotemporal systems, quadratic maps intrinsically offer better conditions that favor the emergence of chaos, which is characterized by high sensitivity to initial conditions. The findings emphasize the complexity of these systems and the crucial role of bifurcation curves in understanding stability regions. The paper concludes with key insights and suggestions for future research in this field.



    The idea of a fixed point was started in 19th century and different mathematicians, like Schauder, Tarski, Brouwer [1,2,3] and others worked on it in 20th century. The presence for common fixed points of different families with nonexpansive and contractive mappings in Hilbert spaces as well as in Banach spaces was the exhaustive topic of research since the early 1960s as explored by many researchers like Banach, Brouwer and Browder etc. Latterly, Khamsi and Kozlowski [4,5] proved results in modular function spaces for common fixed points of nonexpansive, asymptotically nonexpansive and contractive mappings. The theory of a fixed point has a substantial position in the fields of analysis, geometry, engineering, topology, optimization theory, etc. For some latest algorithms developed in the fields of optimisation and inverse problems, we refer to [6,7]. For more detailed study of fixed point and applications, see [8,9,10,11,12,13,14,15,16,17,18,19,20,21,22] and the references there in.

    The concept of fixed points of one parameter semigroups of linear operators on a Banach space was originated from 19th century from the remarkable work of Hille-Yosida in 1948. Now-a-days, it has a lot of applications in many fields such as stochastic processes and differential equations. Semigroups have a monumental position in the fields of functional analysis, quantum mechanics, control theory, functional equations and integro-differential equations. Semigroups also play a significant role in mathematics and application fields. For example, in the field of dynamical systems, the state space will be defined by the vector function space and the system of an evolution function of the dynamical system will be represented by the map (h)kT(h)k. For related study, we refer to [23].

    Browder [24] gave a result for the fixed point of nonexpansive mappings in a Banach space. Suzuki [25] proved a result for strong convergence of a fixed point in a Hilbert space. Reich [26] gave a result for a weak convergence in a Banach space. Similarly, Ishikawa [27] presented a result for common fixed points of nonexpansive mappings in a Banach space. Reich and Shoikhet also proved some results about fixed points in non-linear semigroups, see [20]. Nevanlinna and Reich gave a result for strong convergence of contraction semigroups and of iterative methods for accretive operators in Banach spaces, see [28,29]. There are different results on strong convergence of a fixed point of semigroups and there are sets of common fixed points of semigroups by the intersection of two operators from the family. These results are much significant in the field of fixed point theory. In a recent time, different mathematicians are working to generalize such type of results for a subfamily of an evolution family, see [30,31,32].

    The fixed point of a periodic evolution subfamily was discussed in [30] by Rahmat et al. They gave a result for finding common fixed points of the evolution subfamily with the help of a strongly converging sequence. The method applied in [30] is successfully useful for showing the presence of a fixed point of an evolution subfamily. The purpose of this work is to show the existence of a fixed point of an evolution subfamily with the help of a sequence acting on a Banach space.

    Definition 1.1. Let v: AA be a self-mapping. A point rA is a fixed point of v if v(r)=r.

    The idea of semigroups is originated from the solution of the Cuachy differnetial equations of the form:

    {˙Λ(b)=K(Λ(b)),b0,Λ(0)=Λ0,

    where K is a linear operator.

    Definition 1.2. A family Y={Y(a);a0} of bounded linear operators is a semigroup if the following conditions hold:

    (i) Y(0)=I.

    (ii) Y(j+k)=Y(j)Y(k), j,k0.

    When K=K(t), then such a system is called a non-autonomous system. The result of this system produces the idea of an evolution family.

    Definition 1.3. A family E={E(u,g);ug0} of bounded linear operators is said to be an evolution family if the following conditions hold:

    (i) E(p,p)=I, p0.

    (ii) E(j,q)E(q,b)=E(j,b), jqb0.

    Remark 1.4. If the evolution family is periodic of each number r0, then it forms a semigroup. If we take E(c,0)=Y(c), then

    (a1) Y(0)=E(0,0)=I.

    (a2) Y(c+y)=E(c+y,0)=E(c+y,y)E(y,0)=E(c,0)E(y,0)=Y(c)Y(y), which shows that a periodic evolution family of each positive period, is a semigroup.

