Research article Special Issues

Some features of geological structure of the Shikotan Island (Lesser Kuril Arc)—A view from "Space"

  • In this paper, for the first time, we used Google Earth, an easily accessible method for obtaining geological information to study Shikotan Island (Lesser Kuril Arc). Google Earth flight mode made it possible to examine coastal cliffs on the island, which are inaccessible for hiking or walking, whereas 3-D visualization mode helped us study topographic features, tectonic dislocations, and sediment layering hidden by vegetation and soil, thereby significantly expanding understanding of the geologic structure of the island. Researchers conducting studies in the northwestern part of the island (Tat'yana Cape) discovered a previously unknown structure—a dike field. In the southern part, two thrust faults were identified: An unnamed peak and Tomari Mountain, previously considered a volcano. In the southwestern part of Shikotan Island, there are four unknown volcanic peaks. Together with the Notoro Volcano, they mark the rim of an interpreted caldera of a paleovolcano, which could have been the main unknown source of tuffaceous material for the Mesozoic-Cenozoic deposits of the Matakotanskaya, Malokuril'skaya, and Zelenovskaya Suites. It has been shown that the gabbroid massif of Tsunami Bay (northeastern part of the island) is an autochthonous (local) formation, and not allochthonous, that is, brought from the Pacific Ocean, as evidenced by an intrusive contact with the rocks of the Malokuril'skaya Suite. Despite these positive results, analysis of satellite images of Shikotan Island unexpectedly has not confirmed the existence of the Central Shikotan thrust fault, the largest previously mapped tectonic structure on the island. This work confirms that Google Earth is a very useful tool for geological research in remote areas.

    Citation: Evgeny P Terekhov, Anatoly V Mozherovsky. Some features of geological structure of the Shikotan Island (Lesser Kuril Arc)—A view from 'Space'[J]. AIMS Geosciences, 2024, 10(4): 907-917. doi: 10.3934/geosci.2024042

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  • In this paper, for the first time, we used Google Earth, an easily accessible method for obtaining geological information to study Shikotan Island (Lesser Kuril Arc). Google Earth flight mode made it possible to examine coastal cliffs on the island, which are inaccessible for hiking or walking, whereas 3-D visualization mode helped us study topographic features, tectonic dislocations, and sediment layering hidden by vegetation and soil, thereby significantly expanding understanding of the geologic structure of the island. Researchers conducting studies in the northwestern part of the island (Tat'yana Cape) discovered a previously unknown structure—a dike field. In the southern part, two thrust faults were identified: An unnamed peak and Tomari Mountain, previously considered a volcano. In the southwestern part of Shikotan Island, there are four unknown volcanic peaks. Together with the Notoro Volcano, they mark the rim of an interpreted caldera of a paleovolcano, which could have been the main unknown source of tuffaceous material for the Mesozoic-Cenozoic deposits of the Matakotanskaya, Malokuril'skaya, and Zelenovskaya Suites. It has been shown that the gabbroid massif of Tsunami Bay (northeastern part of the island) is an autochthonous (local) formation, and not allochthonous, that is, brought from the Pacific Ocean, as evidenced by an intrusive contact with the rocks of the Malokuril'skaya Suite. Despite these positive results, analysis of satellite images of Shikotan Island unexpectedly has not confirmed the existence of the Central Shikotan thrust fault, the largest previously mapped tectonic structure on the island. This work confirms that Google Earth is a very useful tool for geological research in remote areas.



    Neural networks (NNs) are computational models inspired by the neuronal structure of the human brain, which consists of numerous artificial neurons (also called nodes or units) that are connected to each other by connection weights. In recent years, various properties of NNs have been widely studied, such as stability [1,2,3] and synchronization [4,5]. It is usually described by a first-order differential equation, and it has been widely used in optimization, classification and solving nonlinear algebraic equations [6,7,8,9].

