Abstract
We study a class of Lotka–Volterra stochastic differential equations with continuous and pure-jump noise components, and derive conditions that guarantee the strong stochastic persistence (SSP) of the populations engaged in the ecological dynamics. More specifically, we prove that, under certain technical assumptions on the jump sizes and rates, there is convergence of the laws of the stochastic process to a unique stationary distribution supported far away from extinction. We show how the techniques and conditions used in proving SSP for general Kolmogorov systems driven solely by Brownian motion must be adapted and tailored in order to account for the jumps of the driving noise. We provide examples of applications to the case where the underlying food-web is: (a) a 1-predator, 2-prey food-web, and (b) a multi-layer food-chain.
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Acknowledgements
I would like to thank my Ph.D. adviser Dr. Rolando Rebolledo for his supportive and attentive guidance during the preparation of the first draft of this article.
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The author has been supported by ANID, ex-CONICYT, through Beca de Doctorado Nacional, 21170406, convocatoria 2017. This research was partially funded by project ANID-FONDECYT 1200925. The author declares that has no financial or personal relationship with other people or organizations that could inappropriately influence or bias the content of this paper.
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Leonardo Videla has been supported by CONICYT through Beca de Doctorado 21170406, Convocatoria 2017. This research was partially funded by project ANID-FONDECYT 1200925.
Appendix: Deferred proofs
Appendix: Deferred proofs
Proof of Lemma 1
Since \((\mathbf{A}, \mathbf{B})\) is feasible, consider the vector \(\mathbf{c}\) given by Definition 1. We will prove that there exists positive constants \(K_1\), \(K_2\) such that:
for every \(\mathbf{x}\in {\mathbb {R}}^n_{+}\). Indeed:
where we have used Jensen’s inequality to obtain the last line. Thus:
Of course, there exists \(R> 0\) such that \(\Vert \mathbf{x}\Vert > R\) implies \(\dfrac{1}{\sum _{i=1}^{n}x_i} < 1\). Define \(\tilde{K}_1= \dfrac{ \max _{i=1, \ldots , n} \left\{ c_i b_i \right\} }{\min _{i=1, \ldots , n} c_i}\) and \(K_2= \dfrac{\min _{i=1, \ldots , n} \left\{ c_i a_{ii} \right\} }{n (1+\max _{i=1,\ldots , n} c_i)} \). Thus, for \(\Vert \mathbf{x}\Vert > R\), we have:
Observe that the right hand side is a continuous function of \(\mathbf{x}\). Let:
Then, (48) holds with \(K_1:=\max \{\tilde{K}_1, r_1+r_2\}\). \(\square \)
Proof of Lemma 2
Let \(V: {\mathbb {R}}^n_{++} \mapsto {\mathbb {R}}_{+}\) be the function defined by:
where \(c_i\) are the constant guaranteed by Assumption 1. Then V is log-Lyapunov and for \(\mathbf{x}\in {\mathbb {R}}^n_{++}\):
By Assumption 2, Taylor’s theorem, and Assumption 3, the last term is bounded above. Moreover, since the intraspecies interaction are negative, we have that the above expression is not grater than:
for some positive constants \(K_1, K_2, K_3\). Now, the last sum is non-negative, by definition of feasibility. In toto, thus, there exist positive constants \(K_1\), \(K_2\), \(K_3\) such that:
We conclude that there exists a constant \(M> 0\) such that on \({\mathbb {R}}^n_{++}\):
If we set:
then
Since V is continuous, \(V_k\) is open, and thus
is a \({\mathcal {F}}_t\)-stopping time. Dynkin’s formula applied to V gives:
Fix \(N \in {\mathbb {N}}\), and consider the set:
Define:
Observe that for every \(k \ge 1\):
where the second-to-last line follows from the fact that \(\mathbf{X}\) has right-continuous a.s. paths and by the relation (51). This last inequality and (52) gives:
and thus necessarily \(\epsilon _N={\mathbb {P}}_{\mathbf{X}_0}(\varOmega _N)=0\) for every \(N \in {\mathbb {N}}\). Consequently,
and this concludes the proof. \(\square \)
Recall that \((P_t: t\ge 0)\) is the semigroup associated to the process \(\mathbf{X}\), i.e.,
for bounded measurable real functions f.