    Similarly, if we take Y(rd)=E(r,d), then

    (b1) E(r,r)=Y(0)=I.

    (b2) E(r,b)=E(r,d)E(d,b)=Y(rd)Y(db)=Y(rb), which shows that a semigroup is an evolution family.

    Remark 1.5. A semigroup is an evolution family, but the converse is not true. In fact, the converse holds if the evolution family is periodic of every number s0.

    Remark 1.6. [33] Let 0s1 and b,kH, then the following equality holds:

    ||sb+(1s)k||2=s||b||2+(1s)||k||2s(1s)||bk||2.

    In this work, we will generalize results from [33] for an evolution subfamily and also give some other results for an evolution subfamily.

    First, denote the set of real numbers and natural numbers by R and N, respectively. We denote the family of semigroups by Y, evolution family by E and evolution subfamily by G. By B, H and D, we will indicate a Banach space, Hilbert space and a convex closed set, respectively. We use for a strong and for a weak convergence. The set of fixed points of

    G={G(s,0);s0}

    is denoted by

    F(G)=s0F(G(s,0)).

    We generalize results of semigroups from [33] for an evolution subfamily G in a Banach space. These types of families are not semigroups. The following example illustrates this fact and gives the difference between them.

    Example 2.1. As

    E={E(h,r)=h+1r+1;hr0}

    is an evolution family because it satisfies both conditions of an evolution family.

    If we take r=0, that is, {E(h,0)}=G, then it becomes a subfamily of E and it is not a semigroup.

    Suzuki proved the following result in [25]:

    Theorem 2.2. Consider a family

    Y={Y(i),i0}

    of strongly continuous non-expansive operators on D (where D is a subset of a Hilbert space H) such that F(Y). Take two sequences {γm} and {qm} in R with

    limmqm=limmγmqm=0,

    qm>0 and γm(0,1). Let bD be fixed and {km} be a sequence in D such that

    km=γmb+(1γm)Y(qm)km,  mN,

    then {km}hF(Y).

    The following result was given by Shimizu and Takahashi [15] in 1998:

    Theorem 2.3. Take a family

    Y={Y(i),i0}

    of operators which are non-expansive and strongly continuous on DH such that F(Y). Take two sequences {ζm} and {λm} in R with

    limmζm=0,limmλm=,

    where ζm(0,1) and λm>0. Let cD be fixed and {gm}D be a sequence such that

    gm=ζmc+(1ζm)1λmλm0Y(s)ds

    for all mN. Then {gm}aF(Y).

    Motivated from above results, we take an implicit iteration for G={G(b,0),b0} of nonexpansive mappings, given as:

    {τm=γmτm1+(1γm)G(ζm,0)τm, m1,τ0D. (2.1)

    We present some results for convergence of Eq (2.1) in a Banach space and a Hilbert space for a nonexpansive evolution subfamily.

    We start with the following lemmas:

    Lemma 3.1. Consider an evolution family E and a subfamily G={G(c,0);c0} of E with period rR+, then

    c0F(G(c,0))=0crF(G(c,0)).

    Proof. As it is obviously true that

    c0F(G(c,0))0crF(G(c,0)),

    we are proving the other part, i.e.,

    0crF(G(c,0))c0F(G(c,0)).

    Take a real number

    k0crF(G(c,0)),

    then

    G(c,0)k=k, 0cr.

    As we know that any real number c0 is written in the form of c=mr+ε, for some mZ+ and 0εr, consider

    G(c,0)k=G(mr+ε,0)k=G(mr+ε,mr)G(mr,0)k=G(ε,0)Gm(r,0)k=G(ε,0)k=k.

    This shows that

    0crF(G(c,0))c0F(G(c,0)).

    Hence, we conclude that

    c0F(G(c,0))=0crF(G(c,0)).

    This completes the proof.

    Lemma 3.2. If Y={Y(β);β0} is a semigroup on a Hilbert space H, then

    F(Y)=β0F(Y(β))=0β1F(Y(β)).

    Proof. Since

    β0F(Y(β))0β1F(Y(β)),

    we only prove the other part, that is,

    0β1F(Y(β))β0F(Y(β)).

