
Predicting the risk of mortality of hospitalized patients in the ICU is essential for timely identification of high-risk patients and formulate and adjustment of treatment strategies when patients are hospitalized. Traditional machine learning methods usually ignore the similarity between patients and make it difficult to uncover the hidden relationships between patients, resulting in poor accuracy of prediction models. In this paper, we propose a new model named PS-DGAT to solve the above problem. First, we construct a patient-weighted similarity network by calculating the similarity of patient clinical data to represent the similarity relationship between patients; second, we fill in the missing features and reconstruct the patient similarity network based on the data of neighboring patients in the network; finally, from the reconstructed patient similarity network after feature completion, we use the dynamic attention mechanism to extract and learn the structural features of the nodes to obtain a vector representation of each patient node in the low-dimensional embedding The vector representation of each patient node in the low-dimensional embedding space is used to achieve patient mortality risk prediction. The experimental results show that the accuracy is improved by about 1.8% compared with the basic GAT and about 8% compared with the traditional machine learning methods.
Citation: Manfu Ma, Penghui Sun, Yong Li, Weilong Huo. Predicting the risk of mortality in ICU patients based on dynamic graph attention network of patient similarity[J]. Mathematical Biosciences and Engineering, 2023, 20(8): 15326-15344. doi: 10.3934/mbe.2023685
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Predicting the risk of mortality of hospitalized patients in the ICU is essential for timely identification of high-risk patients and formulate and adjustment of treatment strategies when patients are hospitalized. Traditional machine learning methods usually ignore the similarity between patients and make it difficult to uncover the hidden relationships between patients, resulting in poor accuracy of prediction models. In this paper, we propose a new model named PS-DGAT to solve the above problem. First, we construct a patient-weighted similarity network by calculating the similarity of patient clinical data to represent the similarity relationship between patients; second, we fill in the missing features and reconstruct the patient similarity network based on the data of neighboring patients in the network; finally, from the reconstructed patient similarity network after feature completion, we use the dynamic attention mechanism to extract and learn the structural features of the nodes to obtain a vector representation of each patient node in the low-dimensional embedding The vector representation of each patient node in the low-dimensional embedding space is used to achieve patient mortality risk prediction. The experimental results show that the accuracy is improved by about 1.8% compared with the basic GAT and about 8% compared with the traditional machine learning methods.
r-d: right dense; l-d: left dense; r-s: right scattered; l-s: left scattered; UPS: uniform practical stability; SUPS: strongly uniform practical stability; LF: Lyapunov function; CFrΔD: Caputo fractional delta derivative; CFrΔDiD: Caputo fractional delta Dini derivative; GLFrΔD: Grunwald–Letnikov fractional delta derivative; GLFrΔDiD: Grunwald–Letnikov fractional delta Dini derivative; CFrDyT: Caputo fractional dynamic equations on time scales; CFrD: Caputo fractional derivative
In the field of dynamic systems, stability analysis is essential for understanding system responses to various initial conditions and disturbances. Traditional Lyapunov stability theory has made significant contributions here, focusing on convergence to the equilibrium [1,2]. However, this strict convergence requirement can be overly restrictive in real-world applications where slight deviations are often tolerable. UPS offers a more flexible framework, allowing systems to operate within an acceptable range around the equilibrium rather than requiring exact convergence (see [3,4]).
The recent growth of fractional calculus has introduced valuable tools for stability analysis. By extending differentiation and integration to arbitrary order, fractional calculus has proven to be highly effective in modeling complex systems with memory effects and non-local interactions [5,6,7]. Among these tools, the Caputo fractional derivative (CFrD) has shown practical relevance for various applications (see [8,9]). However, most studies have relied on scalar Lyapunov functions (LFs), which evaluate stability on an individual-variable basis [10,11]. It is widely recognized that as the complexity of a dynamical system increases, identifying a suitable LF becomes more challenging. This difficulty often leads to the use of multiple LFs, forming a vector LF, where each component reveals insights into different parts of the system's behavior. By this approach, certain complex elements can be simplified into interconnected subsystems, allowing for more relaxed conditions. Thus, the method of vector LFs provides a highly adaptable framework for analysis [12,13,14].
Previous studies, including [15,16,17], have concentrated largely on stability aspects like uniform, asymptotic, and variational stability within delay and impulsive settings, primarily for continuous-time systems. In contrast, research such as [] has examined stability in discrete settings. This paper introduces an innovative approach using vector LFs for Caputo fractional dynamic equations on time scales (CFrDyT), establishing UPS in terms of two measures (m0,m), and presenting a versatile framework well-suited for real-world applications. This approach ensures that systems remain within specific bounds despite small disturbances, reflecting a balance between rigorous stability and practical adaptability.
With the introduction of time scale calculus in [19], a unified approach for analyzing systems evolving in both discrete and continuous time domains has emerged, extending traditional continuous analysis techniques to discrete cases. Integrating this calculus with fractional dynamics enables a more sophisticated framework for understanding systems that undergo both gradual and abrupt changes, common in hybrid systems. When combined with fractional calculus, time scale calculus provides a versatile platform for analyzing dynamic behaviors in both continuous and discrete settings.