    Furthermore, when modeling the link between flux and current, integer order NNs containing inertial terms, also known as inertial neural networks (INNs), are commonly utilized. In [10,11], Babcock and Westervelt initially presented INN, a second-order differential equation. The inertial term is a key element in causing chaos. INN has received a lot of attention since its introduction and has produced some significant outcomes. Cui et al. investigated the stability of delayed INN with stochastic impulses via using the matrix measure method in [12]. Criteria to ensure exponential stability of INN with proportional delays was given in [13] through applying the non-reduced order method. Dong et al. [14] studied the synchronization between memristive INNs by designing a suitable controller. Mittag-Leffler stability of fractional delayed INN was explored in [15] by utilizing the properties of the Riemann-Liouville integral. Wei et al. analyzed the synchronization between memristive INNs via the interval matrix method in [16] and applied the theoretical results to the field of secret communication.

    Fractional-order inertia neural network (FOINN) is a new kind of NN model, that introduces the concept of fractional-order calculus and is better able to describe the dynamic characteristics of the nonlinear system [17,18]. Compared with traditional integer order NNs, FOINNs have better performance and applicability when dealing with nonlinear and complex systems. In practical applications, FOINN has a wide range of application prospects, such as a control system, signal processing and pattern recognition. In recent years, some important progress has been made on the stability and synchronization of FOINNs. In [19], the stability of FOINN with delay-dependent impulses were investigated by constructing Lyapunov-Krasovskii functions (LKFs). Peng and Jian analyzed the Mittag-Leffler synchronization of delayed FOINN under two different control strategies in [20], and obtained sufficient criteria for Mittag-Leffler synchronization between delayed FOINNs through the Lyapunov stability theory and fractional-order differential inequalities. Liu et al. established a class of synchronous control strategies based on the properties of FOINNs, and several conditions to achieve synchronization are given in [21].

    Finite-time stability (FTS) is the property that the system can reach a stable state and remain in that state for a finite period of time. For FOINNs, FTS is an important property, which determines whether the system can converge to a stable state in a finite time, and is of great significance for practical applications. When studying the FTS of FOINNs, it is necessary to consider the dynamic characteristics of the system, the topology of the network and the characteristics of fractional-order calculus. In addition, the time delays factors in the modeling process are also factors that affect the FTS of the system [22,23,24,25,26]. Time delays are usually expressed as certain terms in the differential equation that depend on the state of the system at a previous point in time. Time delays can make the dynamic behavior of the system complicated, even oscillating, unstable, or chaotic [27]. In the fields of control systems, biological systems, chemical reaction dynamics, etc., time delays often make stability analysis and control design of systems more difficult. The appearance of time delays may also cause the solution of differential equations to be no longer smooth, but to have a certain piecewise property, which brings challenges to both numerical solution and analysis.

    The vagueness can cause the solution of differential equation to become fuzzy or uncertain, which makes the analysis and prediction of the system behavior more difficult. In control systems, artificial intelligence, fuzzy control, and other fields, the existence of vagueness needs to be dealt with by special mathematical tools and methods in [28]. In order to better handle the fuzziness during operation, Yang et al. introduced fuzzy logic into NN models in [29]. Fuzzy logic not only maintains the connectivity between NN nodes, but also integrates the ability of low-level and high-level information processing of NN models. At present, many scholars have designed appropriate feedback control methods to realize the stability and synchronization of FOINNs. In [30], Aouiti et al. studied the stabilization of the fractional-order fuzzy inertial neural network (FOFINN) in finite time by designing nonlinear feedback controllers. Hu et al. explored the stability of complex-valued fractional-order NNs (FONNs) in finite time by designing nonlinear feedback controllers in [31]. By designing a segmented feedback control strategy, synchronization in finite time between fuzzy FONNs was investigated in [32]. In [30,31,32], the feedback control strategy based on system state is the most common and effective control method. However, for many real-world systems, traditional fixed parameter controllers may not effectively deal with the complexity, including nonlinearity, time-variability and uncertainty. Meanwhile, adaptive control technology can adapt to the changes of the system and improve the robustness and performance of the system. Moreover, in fuzzy systems, the dynamic characteristics of the system might not be accurately modeled or measured, which make it difficult to apply traditional control methods. Therefore, it is necessary to consider adaptive controllers in the controller design process of fuzzy NNs.

    Based on the above analysis, the main works and contributions of this paper are as follows:

    1) Based on FONNs, distributed delay and fuzzy factors are further considered in this paper, which is different from [30,33]. Additionally, the unbounded activation functions are considered in the model.