    Take a real number u such that

    u0β1F(Y(β)),

    then we have Y(u)=u, for every β[0,1]. Since β[0,1], we can write it as β=n+ϱ, where nZ+ and 0ϱ1. Therefore, we have

    Y(β)u=Y(n+ϱ)u=Y(n)Y(ϱ)u=Yn(1)Y(ϱ)u=Yn(1)u=u.

    This shows that uβ0F(Y(β)). It implies that

    0β1F(Y(β))β0F(Y(β)).

    Thus,

    β0F(Y(β))=0β1F(Y(β)).

    This completes the proof.

    Now, we give a result for a weak convergence of a sequence in a Hilbert space.

    Theorem 3.3. Let G={G(a,0)} be a subfamily of E of strongly continuous nonexpansive operators on D and F(G), where D is a subset of H. Take two sequences {γm} and {ζm} in R such that

    {γm}(0,c](0,1),ζm>0,
    lim infmζm=0,lim supmζm>0,

    and

    limm(ζm+1ζm)=0.

    Then

    τm=γmτm1+(1γm)G(ζm,0)τmτ,

    where τF(G).

    Proof. Claim (ⅰ). For any zF(G), limm||τmz|| exists. In fact,

    ||τmz||=||γm(τm1z)+(1γm)(G(ζm,0)τmz)||γm||τm1z||+(1γm)||G(ζm,0)τmz||γm||τm1z||+(1γm)||τm1z||,  m1.

    Thus, we have

    ||τmz||||τm1z||,  m1.

    This shows that limm||τmz|| exists. Therefore, the sequence {τm} is bounded.

    Claim (ⅱ).

    limm||G(ζm,0)τmτm||=0.

    From Remark 1.6, we have

    ||τmz||2=||γm(τm1z)+(1γm)(G(ζm,0)τmz)||2=γm||τm1z||2+(1γm)||G(ζm,0)τmz||2γm(1γm)||τm1G(ζm,0)τm||2γm||τm1z||2+(1γm)||τmz||2γm(1γm)||τm1G(ζm,0)τm||2.

    Thus, we have

    ||τmz||2||τm1z||2(1γm)||τm1G(ζm,0)τm||2,  m1.

    As we know that {γm}(0,c](0,1), so we have

    (1c)||τm1G(ζm,0)τm||2||τm1z||2||τmz||2, (3.1)

    i.e.,

    (1c)lim supm||τm1G(ζm,0)τm||2lim supm||τm1z||2||τmz||2=0.

    Therefore,

    limm||τm1G(ζm,0)τm||=0.

    On the other hand,

    limm||τmG(ζm,0)τm||=limmγm1||τm1G(ζm,0)τm||=0.

    Claim (ⅲ).

    {τm}τ,  where  τF(G).

    As {τm} is bounded, take a subsequence {ωmi} of {τm} such that {ωmi}τ. Let ωmi=hi, γmi=ξi and ζmi=vi. From [34], we have

    limivi=limi||hiG(vi,0)hi||vi=0.

    Now, we will show that G(ζ,0)τ=τ.

    We have

    ||hiG(ζ,0)τ||[ζvi]1a=0||G((a+1)vi,0)hiG(avi,0)hi||+||G([ζvi]vi,0)hiG(ζvivi,0)τ||+||G(ζvivi,0)τG(ζ,0)||ζvi||G(vi,0)hihi||+||hiτ||+||G(ζ[ζvi]vi,0)ττ||ζ||G(vi,0)hihi||vi+||hiτ||+max0vvi||G(v,0)ττ||,  iN.

    Thus, we get

    lim supi||hiG(ζ,0)τ||lim supi||τiτ||.

    Hence, G(ζ,0)τ=τ by using Opial's condition. Therefore, τF(G). Now, we need to show that {τm}τ. For this, take a subsequence {ηmj} of {τm} such that ηmju and uτ. By above method, we can show that uF(G). Since both limits limm||τmτ|| and limm||τmu|| exist, we can write

    limm||τmτ||=lim supi||ωmiτ||<lim supi||ωmiu||=limm||τmu||=lim supj||ηmju||<lim supj||ηmjτ||=limm||τmτ||.

    It shows that u=τ, which is a contradiction. Thus, τmτ.

    This completes the proof.

    Now, we will provide a theorem in a Banach space for a weak convergence.