Building on these advancements, this paper extends the results in [20,21], presenting a novel methodology for examining the (m0,m)-uniform practical stability (UPS) and (m0,m)-strongly uniform practical stability (SUPS) of CFrDyT. To further extend the scope of practical stability analysis [22], this work applies the novel derivatives introduced in [23], the Caputo fractional delta derivative (CFrΔD) and Caputo fractional delta Dini derivative (CFrΔDiD) of order ζ∈(0,1), which enables unified stability analysis, creating a robust framework for hybrid systems exhibiting both gradual and abrupt changes.
Let us examine the system
CΔζy=D(t,y), t∈T,y(t0)=y0,t0≥0. | (1.1) |
Here,
D∈Crd[T×RN,RN] |
is a function satisfying
D(t,0)≡0, |
and CΔζy denotes the CFrΔD of y∈RN of order ζ. Let
y(t)=y(t,t0,y0)∈Cζrd[T,RN] |
represent a solution of (1.1). Assuming that the function D possesses sufficient smoothness to ensure the existence, uniqueness, and continuous dependence of solutions (see [24,25]), this paper examines the (m0,m)-UPS and (m0,m)-SUPS of the system (1.1).
To achieve this, we use the comparison system of the form
CΔζκ=Θ(t,κ), κ(t0)=κ0≥0, | (1.2) |
where
Θ∈Crd[T×Rn+,Rn+]. |
The system (1.2) is a simpler system of lesser dimension than (1.1), whose qualitative properties including the existence and uniqueness of its solution
κ(t)=κ(t;t0,κ0) |
and practical stability are already known or easy to find, see [26].
The structure of this research is outlined as follows: In Section 2, necessary terminologies, key definitions, remarks, and foundational lemmas that support the later developments are given. In Section 3, we develop and give details of core findings and theoretical contributions of our research. In Section 4, we present practical examples to illustrate the relevance and applicability of our approach. Lastly, in Section 5, we present a summary of the main findings and discuss their implications.
Definition 2.1. [27] If t∈T, then
ϖ(t)=inf{s∈T:s>t} |
is called the forward jump operator and
ρ(t)=sup{s∈T:s<t} |
is called the backward jump operator. So that t∈T is said to be: right dense (r-d) if
ϖ(t)=t, |
right scattered (r-s) if ϖ(t)>t, left dense (l-d) if ρ(t)=t, and left scattered if ρ(t)<t. Also the function
τ(t)=ϖ(t)−t |
is called the graininess function.
Definition 2.2. [28] A function
h:T→R |
is said to be r-d continuous represented by Crd, if it remains continuous at every r-d point in T, and has finite left-sided limits at each l-d point of T.
Definition 2.3. [28] We define the following class of functions:
K={ψ∈[[0,r],[0,∞)]}: ψ(t) is strictly increasing on [0,r] and ψ(0)=0;
CK={a∈Crd[T×R+,R+]:a(t,s)∈K for each t};
M={m∈Crd[T×Rn,R+]:inf(t,x)m(t,x)=0}.
We now define the derivative of LF utilizing the CFrΔDiD as presented in [23].
Definition 2.4. Let
[t0,T)T=[t0,T)∩T, |
where T>t0. Then a Lyapunov-like function
ℷ(t,y)∈Crd[T×RN,RN+] |
is defined as the generalized CFrΔDiD relative to (1.1) as follows: given ϵ>0, there exists a neighborhood P(ϵ) of t∈T such that
1τζ{ℷ(ϖ(t),y(ϖ(t))−ℷ(t0,y0)−[t−t0τ]∑ι=1(−1)ι+1(ζCι)[ℷ(ϖ(t)−ιτ,y(ϖ(t)−τζD(t,y(t))−ℷ(t0,y0)]}<CΔζ+ℷ(t,y)+ϵ, |
for each s∈P(ϵ) and s>t, and
y(t)=y(t,t0,y0) |
is any solution of (1.1), where 0<ζ<1, ϖ is the forward jump operator as defined in Definition 2.1,
τ=ϖ−t, ζCι=ζ(ζ−1)...(ζ−ι+1)ι! |
and [(t−t0)τ] denotes the integer part of the fraction (t−t0)τ.