    2) Appropriate order reduction techniques are then employed to convert the model into a first-dimensional FONN model. In contrast to the strategy utilized in [34] to minimize the order of INN, our approach involves two positive parameters ϱi and ξi, which make the model more general.

    3) In order to achieve FTS of FOFINN, we design two different controllers, namely state feedback controller and adaptive controller, respectively. By selecting appropriate Lyapunov functions and combining inequality techniques with the FTS theorem, sufficient conditions for FTS of FOFINN models with mixed delays under two control strategies were obtained, and the settling time (ST) is calculated accordingly. Compared with feedback controllers designed in existing works [35,36], the coefficients in the controllers designed in this paper not only depend on constants, but also include functions which change with time.

    Finally, we provide the organizational structure of this article. In Section 2, we mainly introduce relevant definitions, assumptions, lemmas, and the NN models. In Section 3, we investigate the problem of FTS of FOFINN with mixed delays by designing delay dependent feedback controller and delay dependent adaptive controller. By using the fractional-order FST theorem, the ST to reach stable state that is independent of the initial value is obtained. Examples are given in Section 4 to verify the results in Theorems 3.1 and 3.2.

    Notations: R=(,+), R+=(0,+). Rn and Rn×m represent the space which combined by real valued n-dimensional vector and real valued n×m-dimensional matrices, respectively. Z+ is the set which contains all positive integers. and are fuzzy AND and fuzzy OR operations, respectively. || represents the Euclidean norm. In addition, for simplicity, we denote i=ni=1, i=ni=1, and i=ni=1.

    We review the relevant definitions and properties of fractional order calculus first.

    Definition 2.1. [34] The following is the definition of the Caputo fractional-order derivative with non-integer order μ of function y(t):

    Ct0Dμy(t)=1Γ(1μ)tt0y(t)(tζ)μdζ, (2.1)

    where μ(0,1), and

    Γ(t)=t0eζζt1dζ. (2.2)

    Definition 2.2. [31] The fractional-order integral of order μ(0,1) is defined as follows:

    tIμt0y(t)=1Γ(μ)tt0y(ζ)(tζ)1μdζ. (2.3)

    Remark 2.1. Due to the fact that the fractional derivative depends on the lower bound of the integral, compared to the integer derivative operator, the fractional derivative operator is a nonlocal operator.

    Definition 2.3. [37] System (2.8) is finite time stable if it is asymptotically stable in finite time, i.e., y(t)=0,t>T(y0), where T(y0) is called the settling time function (STF).

    Lemma 2.1. [33] If p(0,1) and κjR, then

    (nj=1|κj|)pnp1nj=1|κj|p. (2.4)

    Lemma 2.2. [33] For any 0<μ<1, α,β>0 such that

    C0DμV(t)αVν(t)βVε(t) (2.5)

    holds, where 0ν, ν<ε<1+2ν, then, system (2.8) will achieve FTS with following settling time

    T=[Γ(1+μ)β2ε2ν11+ν(1+ε)((V1+ν(t0)+(βα)1+νεν)1+ε1+ν(βα)1+εεν)]1μ. (2.6)

    Consider the FOFINN shown below.

    C0D2μςi(t)=aiC0Dμςi(t)biςi(t)+jcijζj(ςj(t))+jzijζj(ςj(tφj(t)))+jmijtHj(tϵ)ζj(ςj(ϵ))dϵ+jeijζj(ςj(tφj(t)))+jkijζj(ςj(tφj(t))), (2.7)

    where i,jZ+ and the term C0Dμ is called the inertial term; ai,bi>0, φj(t)>0 represents the delay function in the jth neuron, and φj(t) is bouned by P; cij,zij,mij,λij represent connection weights between the ith and jth neuron; eij and kij stand for the elements of the fuzzy feedback MIN template, and the fuzzy feedback MAX template, respectively; ζi() is the activation function; Hj() is the delay kernel.