    Theorem 3.4. Consider a reflexive Banach space B in R with Opial's property and a subset D of B. Let G={G(a,0)} be a subfamily of E of nonexpansive and strongly continuous mappings such that F(G). Take two sequences {γm} and {ζm} such that γm(0,1), ζm>0 and

    limmζm=limmγmζm=0.

    Then

    τm=γmτm1+(1γm)G(ζm,0)τmτF(G).

    Proof. Claim 1. As

    limmζm=limmγmζm=0,

    then we have limmγm=0. This shows that there exists a positive integer p, for all kN so that γm(0,c](0,1).

    From Theorem 3.3, limm||τmz|| exists for each zF(G).

    Claim 2. {G(ζm,0)τm} is bounded. From (2.1), we have

    ||G(ζm,0)τm}||=||11γmτmγm1γmτm1||11γm||τm||+γm1γm||τm1||1c||τm||+c1c||τm1||,

    which shows that {G(ζm,0)τm} is bounded.

    Claim 3. {τm}τ.

    As {τm} is bounded, take a sub-sequence {ωml} of {τm} such that ωmlτ. Let ωml=bl, γml=ρl and ζml=yl, lN. Let ζ>0 be fixed, then

    ||blG(ζ,0)τ||[ζyl]1a=0||G((a+1)yl,0)blG(ayl,0)bl||+||G([ζyl]yl,0)blG(ζylyl,0)τ||+||G(ζylyl,0)τG(ζ,0)||ζyl||G(yl,0)blbl||+||blτ||+||G(ζ[ζyl]yl,0)ττ||ζ||G(yl,0)blbl||yl+||blτ||+max0yyl||G(y,0)ττ||,  lN.

    Thus, we have

    lim supl||blG(ζ,0)τ||lim supl||blτ||.

    Therefore,

    G(ζ,0)τ=τF(G)

    by using Opial's property. By same method given in Theorem 3.3, we can prove that {τm}τ.

    This completes the proof.

    Theorem 3.5. Consider a real reflexive Banach space B with Opial's property and a subset D of B. Let G={G(a,0)} be a subfamily of E of strongly continuous nonexpansive mappings such that F(G). Take two sequences {γm} and {ζm} such that γm(0,1), ζm>0 and

    limmζm=limmγmζm=0.

    Then

    τm=γmτm1+(1γm)G(ζm,0)τmτF(G).

    Proof. Claim 1. For any zF(G), limm||τmz|| exists.

    Claim 2.

    ||G(ζm,0)τmτm||0  as  m. (3.2)

    As from Theorem 3.4, {G(ζm,0)τm} is bounded. Also, from (1.4), we have

    ||τmG(ζm,0)τm||=γm||τm1G(ζm,0)τm||0  as  m.

    Therefore,

    ||G(ζm,0)τmτm||0  as  m.

    Claim 3. For any ζ>0,

    limm||G(ζm,0)τmτm||=0.

    In fact, we have

    ||τmG(ζm,0)τm||ζζm1b=0||G((b+1)ζm,0)τmG(bζm,0)τm||+||G((ζζm)ζm,0)τmG(ζ,0)τm||ζζm||G(ζm,0)τmτm||+||G((ζζζm)ζm,0)τmτm||ζγmζm||τm1G(ζm,0)||+maxs[0,ζm]{||G(v,0)τmτm||},  mN.

    Thus, from this equation and Eq (3.2), we get

    limm||G(ζm,0)τmτm||=0.

    Claim 4. Now, we will show that {τm}τF(G).

    Since {τm} is bounded, it must have a convergent sub-sequence {μmk} such that μmkτ. From Claim 3, we have

    ||τG(ζ,0)τ||=limk||μmkG(ζ,0)μmk||=0.

    Thus, τF(G). Hence, we have

    limm||τmτ||=limk||μmkτ||=0.

    This completes the proof.

    Example 4.1. Consider the Hilbert space H=L2([0,π],C) and let T={T(a);a0} be a semigroup such that

    (T(a)u)(t)=2πm=1eam2wm(u)sinmt,t[0,π], a0.

    Here,

    wm(u)=π0k(a)sin(ma)ds.