Definition 2.5. [23] Using Definition 2.6, we state the CFrΔDiD of the LF ℷ(t,y) as
CΔζ+ℷ(t,y)=lim supτ→0+1τζ[[t−t0τ]∑ι=0(−1)ι(ζCι)[ℷ(ϖ(t)−ιτ,y(ϖ(t))−τζD(t,y(t))−L(t0,y0)]], | (2.1) |
which is equivalent to
CΔζ+ℷ(t,y)=lim supτ→0+1τζ{ℷ(ϖ(t),y(ϖ(t))−ℷ(t0,y0)−[t−t0τ]∑ι=1(−1)ι+1(ζCι)[ℷ(ϖ(t)−ιτ,y(ϖ(t))−τζD(t,y(t))−ℷ(t0,y0)]} |
and
CΔζ+ℷ(t,y)=lim supτ→0+1τζ{ℷ(ϖ(t),y(ϖ(t))+[t−t0τ]∑ι=1(−1)ι(ζCι)[ℷ(ϖ(t)−ιτ,y(ϖ(t))−τζD(t,y(t))]}−ℷ(t0,y0)(t−t0)−ζΓ(1−ζ), | (2.2) |
where t∈T, and y,y0∈Rn, and
y(ϖ(t))−τζD(t,y)∈RN. |
For discrete times, Eq (2.1) becomes
CΔζ+ℷ(t,y)=1τζ[[t−t0τ]∑ι=0(−1)ι(ζCι)(ℷ(ϖ(t),y(ϖ(t)))−ℷ(t0,y0))], |
and for continuous times (T=R), Eq (2.1) becomes
CΔζ+ℷ(t,y)=CDζ+ℷ(t,y)=lim supκ→0+1κζ{ℷ(t,y(t))−ℷ(t0,y0)−[t−t0κ]∑ι=1(−1)ι+1(ζCι)[ℷ(t−ικ,y(t))−κζD(t,y(t))−ℷ(t0,y0)]}. | (2.3) |
Notice that (2.3) is the same in [5], where κ>0.
Definition 2.6. Let
y(t)=y(t;t0,y0) |
be any solution of (1.1), then system (1.1) is said to be:
(UP1) (m0,m)-uniformly practically stable if, given (λ,A)∈R+ with 0<λ<A, we have m0(t0,y0)<λ implies m(y(t))<A, ∀ t0∈T;
(UP2) (m0,m)-uniformly practically quasi-stable if given (λ,B,T)>0 and t0∈T, we have m0(t0,y0)<λ ⟹ m(y(t))<B, for t≥t0+T;
(UP3) (m0,m)-SUPS if (UP1) and (UP2) hold together.
Definition 2.7. Corresponding to Definition 2.6, the solution
κ(t)=κ(t;t0,κ0) |
of (1.2), is called uniformly practically stable if given 0<λ<A, we have
n∑i=1κ0<λ⟹n∑i=1κi(t;t0,κ0)<A, t≥t0, | (2.4) |
for some t0∈T∩R+.
Lemma 2.1. [23] Let
R,B∈Crd[T,Rn]. |
Assume ∃ t1>t0, with
t1∈T:R(t1)=B(t1) |
and
R(t)<B(t) |
for t0≤t<t1. If the CFrΔDiD of R and B are defined at t1, then the inequality
CΔζ+R(t1)>CΔζ+B(t1) |
holds.
Lemma 2.2. (Comparison theorem) Let
(i) Θ∈Crd[T×Rn+,Rn+] and Θ(t,κ)τ is non-decreasing in κ.
(ii) ℷ(t,y)∈Crd[T×RN,RN+] be locally Lipschitzian in y and
CΔζ+ℷ(t,y)≤Θ(t,ℷ(t,y)),(t,y)∈T×RN. |
(iii) ϱ(t)=ϱ(t;t0,κ0) be the maximal solution of (1.2) existing on T.
Then
ℷ(t,y(t))≤ϱ(t),t≥t0 | (2.5) |
provided that
ℷ(t0,y0)≤κ0, |
where
y(t)=y(t;t0,y0) |
is any solution of (1.1), t∈T, t≥t0.
Proof. We shall make this proof by the principle of induction. For an assertion
S(t):ℷ(t,y(t))≤ϱ(t),t∈T, |
the following holds:
(i) S(t0) is true since ℷ(t0,y0)≤κ0.
(ii) Assuming t is r-s and S(t) is true. Then we prove that S(ϖ(t)) is true; i.e.,
ℷ(ϖ(t),y(ϖ(t)))≤ϱ(ϖ(t)), | (2.6) |
set
ϰ(t)=ℷ(t,y(t)), |
and then
ϰ(ϖ(t))=ℷ(ϖ(t),y(ϖ(t))), |
then from Definition 2.6, we obtain
CΔζ+ϰ(t)=lim supτ→0+1τζ{[(t−t0)τ]∑ι=0(−1)ιζCι[ϰ(ϖ(t)−ιτ)−ϰ(t0)]}, |
also,
CΔζ+ϱ(t)=lim supτ→0+1τζ{[(t−t0)τ]∑ι=0(−1)ιζCι[ϱ(ϖ(t)−ιτ)−ϱ(t0)]},t≥t0, |
then,
CΔζ+ϱ(t)−CΔζ+ϰ(t)=lim supτ→0+1τζ{[(t−t0)τ]∑ι=0(−1)ιζCι[ϱ(ϖ(t)−ιτ)−ϱ(t0)]}−lim supτ→0+1τζ{[(t−t0)τ]∑ι=0(−1)ιζCι[ϰ(ϖ(t)−ιτ)−ϰ(t0)]},(CΔζ+ϱ(t)−CΔζ+ϰ(t))τζ=lim supτ→0+{[(t−t0)τ]∑ι=0(−1)ιζCι[[ϱ(ϖ(t)−ιτ)−ϱ(t0)]−[ϰ(ϖ(t)−ιτ)−ϰ(t0)]]}≤[ϱ(ϖ(t))−ϱ(t0)]−[ϰ(ϖ(t))−ϰ(t0)]≤[ϱ(ϖ(t))−ϰ(ϖ(t))]−[ϱ(t0)−ϰ(t0)], |
then,
[ϱ(ϖ(t))−ϰ(ϖ(t))]≥(CΔζ+ϱ(t)−CΔζ+ϰ(t))τζ+[ϱ(t0)−ϰ(t0)], |
so that,
[ϰ(ϖ(t))−ϱ(ϖ(t))]≤(CΔζ+ϱ(t)−CΔζ+ϰ(t))τζ+[ϰ(t0)−ϱ(t0)]≤(Θ(t,ϰ(t))−Θ(t,ϱ(t)))τζ+[ϰ(t0)−ϱ(t0)]. |
By the non-decreasing property of Θ(t,κ)τ and since S(t) is true, then
ϰ(ϖ(t))−ϱ(ϖ(t))≤0, |
so Eq (2.6) holds.