    Take ˉςi(t)=ϱiC0Dμςi(t)+ξiςi(t), ϱi,ξiR+, then

    {C0Dμςi(t)=1ϱiˉςi(t)ξiϱiςi(t),C0Dμˉςi(t)=(ξiϱiai)ˉςi(t)+(aiξibiϱiξ2iϱi)ςi(t)+ϱi[jcijζj(ςj(t))+jzijζj(ςj(tφj(t)))+jmijtHj(tϵ)ζj(ςj(ϵ))dϵ+jeijζj(ςj(tφj(t)))+jkijζj(ςj(tφj(t)))], (2.8)

    where the initial values are given by ςi(s)=ˆϕ(s) and ˉςi(s)=ˆψ(s), s(,t0].

    Remark 2.2. The addition of fractional calculus greatly enhances the memory and genetic abilities of INN models. Compared with integer order INNs, FOINN has more significance to explore.

    Remark 2.3. Different with [34], parameters ϱi in the reduce order method can not only be taken as 1, but also other positive numbers. This makes the model more general.

    Remark 2.4. In existing literatures [34,35,38,39,40], models consider only included bounded time delays. However, when they come to unbounded time delays, the controllers designed in [34,35,38,39,40] exhibit some limitations. In addition, there is a lack of fuzzy logic in the current literature [37,41], so the controller designed for the addition of fuzzy logic cannot effectively handle the fuzziness present in the system.

    Remark 2.5. This paper relies on the reduced order technique during the analytical phase. Currently, two approaches are offered for analyzing the dynamic characteristics of INN models: The reduced order method and the non-reduced order method. The main advantage of the reduced order method over the non-reduced order method is that it converts the higher order differential equation into the lower order differential equation, which simplifies system analysis; however, the system's stability conditions require additional parameters to verify. For the non-reduced order method, there have been many pioneering results, such as [42,43,44,45]. The advantage of the non-reduced order method is that it directly analyzes the properties of INN by constructing Lyapunov functionals. The structure of the constructor is clear, but the derivation process is relatively complicated.

    We assume functions ζi() and Hi() meet the following assumptions.

    Assumption 2.1. For ζj(),j{1,2,,n}, Lj>0 such that

    |ζj(u)ζj(v)|Lj|uv|andζj(0)=0,

    where u,vR.

    Assumption 2.2. Bump functions Hj()>0, j=1,,n, and we have

    +0Hj(s)ds=1.

    Lemma 2.3. [23] Assume that u and v are two states of FOFINN (2.8), then,

    |jeijζj(u)jeijζj(v)|j|eij||ζj(u)ζj(v)|,|jkijζj(u)jkijζj(v)|j|kij||ζj(u)ζj(v)|.

    In this part, we will analyze the FTS of FOFINN by designing two new control strategies. The controlled system is as follows:

    {C0Dμςi(t)=1ϱiˉςi(t)ξiϱiςi(t)+ui,C0Dμˉςi(t)=(ξiϱiai)ˉςi(t)+(aiξibiϱiξ2iϱi)ςi(t)+ϱi[jcijζj(ςj(t))+jzijζj(ςj(tφj(t)))+jmijtHj(tϵ)ζj(ςj(ϵ))dϵ+jeijζj(ςj(tφj(t)))+jkijζj(ςj(tφj(t)))]+vi. (3.1)

    For simplicity, we introduce the following convenient notations, ςi(t)=ςi, ˉςi(t)=ˉςi, and ςi(tφi(t))=ςφi, ˉςi(tφi(t))=ˉςφi, ui=ui(t), vi=vi(t).

    To achieve the FTS of FOFINN (2.8), we design a feedback controller and have the following theorem.

    Theorem 3.1. Based on the Assumptions 2.1–2.2, the FOFINN (2.8) is said to achieve FTS under the following controller:

    {ui=ρi1ςiρi2sign(ςi)|ˉςφi|ρi3sign(ςi)|ςi|ρi4sign(ςi)|ςi|ϖ,vi=i1ˉςisign(ˉςi)jˉμij|ςφj|ϱijmijtHj(tϵ)ζj(ςj)dϵi3sign(ˉςi)|ˉςi|i4sign(ˉςi)|ˉςi|ϖ, (3.2)

    where i,j{1,,n},0, <ϖ<1+2, ρi3,ρi4,i3,i4 are positive constants, if the following conditions hold

    ρi1ξiϱi+|aiξibiϱiξ2iϱi|+jϱj|cji|Lj, (3.3)
    i11ϱi+ξiϱiai, (3.4)
    ˉμijϱi(|zij|+|eij|+|kij|)Lj, (3.5)
    ρi20. (3.6)

    In addition, the settling time is estimated by

    T=[Γ(1+μ)B2ϖ211+(1+ϖ)((V1+(t0)+(BA)1+ϖ)1+ϖ1+(BA)1+ϖϖ)]1μ, (3.7)

    where A=nmini{ρi3,i3}, B=nmini{ρi4,i4}.