    Surely, it is nonexpansive and strongly continuous semigroup in this Hilbert space. The linear operator Λ generates this semigroup such that Λu=¨u. Let for all kH, the set M(Λ) represent the maximal domain of Λ such that u and ¨u must be continuous. Also, u(0)=0=u(π). Now, consider the non-autonomous Cauchy problem:

    {h(t,ε)t =g(t)2h(t,ε)2ε,  t>0, 0επ,h(0,ε)=b(ε),h(t,0)=h(t,π)=0, t0,

    where b(.)H and g: R+[1,) are nonexpansive functions on R+. This function g is periodic, i.e., g(j+p)=g(j) for every jR+ and for some p1. Take the function

    K(t)=t0g(t)dt,

    then the property of evolution equations will be satisfied by the solution k(.) of the above non-autonomous Cauchy problem. Therefore,

    k(t)=A(t,h)k(h),

    where

    A(t,h)=T(K(t)K(h)),

    see Example 2.9b [35].

    As the function tert||h(t)|| is bounded for any r0 on the set of non-negative real numbers, we have

    0||A(t,0)u||2dt=2π0r=1wr2(u)e2r2K(t)dt=2πr=1wr2(u)0e2r2K(t)dt=||u||220e2r2K(t)dt||u||220e2K(t)dt.

    On the other side, we have

    0e2K(t)dt=b=0(b+1)cbce2K(t)dt=b=0c0e2K(bc+β)dβ=b=0e2bK(c)c0e2K(β)dβcb=0e2bK(c)=ce2K(c)e2K(c)1=W.

    Therefore, we have

    0||A(t,0)u||2dtW||u||22.

    By using Theorem 3.2 from [36], we have a(A)12C, where a(A) is the growth bound of the family A and C1. For more details, see [36].

    This shows that the evolution family on the Hilbert space H is nonexpansive, so Theorem 3.5 can be applied to such evolution families and will be helpful in finding its solution and uniqueness.

    Example 4.2. Let

    E(t,s)=t+1s+1

    be an evolution family on the space l3, then clearly the space l3 is not a Hilbert space, but it is reflexive. If we take its subfamily G(t,0)=t+1 then we still can apply our results to this subfamily. Let γm=1m2 and ζm=1m, then clearly

    limmγmζm=0,

    so by Theorem 3.5 we have the sequence of iteration

    τm=1m2τm1+(11m2)G(1m,0)τm0F(G),

    where 0 is the unique fixed point of the subfamily G.

    Open problem. We have an open problem for the readers that whether Lemmas 3.1 and 3.2 and Theorem 3.5 can be generalized to all periodic and non-periodic evolution families?

    The idea of semigroupos arise from the solution of autonomous abstract Cauchy problem while the idea of evolution family arise from the solution of non-autonomous abstrct Cauchy problem, which is more genreal than the semigroups. In [33], the strong convergence theorms for fixed points for nonexpansive semigroups on Hilbert spaces are proved. We generalized the results to a subfamily of an evolution family on a Hilbert space. These results may be come a gateway for many researchers to extends these ideas to the whole evolution family rather than the subfamily in future. Also these results are helpfull for the mathematician and others to use for existence and uniqeness of solution of non-autonomous abstarct Cauchy problems.

    The authors declare they have not used Artificial Intelligence (AI) tools in the creation of this article.

    The authors would like to thank the Deanship of Scientific Research at Umm Al-Qura University for supporting this work grant code: 23UQU4331214DSR003.

    The authors declare that they have no conflicts of interest.