(iii) For r-d points t∗∈U, where U is a right neighborhood t∈T. We can clearly see that S(t∗) is true immediately from [5, Lemma 3] since at every r-d point of T, ℷ(t,y(t)) is continuous and the domain is R.
(iv) Let t be l-d, and let S(s) be true for all s>t. We want to show that S(t) is true. This immediately follows r-d continuity of ℷ(t,y(t)), y(t), and the maximal solution ϱ(t). Thus, by the principle of induction, the assertion S(t) holds for all t∈T, thereby concluding the proof.
The proof is completed.
Now, we present the (m0,m)-UPS and (m0,m)-SUPS results for the fractional dynamic system (1.1).
Theorem 3.1. ((m,m0)-UPS) Assume that
(m1) 0<λ<A;
(m2) m0,m∈M, and m0 is uniformly finer than m, implying m(t,y)≤ϕ(m0(t,y)), ϕ∈K, whenever m0(t,y)<λ;
(m3) There exists
ℷ∈Crd[T×RN,RN+] |
and
Q∈Crd[Rn+,Rn+], |
such that if
Q(ℷ(t,y))≡V(t,y), |
V(t,y) is locally Lipschitz in y, and for
(t,y)∈S(m,A)={(t,y)∈T×RN:m(t,y)<A}, |
then,
b(m(t,y))≤n∑i=0Vi(t,y),ifm(t,y)<A∞∑0Vi(t,y)≤a(m0(t,y)),ifm0(t,y)<λ; | (3.1) |
(m4) for (t,y)∈S(m,A)
CΔζ+V(t,y)≤Θ(t,V(t,y)), | (3.2) |
where
Θ∈Crd[T×Rn+,Rn+], |
Θ(t,κ) is quasimonotone nondecreasing in κ with
Θ(t,κ)≡0, |
a∈CK, and for each i, 1≤i≤n, Θi(t,κ)τ(t)+κi is nondecreasing in κ for all t∈T;
(m5) ϕ(λ)<A and a(λ)<b(A) hold;
Then the UPS properties of (1.2) imply the corresponding (m0,m)-UPS properties of (1.1).
Proof. Since (1.2) is UPS, then we deduce from (2.4) that ∀ t0∈T and 0<λ<A,
n∑i=0κ0i<a(λ)⟹n∑i=1κi(t;t0,κ0)<b(A), t≥t0. | (3.3) |
We can easily assert that (1.1) is (m,m0)-UPS with respect to (λ,A).
However, if the assertion were false, then for any solution
y(t)=y(t;t0,y0) |
of (1.1) with
m0(t0,y0)<λ, |
there would be a point t1>t0 such that
m(t1,y(t1))=Aandm(t,y(t))≤Afort∈[t0,t1). | (3.4) |
Setting
κ0i=Vi(t,y0), |
and from (2.5), we have
V(t,y(t))≤ϱ(t,t0,κ0), | (3.5) |
where ϱ(t) is the maximal solution of (1.2).
Also, from assumptions (m2) and (m5), it is clear to see that
m(t0,y0)≤ϕ(m0,(t0,y0))<ϕ(λ)<A. |
Then, we deduce that,
n∑i=1κ0i<∞∑0Vi(t0,y0)≤a(m0(t0,y0))<a(λ). | (3.6) |
Combining (3.3)–(3.6), we obtain
b(A)=b(m(t1,y(t1)))≤n∑i=1Vi(t1,y(t1))≤n∑i=1ϱi(t1;t0,κ0)<b(A). | (3.7) |
Equation (3.7) is a contradiction, so the statement that (1.1) is (m0,m)-UPS is true.
Theorem 3.2. ((m,m0)-SUPS) Assume that conditions (m1)–(m4) of Theorem 3.1 is satisfied, and Eq (1.2) is SUPS; then, Eq (1.1) is (m,m0)-SUPS.
