Hermitian operator ?? is this possible we know that the operator
$ H= - \hbar ^{2} \frac{d^{2}}{dx^{2}}+ V(x) $ is hermitian isn't it ??
however what would happen if the potential were still real but it depends on the Wave function, for example huypothetically
$ V(x) = |\Psi (x)|^{2} $ or $ V(x) = arg \Psi (x) $
since the functions $ |x| $ and $ arg (x+iy) $ are ALWAYS real, then the hamiltonian with potentials (1) and (2) should be Hermitian but they depend on the solution so i am not sure about the Hermiticity of a Hamiltonian in the form $ H =p^{2}+ |\Psi (x) |^{2} $ i believe that a real potential makes the Hamiltonian hermitian even in the case that we do not exactly know what potential is
 A: Since the momentum operator is hermitian, it's square, the first expression, is hermitian too. The operators which are considered to be a Laplacians generally tend to have this property. 
If $V(x)$ is a real function, then it's hermitian as you say. If the Hamiltonian contains any function $|\Phi(x)|^2$, then this is a priori just the previous case. If you mean this to be the respective wave function, then the operator is more of a functional. In that case the associated differential equation is certainly not linear, so you leave the framework in the standard terminology. Although the operator as such will still behave hermitean w.r.t. to the scalar product, so the answer is a cautious yes. As a remark, then function involving the argument of the wave function is pretty unphysical as the phase is exactly the quantity, which should be undetectable.
There are theories which have such a non-linear structure , see for example the Nonlinear Schrödinger equation, although notice the integral in the Hamiltonian. On that page you also find a link to the quantized version (Schrödinger field) of the model you constructed as a special case.
