Aug 2026· Mathematical methods in the applied sciences· Vol 49, pp. 17405 - 17419· 0 citations· 27 references
Abstract
To address the limitations of classical fishery population models (e.g., Ricker and Beverton–Holt) in capturing complex interspecific interactions and lag effects, this article constructs an improved two‐species, discrete dynamic model, y n + 1 = a y n 1 + p z n e − y n , z n + 1 = b z n 1 + q y n e − z n $$ {y}_{n+1}=\frac{a{y}_n}{1+p{z}_n}{e}^{-{y}_n},\kern1em {z}_{n+1}=\frac{b{z}_n}{1+q{y}_n}{e}^{-{z}_n} $$ where the parameters a , b , p , q $$ a,b,p,q $$ are positive real numbers and the initial values y 0 , z 0 $$ {y}_0,{z}_0 $$ are arbitrary nonnegative real numbers. We rigorously analyze the dynamic behaviors of the system, establishing that positive solutions are uniformly bounded and strictly persistent under specific intrinsic growth conditions ( a > 1 $$ a>1 $$ and b > 1 $$ b>1 $$ ). Furthermore, we provide a comprehensive classification of the boundary dynamics, exploring non‐hyperbolic and 1:1 resonant scenarios. We derive sufficient conditions for global asymptotic stability (GAS): (1) the trivial fixed point (extinction) is GAS via direct inequality bounding when intrinsic growth rates satisfy a < 1 $$ a<1 $$ and b < 1 $$ b<1 $$ , and (2) utilizing the mean value theorem (MVT) and Lyapunov function methods, the unique positive fixed point (coexistence) is GAS when growth rates lie within the non‐chaotic range ( 1 < a , b ≤ e $$ 1
Let $(ξ_n)^∞_{n=0}$ be a Markov chain with the state space $\chi = \{1, 2, · · · , b\},$ $(g_n(x, y))^∞_{n=1}$ be functions defined on $\chi \times \chi,$ and $$F_{m_n,b_n} (\omega) =\frac{1}{b_n}\sum\limits_{k=m_n+1}^{m_n+b_n}g_k(ξ_{k−1}, ξ_k).$$ In this paper the limit properties of $F_{m_n,b_n}(\omega)$ and the gene...
P. Hu, Zhong-Zhi Wang· Annals of Applied Mathematic...· 0 citations
We consider $n\times n$ covariance matrices $M=\frac{1}{n}XX^*$ where $X=(x_{i,j})$ is a matrix whose entries are independent complex random variables with $\mathbb{E}(x_{i,j})=0$ and $\mathbb{E}(|x_{i,j}|^2)=1$. We derive a $\frac{1}{n}$ expansion of the mixed moments, $\frac{1}{n}\mathbb{E}(\Tr(M^{(r_1)}\cdots M^{(r_...
The problem of finding and classifying integrable equations of the form $u^{j+1}_{n,x}=F(u^{j}_{n,x},u^{j+1}_{n},u^{j}_{n+1},u^{j}_{n},u^{j+1}_{n-1})$ with three independent variables is discussed. The presence of two discrete variables poses additional challenges for the study of such models within the known approache...
I. Habibullin, A. Khakimova· Sbornik. Mathematics· 0 citations
Let $(X_1,\ldots,X_n)$ be a random variable in $(\mathbb{R}\setminus\{0\})^n$ that is both exchangeable and sign-invariant. For every $k\in[n]$, let $S_k=\sum_{i=1}^kX_i$. Define the weak persistence probability as $\mathbb{P}(S_1,\ldots,S_n\geq0)$, and the strong persistence probability as $\mathbb{P}(S_1,\ldots,S_n>0...
Let $W_{N,N+\lambda}$ have the Laguerre unitary distribution with size $N$ and real shape $\lambda\ge0$. For $s>0$, we consider the normalized moment $$C_{s,\lambda}(N)=N^{-s-1}\mathbb{E}[\operatorname{Tr}W_{N,N+\lambda}^{s}]$$ and its dimension decrement $\Gamma_{N,s,\lambda}=C_{s,\lambda}(N)-C_{s,\lambda}(N+1)$. Iter...
We study the behavior at infinity of the invariant Radon measure for the multidimensional affine stochastic recursion $V_n = A_n V_{n-1} + B_n,$ where $(A_n)_{n \geq 1}$ are positive random matrices, $(B_n)_{n \geq 1}$ are random vectors with nonnegative entries, and $(A_n, B_n)_{n \geq 1}$ are independent and identica...
Ion Grama, Sebastian Mentemeier, Hui Xiao· 0 citations
We use cookies to run the site and, with your consent, for analytics and to show ads.
See our Cookie Policy.