Proof. To make this proof, we need (1.1) to be (m0,m)-UPS and (m0,m)-uniformly practically quasi-stable together. Now, (1.1) is (m0,m)-UPS by Theorem 3.1, so we need to prove only (m0,m)-uniform practical quasi-stability. By the assumption of the theorem, Eq (1.2) is (m0,m)-SUPS for
(a(λ),b(λ),b(B),T)>0, |
so that for all t0∈T,
n∑i=1κ0i<a(λ)⟹n∑i=1κi(t,t0,κ0)<b(B),t≥t0+T, | (3.8) |
where κi(t,t0,κ0) is any solution of (1.2). By the UPS of (1.2), we can comfortably make the assumption that
m0(t0,y0)<λ, |
so that
m(t,y(t))<A |
for t≥t0. Setting
κ0i=Vi(t0,y0), |
and by Lemma 2.2, we have the estimate
V(t,y(t))≤ϱ(t,t0,κ0), | (3.9) |
where ϱ(t) is the maximal solution of (1.2). Following this argument closely, and from (3.8) and (3.9), we obtain
b(m(t,y(t)))≤n∑i=1Vi(t,y(t))≤n∑i=1ϱi(t,t0,κ0)<b(B),t≥t0+T. |
So that
m(t,y(t))<B |
whenever
m0(t0,y0)<λ, |
for t≥t0+T. Therefore, we conclude that (1.1) is (m0,m)-SUPS.
Given the following system
CΔζ℘1(t)=−2℘1−℘21exp(℘1)−℘22exp(℘1),CΔζ℘2(t)=−℘21exp(℘2)−2℘2−℘22exp(℘2), | (4.1) |
with initial conditions
℘1(t0)=℘10 |
and
℘2(t0)=℘20, |
for
(℘1,℘2)∈R2. |
Choose the LF for (4.1) to be
ℷ=(V1,V2)T, |
where
V1(t,℘1,℘2)=|℘1| |
and
V2(t,℘1,℘2)=|℘2|. |
Using (2.5), the CFrΔDiD for
V1(t,℘1,℘2)=|℘1| |
is computed as
CΔζ+V1(t,℘1)=lim supτ→0+1τζ{V1(ϖ(t),℘1(ϖ(t))+[t−t0τ]∑ι=1(−1)ι(ζCι)[V1(ϖ(t)−ιτ,℘1(ϖ(t))−τζD1(t,℘1(t))]}−V1(t0,℘10)(t−t0)−ζΓ(1−ζ)=lim supτ→0+1τζ{|℘1(ϖ(t))|+[t−t0τ]∑ι=1(−1)ι(ζCι)[|℘1(ϖ(t))−τζD1(t,℘1)|]}−|℘10|(t−t0)−ζΓ(1−ζ)≤lim supτ→0+1τζ{|℘1(ϖ(t))|+[t−t0τ]∑ι=1(−1)ι(ζCι)[|℘1(ϖ(t))|+|τζD1(t,℘1)|]}−|℘10|(t−t0)−ζΓ(1−ζ)≤lim supτ→0+1τζ{|℘1(ϖ(t))|+[t−t0τ]∑ι=1(−1)ι(ζCι)|℘1(ϖ(t))|+[t−t0τ]∑ι=1(−1)ι(ζCι)|τζD1(t,℘1)|}−|℘10|(t−t0)−ζΓ(1−ζ)≤|℘1(ϖ(t))|lim supτ→0+1τζ[t−t0τ]∑ι=0(−1)ι(ζCι)+|D1(t,℘1)|lim supτ→0+[t−t0τ]∑ι=1(−1)ι(ζCι)−|℘10|(t−t0)−ζΓ(1−ζ). |
Applying (2.12) and (2.14) in [23], we obtain
CΔζ+V1(t,℘1)=|℘1(ϖ(t))|(t−t0)−ζΓ(1−ζ)−|D1(t;℘1)|−|℘10|(t−t0)−ζΓ(1−ζ),CΔζ+V1≤|℘1(ϖ(t))|(t−t0)−ζΓ(1−ζ)−|D1(t;℘1)|. |
When
t→∞, |℘1(ϖ(t))|(t−t0)−ζΓ(1−ζ)→0, |
then
CΔζ+V1≤−|D1(t;℘1)|=−[|−2℘1−℘21exp(℘1)−℘22exp(℘1)|]=−[|−2℘1−(℘21+℘22)exp(℘1)|]≤−[|−2℘1|]≤−[2|℘1|],CΔζ+V1≤−2V1+0V2. | (4.2) |
Similarly, compute the CFrΔDiD for
V2(t,℘1,℘2)=|℘2|=lim supτ→0+1τζ{|℘2(ϖ(t))|+[t−t0τ]∑ι=1(−1)ι(ζCι)[|℘2(ϖ(t))−τζD2(t,℘2)|]}−|℘20|(t−t0)−ζΓ(1−ζ)≤lim supτ→0+1τζ{|℘2(ϖ(t))|+[t−t0τ]∑ι=1(−1)ι(ζCι)[|℘2(ϖ(t))|+|τζD2(t,℘2)|]}−|℘20|(t−t0)−ζΓ(1−ζ)≤lim supτ→0+1τζ{|℘2(ϖ(t))|+[t−t0τ]∑ι=1(−1)ι(ζCι)|℘2(ϖ(t))|+[t−t0τ]∑ι=1(−1)ι(ζCι)|τζD2(t,℘2)|}−|℘20|(t−t0)−ζΓ(1−ζ)≤|℘2(ϖ(t))|lim supτ→0+1τζ[t−t0τ]∑ι=0(−1)ι(ζCι)+|D2(t,℘2)|lim supτ→0+[t−t0τ]∑ι=1(−1)ι(ζCι)−|℘20|(t−t0)−ζΓ(1−ζ). |
