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Thus, (u^) is a mild positive solution of problem (1.1).
Hence, (u^) is a mild positive solution of problem (2).
Therefore, (u^) is a mild positive solution of problem (1.1).
Step 3: We will prove the existence of a mild positive solution of problem (2).
Then, given ((u_{0},v_{0})^{T} in B^{sigma }_{p,q,mathcal{N}}), there exists a constant (tau >0) such that problem (1.3a - 1.3d 1.3a - 1.3due locally mild positive solution ((u,v)^{T}: [0,tau ] righasrrow B^{sigma }_{p,q, mathcal{N}} times B^{sigma }_{p,q,mathcal{N}}).
Similar(55)
end{cases}displaystyle end{aligned} With the help of the monotone iterative method, the existence and uniqueness of the mild positive solutions were obtained in the paper.
By imposing some relatively mild structural conditions on f, H 1, H 2, and φ, one positive solution to the problem is ensured.
In Section 4, under some mild assumption, we establish the maximum eigenvalue interval for the existence of the unique positive solution for FEP (1) and show that such a positive solution depends continuously on the parameter λ.
The positive solution apparently described normal electrons.
"I expect we can come to a positive solution.
has a positive solution.
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