Proof of Lemma 3
Let \(F_{i}(\mathbf{x})=x_{i} (B_i+\sum _{j=1}^n A_{ij}x_j ) \), \(G_{i}(\mathbf{x})= x_{i}\sigma _{i}\), and \(H_i(\mathbf{x}, \mathbf{z})= x_i L_{i}(\mathbf{x}, \mathbf{z})\). For two initial conditions \(\mathbf{x}, \mathbf{y}\), let \(\ {^\mathbf{x}}{\tilde{\mathbf{X}}}{}\) and \(\ {^\mathbf{y}}{\tilde{\mathbf{X}}}{}\) be the solutions of (2) in the natural coupling, i.e., driven by the same Lévy noise \((\mathbf{W}, \tilde{N})\). Let \(D_{k}:= \{\mathbf{x}\in {\mathbb {R}}^n_+: \Vert \mathbf{x}\Vert \le k\}\), and set \(\eta _k:=\inf \{ t\ge 0: \ {^\mathbf{x}}{\tilde{\mathbf{X}}}{_t} \in D^C_k \text { or } \ {^\mathbf{y}}{\tilde{\mathbf{X}}}{_t} \in D^C_k \}\). For \(\mathbf{u}=\mathbf{x}\text { or } \mathbf{y}\) define:
Observe that \(\mathbf{F}=(F_{1}, F_2, \ldots , F_n) \) is locally Lipschitz continuous, and thus for every \(k\in {\mathbb {N}}\) there exist a constant \(M_k\) such that for \(\mathbf{x}, \mathbf{y}\in D_k\):
Fix \(T\ge 0\). For any time \(0 \le t \le T\) define \(t_{k}:= t \wedge \eta _k\). For \(t \le T_k\):
Cauchy-Schwartz inequality yields:
On \(s \le T_k\), by (53) we have that:
and trivially, for \(s \le T_k\):
Let \(\tilde{M}_1\) be a Lipschitz constant for G . By Burkholder-Davis-Gundy inequality, Lipschitz-continuity of G and Fubini’s theorem:
Analogously, for the jump component, we have:
where the constant \(\tilde{M}_2\) is guaranteed by Assumption3(c). Thus, if we take supremum on \(0 \le t \le T_{k}\) and then take expectation at both sides of the inequality (54), we obtain:
where C is a universal constant and \((C_k: k\ge 0)\) is an increasing positive sequence. We conclude by Gromwall’s Lemma that:
Now, let \(f: {\mathbb {R}}^n_{+} \mapsto {\mathbb {R}}\) be a bounded continuous function, and fix \(\mathbf{x}\in {\mathbb {R}}^n_{+}\), \(t \ge 0\), \(\varepsilon > 0\). Let \(r > 0\) such that \( \bar{B} ( \mathbf{x}, r ) \subset {\mathbb {R}}^n_{++}\). Plainly, for \(\mathbf{y}\in \bar{B} ( \mathbf{x}, r)\):
On the other hand, observe that from inequality (52), we deduce that for \(\mathbf{y}\in \bar{B}(\mathbf{x}, r)\):
and thus, we can choose a \(k_0\) such that uniformly on \(\mathbf{y}\in \bar{B} (\mathbf{x}, r)\), we have:
Since f is continuous, it is uniformly continuous on \(D_{k_0}\). Let \(\delta : {\mathbb {R}}_{+} \mapsto {\mathbb {R}}_{+}\) be a modulus of continuity of f on \(D_{k_0}\), i.e. a function that satisfies that for every \(\mathbf{y}_0 \in D_k\), \(f(B(\mathbf{y}_0, \delta (\varepsilon )) \cap D_k) \subseteq B (f(\mathbf{y}_0), \varepsilon )\). Let \(\varDelta = \delta (\varepsilon /3)\). Then, again for \(\mathbf{y}\in \bar{B} (\mathbf{x}, r)\):