    Proof. Take V=V(t)=i|ςi|+i|ˉςi|. Then, we have

    C0DμVisign(ςi)C0Dμςi+isign(ˉςi)C0Dμˉςiisign(ςi){1ϱiˉςiξiϱiςiρi1ςiρi2sign(ςi)|ˉςφi|ρi3sign(ςi)|ςi|ρi4sign(ςi)|ςi|ϖ}+isign(ˉςi){(ξiϱiai)ˉςi+(aiξibiϱiξ2iϱi)ςi+ϱi[jcijζj(ςj)+jzijζj(ςφj)+jeijζj(ςφj)+jkijζj(ςφj)]i1ˉςisign(ˉςi)jˉμij|ςφj|i3sign(ˉςi)|ˉςi|i4sign(ˉςi)|ˉςi|ϖ}. (3.8)

    Combined with Lemma 2.3 and Assumptions 2.1–2.2, we can obtain

    C0DμVi{1ϱi|ˉςi|ξiϱi|ςi|ρi1|ςi|ρi2|ˉςφi|ρi3|ςi|ρi4|ςi|ϖ}+i{(ξiϱiai)|ˉςi|+|aiξibiϱiξ2iϱi||ςi|+ϱi[j|cij|Lj|ςj|+j|zij|Lj|ςφj|+j|eij|Lj|ςφj|+j|kij|Lj|ςφj|]i1|ˉςi|jˉμij|ςφj|i3(t)|ˉςi|i4(t)|ˉςi|ϖ}. (3.9)

    From Lemma 2.1, we can get

    C0DμVi{1ϱi+ξiϱiaii1}|ˉςi|iρi2|ˉςφi|+i{ξiϱiρi1+aiξibiϱiξiϱi+jϱj|cji|Li}|ςi|+i{j[ϱi(|zij|+|eij|+|kij|)Ljˉμij]}|ςφj|iρi3(t)|ςi|iρi4(t)|ςi|ϖii3(t)|ˉςi|ii4(t)|ˉςi|ϖiρi3|ςi|iρi4|ςi|ϖii3|ˉςi|ii4|ˉςi|ϖnminiR+{ρi3,i3}[i(|ςi|+|ˉςi|)]nminiR+{ρi4,μi4}[i(|ςi|+|ˉςi|)]ϖAV(t)BV(t)ϖ. (3.10)

    From Lemma 2.2, we can obtain that FOFINN 3.1 could achieve FTS within the ST (3.7).

    Adaptive control provides techniques that adjust a controller for a system with parametric uncertainty, structural uncertainty, and environmental uncertainty, where fuzzy logic is the typical structural uncertainty. The adaptive controller can adaptively adjust the output values based on the current state of the system, which to some extent reduces the loss of control input. Thus, we design a type of adaptive controller to achieve the predetermined performance of FOFINN. On the basis of controller (3.2), we replace the control parameters ρi1 and i1 with variable parameters which related to the system states, then the controller becomes an adaptive controller. Hence, we have the following theorem.

    Theorem 3.2. Assume the Assumptions 2.1–2.2 and conditions (3.4)–(3.6), FOFINN (2.8) is said to be FTS under the following adaptive controllers

    {ui=|ρi1(t)|ςiρi2sign(ςi)|ˉςφi|ρi3sign(ςi)|ςi|ρi4sign(ςi)|ςi|ϖ,vi=|i1(t)|ˉςisign(ˉςi)jˉμij|ςφj|ϱijmijtHj(tϵ)ζj(ςj)dϵi3sign(ˉςi)|ˉςi|i4sign(ˉςi)|ˉςi|ϖ. (3.11)

