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Moreover, we present the existence and nonexistence of a solution to the second problem in terms of the parameter λ by the properties of the Green function and the Guo-Krasnosel'skii theorem.
Even if we would just assume without any immediate physical motivation that the noise term in (43) is purely additive ϵ d W t ( x ), there is a problem to apply Kramers' law since we do not have a structure like in (22) with G = Id as W t ( x ) is a Q-Wiener process defined in (5) and driving space-time white noise in (4) is particularly excluded due to the nonexistence of a solution.
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Moreover, they also studied the nonexistence of a positive solution.
Moreover, the nonexistence of a positive solution is also studied.
Furthermore, the interval of α about the nonexistence of a positive solution is also given.
Nonexistence of a positive solution was also proved when a ≤ λ 1.
First, we show the nonexistence of a positive solution of (1.6) for small λ.
In this section we study the nonexistence of a global solution for the initial value problem (1).
In this section, we give some sufficient conditions for the nonexistence of a positive solution to boundary value problem (1.2).
The nonexistence of a positive solution boundary value problem for a class nonlinear fractional difference equations with 3 < α ≤ 4 is considered in terms of parameter.
The nonexistence of a global solution for nonlinear partial differential equations, which arises from the Liouville type theorem of harmonic function, is a nonlinear Liouville type theorem.
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