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Let (Phi_{t}(X_{0})=Phi t,X_{0}):=(S t), e(cdot,t), i(cdot,t), T t))) be any nonnegative solution of system (1.4) with the boundary conditions (1.5) and the initial condition (1.6).
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Let be a nonnegative solution of (1.11).
Let u be a nonnegative solution of (1.1) and (1.2).
Under the assumption [IU] (i.e., the associated heat kernel is intrinsically ultracontractive), we establish an integral representation theorem: any nonnegative solution is represented uniquely by an integral on (D×{0})∪(∂MD×[0,T)), where ∂MD is the Martin boundary of D for the associated elliptic operator.
Moreover, is a nonnegative solution to (2.19).
Thus is a nonnegative solution of (1.1)−(1.4).
Assume that holds, and is a nonnegative solution of (1.11).
By Lemma 2.2, is a nonnegative solution of (1.5).
Hence ( λ, U ) is a nonnegative solution of (3.25).
Assume that and is a nonnegative solution of (1.11).
Thus, u is a nonnegative solution of (1 -(4).
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com