Applying (2.12) and (2.14) in [23], we obtain
CΔζ+V2≤|℘2(ϖ(t))|(t−t0)−ζΓ(1−ζ)−|D2(t;℘2)|. |
When
t→∞, |℘2(ϖ(t))|(t−t0)−ζΓ(1−ζ)→0, |
then,
CΔζ+V2≤−|D2(t;℘2)|=−[|−℘21exp(℘2)−2℘2−℘22exp(℘2)|]=−[|−2℘2−(℘21−℘22)exp(℘2)|]≤−[|−2℘2|]≤−2|℘2|. |
Therefore,
CΔζ+V2≤0V1−2V2. | (4.3) |
From (4.2) and (4.3), it follows that
CΔζ+ℷ≤(−200−2)(V1V2)=Θ(t,V). | (4.4) |
Next, we choose a comparison system
CΔζ+κ=Θ(t,κ)=Mκ | (4.5) |
with
M=(−200−2). |
Clearly, Figure 1 below shows the stability of system (4.5). The vector inequality (4.4), along with all the other requirements of Theorem 3.1, holds when the matrix M has eigenvalues with negative real parts. Given that the eigenvalues of M are both −2, it can be concluded that (4.1) is not only (m,m0)-UPS but also (m,m0)-SUPS.
Given the following system
CΔζℵ1(t)=4ℵ1−ℵ22+3ℵ23ℵ1,CΔζℵ2(t)=−3ℵ21+ℵ2+4ℵ2−ℵ23ℵ2,CΔζℵ3(t)=−ℵ21ℵ3+3ℵ3, | (4.6) |
with initial conditions
ℵ1(t0)=ℵ10,ℵ2(t0)=ℵ20,andℵ3(t0)=ℵ30, |
for
ℵ=(ℵ1,ℵ2,ℵ3)∈R3. |
Choose a vector LF
ℷ=(V1,V2,V3)T:V1=ℵ21, V2=ℵ22, V3=ℵ23 |
and
ℷ0(ℵ1,ℵ2,ℵ3)=2∑i=1Vi(ℵ1,ℵ2,ℵ3)=ℵ21+ℵ22+ℵ23. |
Computing the CFrΔDiD for
V1=ℵ21, |
we obtain:
CΔζ+V1=lim supτ→0+1τζ{[(ℵ1(ϖ(t)))2]−[(ℵ10)2]+[t−t0τ]∑ι=1(−1)ι(ζCι)[(ℵ1(ϖ(t))−τζD1(t,ℵ))2]−[((ℵ10)2]}=lim supτ→0+1τζ{[(ℵ1(ϖ(t)))2]−[(ℵ10)2]+[t−t0τ]∑ι=1(−1)ι(ζCι)[(ℵ1(ϖ(t)))2−2ℵ1(ϖ(t))τζD1(t,ℵ1,ℵ2,ℵ3)+τ2ζ(D1(t,ℵ1,ℵ2,ℵ3))2]−[(ℵ10)2]}=−lim supτ→0+1τζ{[t−t0τ]∑ι=0(−1)ι(ζCι)[(ℵ10)2]}+lim supτ→0+1τζ{[t−t0τ]∑ι=0(−1)ι(ζCι)[(ℵ1(ϖ(t)))2]}−lim supτ→0+{[t−t0τ]∑ι=1(−1)ι(ζCι)[2ℵ1(ϖ(t))τζD1(t,ℵ1,ℵ2,ℵ3)]}. |
From (2.12) and (2.14) in [23], we obtain
CΔζ+V1≤(t−t0)−ζΓ(1−ζ)[(ℵ1(ϖ(t)))2]−[2ℵ1(ϖ(t))D1(t,ℵ1,ℵ2,ℵ3)]. |
When
t→∞, (t−t0)−ζΓ(1−ζ)[(ℵ1(ϖ(t)))2]→0, |
so that we obtain
CΔζ+V1≤−2[ℵ1(ϖ(t))D1(t,ℵ1,ℵ2,ℵ3)]. |
Using
ℵ(ϖ(t))≤τCΔζℵ(t)+ℵ(t), |
we obtain
CΔζ+V1=−2[τ(t)D21(t,ℵ1,ℵ2,ℵ3)+ℵ1(t)D1(t,ℵ1,ℵ2,ℵ3)]=−2[τ(t)(4ℵ1−ℵ22+3ℵ23ℵ1)2+ℵ1(4ℵ1−ℵ22+3ℵ23ℵ1)]=−2τ(t)[(4ℵ1−ℵ22+3ℵ23ℵ1)2]−2ℵ1[4ℵ1−ℵ22+3ℵ23ℵ1]. | (4.7) |
If T=R then τ=0, reducing (4.7) to the form
CΔζ+V1(ℵ1,ℵ2,ℵ3)=−2ℵ1[4ℵ1−ℵ22+3ℵ23ℵ1]=−8ℵ21+2ℵ22+6ℵ23=(−8 2 6)⋅(V1 V2 V3)T. | (4.8) |
When T=N0 then, τ=1, reducing (4.7) to
CΔζ+V1(ℵ1,ℵ2,ℵ3)=−2[(4ℵ1−υ22+3ℵ23ℵ1)2]−2ℵ1[4ℵ1−ℵ22+3ℵ23ℵ1]≤−2ℵ1[4ℵ1−ℵ22+3ℵ23ℵ1], |
resulting in the same outcome as (4.8). Evidently, this applies to any other discrete time as well.