    [1] K. R. Crounse, L. O. Chua, Methods for image processing and pattern formation in cellular neural networks: A tutorial, IEEE Trans. Circuits Syst. I, 42 (1995), 583–601. https://doi.org/10.1109/81.473566 doi: 10.1109/81.473566
    [2] Z. Lv, F. Sun, C. Cai, A new spatiotemporal chaotic system based on two-dimensional discrete system, Nonlinear Dyn., 109 (2022), 3133–3144. https://doi.org/10.1007/s11071-022-07585-2 doi: 10.1007/s11071-022-07585-2
    [3] V. I. Nekorkin, M. G. Velarde, Synergetic phenomena in active lattices: patterns, waves, solitons, chaos, Springer, 2002. https://doi.org/10.1007/978-3-642-56053-8
    [4] Y. Song, X. Zou, Spatiotemporal dynamics in a diffusive ratio-dependent predator–prey model near a Hopf–Turing bifurcation point, Comput. Math. Appl., 67 (2014), 1978–1997, 2014. https://doi.org/10.1016/j.camwa.2014.04.015 doi: 10.1016/j.camwa.2014.04.015
    [5] Y. Tao, W. Cui, Z. Zhang, Spatiotemporal chaos in multiple dynamically coupled map lattices and its application in a novel image encryption algorithm, J. Inf. Secur. Appl., 55 (2020), 102650. https://doi.org/10.1016/j.jisa.2020.102650 doi: 10.1016/j.jisa.2020.102650
    [6] C. Tian, On the pseudo-randomicity of discrete spatiotemporal systems, Int. J. Bifurcat. Chaos, 24 (2014), 1450013. https://doi.org/10.1142/s0218127414500138 doi: 10.1142/s0218127414500138
    [7] C. Tian, Chaos in the sense of Devaney for two-dimensional time-varying generalized symbolic dynamical systems, Int. J. Bifurcat. Chaos, 27 (2017), 1750060. https://doi.org/10.1142/s0218127417500602 doi: 10.1142/s0218127417500602
    [8] C. Tian, Hypercyclicity for a class of discrete spatiotemporal systems, Int. J. Bifurcat. Chaos, 27 (2017), 1750045. https://doi.org/10.1142/s0218127417500456 doi: 10.1142/s0218127417500456
    [9] C. Tian, G. Chen, Stability and chaos in a class of 2-dimensional spatiotemporal discrete systems, J. Math. Anal. Appl., 356 (2009), 800–815. https://doi.org/10.1016/j.jmaa.2009.03.046 doi: 10.1016/j.jmaa.2009.03.046
    [10] R. Chen, F. Zhang, L. Teng, X. Wang, Cross-image encryption algorithm based on block recombination and spatiotemporal chaos system, J. Opt., 52 (2023), 2109–2129. https://doi.org/10.1007/s12596-023-01104-1 doi: 10.1007/s12596-023-01104-1
    [11] E. Fornasini, A 2-D systems approach to river pollution modelling, Multidimens. Syst. Signal Process., 2 (1991), 233–265. https://doi.org/10.1007/bf01952235 doi: 10.1007/bf01952235
    [12] E. Fornasini, G. Marchesini, Doubly-indexed dynamical systems: State-space models and structural properties. Math. Syst. Theory, 12 (1978), 59–72. https://doi.org/10.1007/bf01776566 doi: 10.1007/bf01776566
    [13] J. Fritz, Partial Differential Equations, volume 1. Springer Science & Business Media, 1991. https://doi.org/10.1007/978-1-4419-1096-7_5
    [14] S. Liu, F. Sun, Spatial chaos-based image encryption design, Sci. China Ser. G, 52 (2009), 177–183. https://doi.org/10.1007/s11433-009-0032-2 doi: 10.1007/s11433-009-0032-2
    [15] Y. Ma, Y. Tian, L. Zhang, P. Zuo, Two-dimensional hyperchaotic effect coupled mapping lattice and its application in dynamic s-box generation, Nonlinear Dyn., 112 (2024), 17445–17476. https://doi.org/10.1007/s11071-024-09907-y doi: 10.1007/s11071-024-09907-y
    [16] R. Roesser, A discrete state-space model for linear image processing, IEEE Trans. Autom. Control, 20 (1975), 1–10. https://doi.org/10.1109/tac.1975.1100844 doi: 10.1109/tac.1975.1100844
    [17] F. Sun, S. Liu, Z. Li, Z. Lü, A novel image encryption scheme based on spatial chaos map, Chaos Soliton. Fract., 38 (2008), 631–640. https://doi.org/10.1016/j.chaos.2008.01.028 doi: 10.1016/j.chaos.2008.01.028
