We prove the existence of ground state solution to the following problem. \begin{align*} (-\Delta)^{s}u+u&=\lambda|u|^{-\gamma-1}u+P(x)|u|^{p-1}u,~~^N\setminus\Omega\ N_su(x)&=0,~~\Omega \end{align*} where , , , with . % $0<s^-=\underset{{(x,y)\in\Omega\times\Omega}}{\inf}{s(x,y)}\leq s(x,y)\leq s^+=\underset{{(x,y)\in\Omega\times\Omega}}{\sup}{s(x,y)}<10<\gamma^-=\underset{{x\in\Omega}}{\inf}{\gamma(x)}\leq \gamma(x)\leq \gamma^+=\underset{{x\in\Omega}}{\sup}{\gamma(x)}<11-\gamma^-<1<p^-=\underset{x\in\Omega}{\inf}{p(x)}\leq p(x)\leq p^+=\underset{x\in\Omega}{\sup}{p(x)}<2_{s^-}^=\underset{{x\in\Omega}}{\inf}{2_s^(x)}2_s^(x)=\frac{2N}{N-2\tilde{s}(s)}\tilde{s}(x)=s(x,x)$. Moreover, is a smooth bounded domain, denotes the -fractional Laplacian and finally denotes the nonlocal operator that describes the Neumann boundary condition which is given as follows. \begin{align} N_{s}u(x)&=C_{N,s}\int_{^N\setminus\Omega}\frac{u(x)-u(y)}{|x-y|^{N+2s}}dy,~x\in\Omega. \end{align*} We further establish the existence of infinitely many bounded solutions to the problem.

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