Using (56) and Markov’s Inequality, the last term is not greater than \( \Vert \mathbf{x}-\mathbf{y}\Vert ^2 \dfrac{2 C \Vert f \Vert e ^{C_k t}}{\varDelta ^2} \) and this is smaller than \(\varepsilon /3\) for every \(\mathbf{y}\) in the open ball \(B \left( \mathbf{x}, r \wedge \dfrac{\sqrt{\varepsilon }\varDelta }{\sqrt{6 C \Vert f \Vert e^{C_{k}t}}} \right) \). The result follows. \(\square \)
Proof of Lemma 9
For fixed \(\alpha > 0\) set \(\varrho (\alpha ; \mathbf{x})= \exp \{\alpha (1+\mathbf{c}^T \mathbf{x}) \}\). An easy computation shows that:
Fix \(\alpha _1> 0\) such that for \(i=1, \ldots , n\):
and observe that for every \(0 \le \alpha \le \alpha _1\), our choice of the \(c_i\), Assumptions 3 and 5 imply that for every \(\delta > 0\) there exists \(M> 0\) such that:
whenever \(\alpha \) is small enough. Just as in the proof of Lemma 5, Dynkin’s formula yields:
for \(0 \le \alpha \le \alpha _1\). Consider the random variables \(\ {^\mathbf{x}}{U}{_t} = \varrho (\alpha _1, \ {^\mathbf{x}}{\mathbf{X}}{_t})\). Since \(\varrho (\alpha ; \cdot )\) is continuous, De la Vallée Poussin’s Lemma implies that for every compact set \(K \subset {\mathbb {R}}^n_{+}\) and \(T > 0\) the family:
is a uniformly integrable (UI) family of random variables, written:
Now, by our assumptions on \(\mathbf{L}\):
for some positive constant C. Consequently, there exists \(\alpha _0\) such that for \(\alpha < \alpha _0\):
Consequently, there exists \(R_1\) such that whenever \(\varrho (\alpha _1, \mathbf{x})> R_1\) and \(\alpha < \alpha _0\):
Next, consider a sequence \((\mathbf{x}_{k})\) converging to \(\mathbf{x}\in {\mathbb {R}}^n_{+}\), and set \(\varepsilon > 0\). Fix \(T > 0\). Since \(\mathbf{x}_{k}\) is convergent, there exists a compact set K containing \((\mathbf{x}_k)\) and \(\mathbf{x}\). By the UI property (60), there exists \(R_2 >0\) such that for every \(\mathbf{y}\in K\) and \(0 \le t \le T\):
Fix \(R_3 = \max \{R_1, R_2\}\), and let \(\eta : {\mathbb {R}}^n_{+}\mapsto [0,1]\) be a smooth function such that \(\eta (\mathbf{x})=1\) for \(\varrho (\alpha _1; \mathbf{x})< R_3\) and \(\eta (\mathbf{x})=0\) for \(\varrho (\alpha _1; \mathbf{x}) > 2 R_3\). Now, for \(\alpha < \alpha _0\), \(0\le t \le T\) and \(k \in {\mathbb {N}}\):
The \({\mathcal {C}}_b\)-Feller property (Lemma 3) applies to the first term on the right, and thus there exist a \(k_0 > 0\) such that for every \(k \ge k_0\) it is smaller that \(\varepsilon /2\). As for the second term, observe that:
Of course, an analogous inequality holds for the terms \({\mathbb {E}}_{\mathbf{x}_k}(\cdot )\). This concludes the proof.
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Videla, L. Strong stochastic persistence of some Lévy-driven Lotka–Volterra systems. J. Math. Biol. 84, 11 (2022). https://doi.org/10.1007/s00285-022-01714-6
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DOI: https://doi.org/10.1007/s00285-022-01714-6
Keywords
- Ecological models
- Stochastic Lotka–Volterra systems
- Lévy-driven SDE
- Strong stochastic persistence
- Food-chains