    Additionally, the settling time is estimated by

    T=[Γ(1+μ)Υ22ϖ211+(1+ϖ)((V1+(t0)+1)1+ϖ1+1)]1μ, (3.12)

    where

    C0Dμρi1(t)=(ρi1(t)δsign(ρi1(t)))|ςi|ρi4sign(ρi1(t))|ρi1(t)|ρi3sign(ρi1(t))|ρi1(t)|ϖ, (3.13)
    C0Dμi1(t)=(i1(t)δsign(i1(t)))|ˉςi|i4sign(i1(t))|i1(t)|i3sign(i1(t))|i1(t)|ϖ, (3.14)

    and Υ1=nminiZ+{miniZ+{ρi3,i3},miniZ+{ρi4,i4}}, Υ2=Υ1, δmaxiZ+{1ϱi+ξiϱiai,ξiϱi+|aiξibiϱiξ2iϱi|+jϱj|cji|Li|}.

    Proof. In order to keep it simple, we denote ρi1=ρi1(t) and i1=i1(t), respectively. Take the following Lyapunov functional:

    V=V(ςi,ˉςi,ρi1,i1)=i(|ςi|+|ˉςi|+|ρi1|+|i1|). (3.15)

    Then, similarly to (3.8), we obtain

    C0DμVisign(ςi)C0Dμςi+isign(ˉςi)C0Dμˉςi+isign(ρi1)C0Dμρi1+isign(i1)C0Dμi1. (3.16)

    From the model (2.8), Lemma 2.1, Lemma 2.3, as well as (3.11), we have

    C0DμVisign(ςi){1ϱiˉςiξiϱiςi|ρi1(t)|ςiρi2sign(ςi)|ˉςφi|ρi3sign(ςi)|ςi|ρi4sign(ςi)|ςi|ϖ}+isign(ˉςi){(ξiϱiai)ˉςi+(aiξibiϱiξ2iϱi)ςi+ϱi[jcijζj(ςj)+juijζj(ςφj)+jeijζj(ςφj)+jkijζj(ςφj)]|i1(t)|ˉςisign(ˉςi)jˉμij|ςφj|i3sign(ˉςi)|ˉςi|i4sign(ˉςi)|ˉςi|ϖ}+isign(ρi1(t))((ρi1(t)δsign(ρi1(t)))|ςi|sign(ρi1(t))ρi4|ρi1(t)|sign(ρi1(t))ρi3|ρi1(t)|ϖ)+isign(i1(t))((i1(t)δsign(i1(t)))|ˉςi|sign(i1(t))i4|i1(t)|sign(i1(t))i3|i1(t)|ϖ)i{1ϱi|ˉςi|ξiϱi|ςi||ρi1(t)||ςi|ρi2|ˉςφi|ρi3|ςi|ρi4|ςi|ϖ}+i{(ξiϱiai)|ˉςi|+|aiξibiϱiξ2iϱi||ςi|+ϱij[|cij|Lj|ςj|+|uij|Lj|ςφj|+|eij|Lj|ςφj|+|kij|Lj|ςφj|]|i1||ˉςi|jˉμij|ςφj|i3|ˉςi|i4|ˉςi|ϖ}+i((|ρi1(t)|δ)|ςi|ρi4|ρi1(t)|ρi3|ρi1(t)|ϖ)+i((|i1(t)|δ)|ˉςi|i4|i1(t)|i3|i1(t)|ϖ). (3.17)

    Combine with conditions (3.3)–(3.6), we have

    C0DμVi{1ϱi+ξiϱiaiδ}|ˉςi|iρi2|ˉςφi|+i{ξiϱi+|aiξibiϱiξ2iϱi|+jϱj|cji|Li|δ}|ςi|+i{j[ϱi(|zij|+|eij|+|kij|)Ljˉμij]}|ςφj|iρi3|ςi|ii3|ˉςi|iρi4|ρi1(t)|ii4|i1(t)|iρi4|ςi|ϖii4|ˉςi|ϖiρi3|ρi1(t)|ϖii3|i1(t)|ϖΥ1VΥ2(t)Vϖ. (3.18)

    Hence, from Lemma 2.2, we can see that FOFINN (2.8) could achieve FTS within the settling time (3.12).