    [18] F. H. Willeboordse, The spatial logistic map as a simple prototype for spatiotemporal chaos, Chaos, 13 (2003), 533–540. https://doi.org/10.1063/1.1568692 doi: 10.1063/1.1568692
    [19] C. Yuan, S. Liu, Exact regions of oscillation for a mixed 2D discrete convection system, J. Differ. Equ. Appl., 21 (2015), 37–52. https://doi.org/10.1080/10236198.2014.979167 doi: 10.1080/10236198.2014.979167
    [20] K. Sarkar, S. Khajanchi, Spatiotemporal dynamics of a predator-prey system with fear effect, J. Franklin Inst., 360 (2023), 7380–7414. https://doi.org/10.1016/j.jfranklin.2023.05.034 doi: 10.1016/j.jfranklin.2023.05.034
    [21] E. M. Izhikevich, Dynamical systems in neuroscience, MIT Press, 2007. https://doi.org/10.7551/mitpress/2526.001.0001
    [22] L. Randriamihamison, A. K. Taha, About the singularities and bifurcations of double indices recursion sequences, Nonlinear Dyn., 66 (2011), 795–808. https://doi.org/10.1007/s11071-011-9952-2 doi: 10.1007/s11071-011-9952-2
    [23] M. L. Sahari, A. K. Taha, L. Randriamihamison, Stability and bifurcations in 2D spatiotemporal discrete systems, Int. J. Bifurcat. Chaos, 28 (2018), 1830026. https://doi.org/10.1142/s0218127418300264 doi: 10.1142/s0218127418300264
    [24] M. L. Sahari, A. K. Taha, L. Randriamihamison, Bifurcations in 2D spatiotemporal maps, Int. J. Bifurcat. Chaos, 31 (2021), 2150091. https://doi.org/10.1142/s0218127421500917 doi: 10.1142/s0218127421500917
    [25] M. L. Sahari, A. K. Taha, L. Randriamihamison, A note on the spectrum of diagonal perturbation of weighted shift operator, Le Matematiche, 74 (2019), 35–47, 2019. http://dx.doi.org/10.48550/arXiv.1609.05203 doi: 10.48550/arXiv.1609.05203
    [26] P. R. Halmos, Introduction to Hilbert space and the theory of spectral multiplicity, Courier Dover Publications, 2017. https://doi.org/10.2307/3608269
    [27] Y. A. Kuznetsov, I. A. Kuznetsov, Y. Kuznetsov, Elements of applied bifurcation theory, volume 112. Springer, 1998. https://doi.org/10.1007/978-1-4757-2421-9
    [28] I. Gumowski, C. Mira, Dynamique chaotique: Transformations ponctuelles, transition, ordre-désordre. Cepadues, 1980. https://doi.org/10.1002/zamm.19810611023
    [29] C. Mira, Chaos and fractal properties induced by noninvertibility of models in the form of maps, Chaos Soliton. Fract., 11 (2000), 251–262. https://doi.org/10.1016/s0960-0779(98)00291-4 doi: 10.1016/s0960-0779(98)00291-4
    [30] A. L. Shields, Weighted shift operators and analytic function theory, Math. Surv., 13 (1974), 49–128. https://doi.org/10.1090/surv/013/02 doi: 10.1090/surv/013/02
    [31] P. R. Halmos, A Hilbert space problem book, volume 19, Springer Science & Business Media, 2012. https://doi.org/10.1007/978-1-4684-9330-6
    [32] W. B. Gordon, Period three trajectories of the logistic map, Math. Mag., 69 (1996), 118–120. https://doi.org/10.1080/0025570x.1996.11996403 doi: 10.1080/0025570x.1996.11996403
    [33] M. H. Lee, Three-cycle problem in the logistic map and Sharkovskii's theorem, Acta Phys. Pol. B, 42 (2011). https://doi.org/10.5506/APhysPolB.42.1071 doi: 10.5506/APhysPolB.42.1071
    [34] M. H. Lee, Solving for the fixed points of 3-cycle in the logistic map and toward realizing chaos by the theorems of Sharkovskii and Li-Yorke, Commun. Theor. Phys., 62 (2014), 485. https://doi.org/10.1088/0253-6102/62/4/06 doi: 10.1088/0253-6102/62/4/06
    [35] P. Saha, S. H. Strogatz, The birth of period three, Math. Mag., 68 (1995), 42–47. https://doi.org/10.1080/0025570x.1995.11996273 doi: 10.1080/0025570x.1995.11996273
    [36] J. C. Cathala, H. Kawakami, C. Mira, Singular points with two multipliers, s1 = - s2 = 1, in the bifurcation curves of maps, Int. J. Bifurcat. Chaos, 2 (1992), 1001–1004. https://doi.org/10.1142/s0218127492000616 doi: 10.1142/s0218127492000616
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