Also, computing the CFrΔDiD for
V2(ℵ)=ℵ22, |
we obtain:
CΔζ+V2(ℵ)=lim supτ→0+1τζ{[(ℵ2(ϖ(t)))2]−[(ℵ20)2]+[t−t0τ]∑ι=1(−1)ι(ζCι)[(ℵ2(ϖ(t))−τζD2(t,ℵ))2]−[(ℵ20)2]}=lim supτ→0+1τζ{[(ℵ2(ϖ(t)))2]−[(ℵ20)2]+[t−t0τ]∑ι=1(−1)ι(ζCι)[(ℵ2(ϖ(t)))2−2ℵ2(ϖ(t))τζD2(t,ℵ1,ℵ2,ℵ3)+τ2ζ(D2(t,ℵ1,ℵ2,ℵ3))2]−[(ℵ20)2]}=−lim supτ→0+1τζ{[t−t0τ]∑ι=0(−1)ι(ζCι)[(ℵ20)2]}+lim supτ→0+1τζ{[t−t0τ]∑ι=0(−1)ι(ζCι)[(ℵ2(ϖ(t)))2]}−lim supτ→0+{[t−t0τ]∑ι=1(−1)ι(ζCι)[2ℵ2(ϖ(t))τζD2(t,ℵ1,ℵ2,ℵ3)]}. |
From (2.12) and (2.14) in [23], we obtain
CΔζ+V2(ℵ)≤(t−t0)−ζΓ(1−ζ)[(ℵ2(ϖ(t)))2]−[2ℵ2(ϖ(t))D2(t,ℵ1,ℵ2,ℵ3)]. |
When
t→∞, (t−t0)−ζΓ(1−ζ)[(ℵ2(ϖ(t)))2]→0, |
so that
CΔζ+V2(ℵ)≤−2[ℵ2(ϖ(t))D2(t,ℵ1,ℵ2,ℵ3)], |
using
ℵ(ϖ(t))≤τCΔζℵ(t)+ℵ(t), |
we obtain
CΔζ+V2(ℵ)=−2[τ(t)D22(t,ℵ1,ℵ2,ℵ3)+ℵ2(t)D2(t,ℵ1,ℵ2,ℵ3)]=−2[τ(t)(−3ℵ21+ℵ2+4ℵ2−ℵ23ℵ2)2+ℵ2(−3ℵ21+ℵ2+4ℵ2−ℵ23ℵ2)]=−2τ(t)[(−3ℵ21+ℵ2+4ℵ2−ℵ23ℵ2)2]−2ℵ1[−3ℵ21+ℵ2+4ℵ2−ℵ23ℵ2]. | (4.9) |
If T=R, then τ=0, reducing (4.9) to
CΔζ+V2(ℵ1,ℵ2)=−2ℵ2[−3ℵ21+ℵ2+4ℵ2−ℵ23ℵ2]=6ℵ21−8ℵ22+ℵ23=(6 −8 1)⋅(V1 V2 V3)T. | (4.10) |
When T=N0, then τ=1, and (4.9) reduces to:
CΔζ+V2(ℵ)=−2[(−3ℵ21+ℵ2+4ℵ2−ℵ23ℵ2)2]−2ℵ1[−3ℵ21+ℵ2+4ℵ2−ℵ23ℵ2]≤−2ℵ1[−3ℵ21+ℵ2+4ℵ2−ℵ23ℵ2], |
resulting in (4.10).