    Remark 3.1. Due to the inclusion of a time driven variable coefficients in the adaptive controller (3.11) that we designed, it is more flexible than the feedback controllers in [35,36]. At the same time, from Lemma 2.2, it can be found that the settling time can be estimated by adjusting the size of parameters μ, , and ϖ.

    Several numerical examples are given in this part to validate the results we obtained.

    Example 4.1. Take the following controlled FOFINN into consideration.

    {C0Dμz1(t)={1η1ˉz1(t)ξ1η1z1(t)}+u1,C0Dμz2(t)={1η2ˉz2(t)ξ2η2z2(t)}+u2,C0Dμˉz1(t)={(ξ1η1a1)ˉz1(t)+(a1ξ1b1η1ξ21η1)z1(t)+η1[jc1jζj(ςj(t))+jh1jζj(ςj(tφj(t)))+jm1jtHj(tϵ)ζj(ςj(ϵ))dϵ+je1jζj(ςj(tφj(t)))+jk1jζj(ςj(tφj(t)))]}+v1,C0Dμˉz2(t)={(ξ2η2a2)ˉz2(t)+(a2ξ2b2η2ξ22η2)z2(t)+η2[jc2jζj(ςj(t))+jh2jζj(ςj(tφj(t)))+jm2jtHj(tϵ)ζj(ςj(ϵ))dϵ+je2jζj(ςj(tφj(t)))+jk2jζj(ςj(tφj(t)))]}+v2, (4.1)

    where ϱi=[1,1], ξi=[1,1], ai=[2,2], bi=[3,3], cij=[3,2;5,1], zij=[0.7,0.5;0.3,0.9], mij=[0.6,0.3;0.5,0.6], eij=[0.3,0.4;0.5,0.6], kij=[0.7,0.9;0.8,0.5] and φi(t)=0.6exp(sin(t))+0.6exp(sin(t)), Hj(t)=exp(t).

    From Theorem 3.1, we can obtain that ˉμ111.7, ˉμ121.8, ˉμ211.6, ˉμ222, ρ117, ρ214, i10.

    Take ρ11=14, ρ21=9, ρ12=1.086, ρ22=2.5, 11=21=2, ˉμij=[3.7,3.8;3.6,4], ρ13=0.055, ρ23=0.135, ρ14(t)=0.09, ρ24(t)=0.026, 13=23=0.015, 14=0.016, 24=0.014, =0.7, ϖ=0.01, then, we can find that conditions (3.3)–(3.6) are all met. Therefore, the ST of controlled FOFINN (3.1) is

    T=[Γ(1+μ)B2ϖ211+(1+ϖ)((V1+(t0)+(BA)1+ϖ)1+ϖ1+(BA)1+ϖϖ)]1μ=45.1461. (4.2)

    Figures 1 and 2 show the state trajectory of FOINN (4.1) without controller and the values of delay function φj(t), respectively. We can find that FOFINN can converge to a stable state before 1.2. This further demonstrates the effectiveness of our designing controller.

    Figure 1.  States of FOFINN (4.1) without controllers.
    Figure 2.  Values of delay function φi(t).

    Figures 3 and 4 show the state of FOFINN (4.1) under feedback controller (3.2) and the values of controller (3.2). It can be observed that under controller (3.11), the state of FOFINN converges to a stable state before reaching the ST, i.e., FOFINN could achieve FTS. This also proves that the feedback controller (3.2) we designed is effective.

    Figure 3.  States of FOINN (4.1) under controller (3.2).
    Figure 4.  Values of controller (3.2).

    Example 4.2. We consider the same system as in Example 4.1 and consider the following adaptive controller:

    {ui=|ρi1(t)|ςiρi2sign(ςi)|ˉςφi|ρi3sign(ςi)|ςi|ρi4sign(ςi)|ςi|ϖ,vi=|i1(t)|ˉςisign(ˉςi)jˉμij|ςφj|ϱijmijtHj(tϵ)ζj(ςj)dϵi3sign(ˉςi)|ˉςi|i4sign(ˉςi)|ˉςi|ϖ, (4.3)

    where parameters ρi2, ρi3, ρi4, ˉμij, mij, ϱi, i3, i4 are the same as we take in Example 4.1, and

