I have very little background with functional derivatives and I would like to clarify some issues.
I am trying to compute the second functional derivative of the Klein Gordon action expressed in real components
S[ϕ1,ϕ2,∂μϕ1,∂νϕ2]=∫d4xL=∫d4x(−∂μϕ1∂μϕ1−∂μϕ2∂μϕ2+
−m2(ϕ21+ϕ22)−λ(ϕ21+ϕ22)2)
I know how to compute the first functional derivative
δSδϕ1(x)=∂L∂ϕ1−∂μ∂L∂(∂μϕ1)
which gives
2(∂2ϕ1(x)−m2ϕ1(x)−4λϕ1(x)[ϕ21(x)+ϕ22(x)])
from now on I have doubts. I wanna compute
δ2Sδϕ1(y)δϕ1(x)
If there were no derivatives this would be trivial but I don't know how to deal with ∂2. I have thought in introducing a delta to write this as an integral and use the formula I have used to compute the first functional derivative, but I am concerned about taking derivatives of something having a Dirac delta.
So, my question is, how am I supposed to compute this functional derivative?