Finally, for the CFrΔDiD of
V3(ℵ1,ℵ2,ℵ3)=ℵ23, |
we obtain
CΔζ+V3=lim supτ→0+1τζ{[(ℵ3(ϖ(t)))2]−[(ℵ30)2]+[t−t0τ]∑ι=1(−1)ι(ζCι)[(ℵ3(ϖ(t))−τζD3(t,ℵ))2]−[(ℵ30)2]}=lim supτ→0+1τζ{[(ℵ3(ϖ(t)))2]−[(ℵ30)2]+[t−t0τ]∑ι=1(−1)ι(ζCι)[(ℵ3(ϖ(t)))2−2ℵ3(ϖ(t))τζD3(t,ℵ1,ℵ2,ℵ3)+τ2ζ(D3(t,ℵ1,ℵ2,ℵ3))2]−[(ℵ30)2]}=−lim supτ→0+1τζ{[t−t0τ]∑ι=0(−1)ι(ζCι)[(ℵ30)2]}+lim supτ→0+1τζ{[t−t0τ]∑ι=0(−1)ι(ζCι)[(ℵ3(ϖ(t)))2]}−lim supτ→0+{[t−t0τ]∑ι=1(−1)ι(ζCι)[2ℵ3(ϖ(t))τζD3(t,ℵ1,ℵ2,ℵ3)]}. |
From (2.12) and (2.14) in [23], we obtain
CΔζ+V3≤(t−t0)−ζΓ(1−ζ)[(ℵ3(ϖ(t)))2]−[2ℵ1(ϖ(t))D3(t,ℵ1,ℵ2,ℵ3)]. |
As
t→∞, (t−t0)−ζΓ(1−ζ)[(ℵ3(ϖ(t)))2]→0, |
then
CΔζ+V3≤−2[ℵ3(ϖ(t))D3(t,ℵ1,ℵ2,ℵ3)]. |
Using
ℵ(ϖ(t))≤τCΔζℵ(t)+ℵ(t), |
we obtain
CΔζ+V3=−2[τ(t)D23(t,ℵ3,ℵ2,ℵ3)+υ3(t)D3(t,ℵ1,ℵ2,ℵ3)]=−2[τ(t)(−ℵ21ℵ3+3ℵ3)2+ℵ3(−ℵ21ℵ3+3ℵ3)]=−2τ(t)[(−ℵ21ℵ3+3ℵ3)2]−2ℵ3[−ℵ21ℵ3+3ℵ3]. | (4.11) |
If T is continuous, then τ=0, and (4.11) reduces to:
CΔζ+V3(ℵ1,ℵ2,ℵ3)=−2ℵ3[−ℵ21ℵ3+3ℵ3]=2ℵ21−6ℵ23=(2 0 −6)⋅(V1 V2 V3)T. | (4.12) |
Otherwise, for discrete T τ=1, (4.11) reduces to:
CΔζ+V3=−2[(−ℵ21ℵ3+3ℵ3)2]−2ℵ1[−ℵ21ℵ3+3ℵ3]≤−2ℵ1[−ℵ21ℵ3+3ℵ3], |
then we also obtain (4.12).
From (4.8), (4.10), and (4.12), we obtain
CΔζ+V≤(−8266−8120−6)(V1V2V3)=Θ(t,V). | (4.13) |
Next, we choose a comparison system of the form
CΔζ+κ=Θ(t,κ)=Mκ |
with
M=(−8266−8120−6). |
The vector inequality (4.13), along with all the conditions outlined in Theorems 3.1 and 3.2, hold true if the matrix M has eigenvalues with negative real parts. Given that the eigenvalues of M are
λ1=−12.433,λ2=−7.199,λ3=−2.369, |
it follows that (4.6) is uniformly practically stable. Thus, we conclude that system (4.6) exhibits UPS.
In conclusion, this paper develops a unified approach for UPS analysis of CFrDyT, utilizing vector LFs and a two-measure framework. By applying the CFrΔD and the CFrΔDiD, this study extends stability analysis methods across both continuous and discrete domains, making it versatile for hybrid systems exhibiting both gradual and abrupt changes. The use of vector LFs over scalar LFs enables a broader and more robust stability analysis, accommodating complex system dynamics with improved precision and adaptability. Illustrative examples, Eqs (4.1) and (4.6), demonstrate the practical application of the proposed framework, underscoring its effectiveness and relevance in capturing the essential stability characteristics of fractional dynamic systems. This work offers significant contributions to stability theory by enhancing the tools available for fractional dynamic systems, with implications for fields such as engineering, control theory, and applied sciences.
Michael Ineh: conceptualization, methodology, software, formal analysis, writing—original draft preparation, writing—review and editing; Umar Ishtiaq: conceptualization, validation, investigation, resources, visualization, funding acquisition; Jackson Ante: conceptualization, methodology, supervision; Mubariz Garayev: validation, investigation, resources, visualization, funding acquisition; Ioan-Lucian Popa: conceptualization, software, validation, investigation, project administration. All authors have read and agreed to the published version of the manuscript.
The authors declare they have not used Artificial Intelligence (AI) tools in the creation of this article.
The authors extend their appreciation to King Saud University for funding this work through Researchers Supporting Project number (RSPD2025R1056), King Saud University, Riyadh, Saudi Arabia.
The authors declare that they have no conflicts of interest.
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