    C0Dμρi1(t)=(ρi1(t)δsign(ρi1(t)))|ςi|ρi4sign(ρi1(t))|ρi1(t)|ρi3sign(ρi1(t))|ρi1(t)|ϖ, (4.4)
    C0Dμi1(t)=(i1(t)δsign(i1(t)))|ˉςi|i4sign(i1(t))|i1(t)|i3sign(i1(t))|i1(t)|ϖ. (4.5)

    Take δ=10 and after verification, the conditions (3.3) and (3.6) are still met, so, from Lemma 2.2, the system can achieve FTS with the following ST:

    T=[Γ(1+μ)Υ22ϖ211+(1+ϖ)((V1+(t0)+1)1+ϖ1+1)]1μ=46.1001. (4.6)

    The state of FOFINN (4.1) under controller (3.11) is shown in Figure 5. We can find that FOFINN converges to a stable state before reaching ST. Due to the fact that the control parameters change with the state of FOFINN, the convergence speed to stable state is slower and the ST under adaptive controller (3.11) is larger than under feedback controller (3.2).

    Figure 5.  State of FOFINN under the controller (3.11).

    Figure 6 is the values of adaptive parameters ρ11(t), 11(t), ρ21(t), 21(t) in controller (3.11).

    Figure 6.  Values of adaptive parameters ρ11(t), ρ21(t), 11(t), 21(t).

    Remark 4.1. The symbol function in the controller will generate chattering effects in the control process, increasing the control cost. To avoid the buffeting effect, sign function can be replaced by function tanh().

    Remark 4.2. To the best of our knowledge, the stability of FOFINNs has scarcely been explored, particularly the fixed-time synchronization of such networks with mixed delay and neutral terms. Therefore, the findings presented in this paper are groundbreaking.

    Remark 4.3. In [30,46], authors previously required that activation functions be bounded. However, this paper removes the boundedness assumption, making our results more general and lessening the conservativeness of the derived stibility criteria to some extent. The results in this paper can be generalized to those in [30,46], but the opposite is not true.

    Remark 4.4. In [39,40,41], the criteria of FTS for integer order NNs have been obtained. We know that non-integer derivatives are more widely used than integer derivatives, so fractional derivatives are one of the factors that must be considered in modeling. In [47], the FTS criteria of memristor-based FONN are given based on the linear controller, but the calculation expression of the settling time is not given in detail. Compared to the results presented in [39,40,41,47], our results significantly enhance and broaden their theoretical outcomes to a certain extent.

    Remark 4.5. In the design of control systems and mechanical systems, the inertia term is an important part, which affects the dynamic response and stability of the system. In the recent results [26,27,31,32], the FTS of NN models with inertial terms is not analyzed. Compared to their results, our results are more general.

    Remark 4.6. Since the settling time of the system is derived according to the inequality techniques, there may be some errors in the estimation of the system settling time. In order to solve this problem, we can consider applying the less conservative inequality techniques.

    This paper delves into the FTS of FOFINNs with mixed delays. Leveraging the fractional-order FTS theorem, properties of fractional calculus, and inequality approaches, we derive some novel sufficient conditions to ensure the globally FTS of FOFINN. Additionally, we design two types of controllers, namely the feedback controller and adaptive controller, and compute the settling times for each controller. Finally, we provide two examples to validate our results. Future research will focus on designing more concise and easy to implement controllers to achieve FTS of FONNs.

    Tiecheng Zhang: Conceptualisation, writing - original draft, formal analysis, writing - review & editing; Liyan Wang: Methodology, software; Yuan Zhang: Supervision, validation; Jiangtao Deng: Writing - review & editing. All authors have read and approved the final version of the manuscript for publication.

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

    This research is supported by the Guiding Project for 2023 of Scientific Research Plan of Hubei Provincial Department of Education, the Open Subject for Teacher Education Research of Hubei Normal University (Grant No. 2022TEZ06), the Philosophy and Social Science Research Project of Hubei Provincial Department of Education (Grant No. 23Y122), Science Research Project of Hubei Normal University (Grant No. 2023046, 2023049), and Guiding Project of Hubei Provincial Department of Education's Scientific Research Program (Grant No. B2022187).

    The authors declare that there are no conflicts of interest regarding the publication of this paper.



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