Are there SUSY Lagrangian terms that are not D-term nor F-term? I've read that a way to construct supersymmetric invariant lagrangian could be either to integrate a superfield in the whole superspace, i.e. in all anticommuting coordinates (D-term), or in half of them (F-term).
Obviously I call F-term a lagrangian term that can't be written as D-term, because all D-term could be written trivially as integrals in half the superspace.
But now I can't understand why couldn't be supersymmetric invariant lagrangian terms that are not even F-term, but they are however invariant.
EDIT
I thought that the answer could be that given an ordinary lagrangian $F(x)$ term (dependent only on space-time coordinates) I can make it a part of a chiral superfields, as a coefficients of $\theta\theta$ in $y-\theta$ expansion
$$ \Phi(y,\theta) = \phi(y) + \sqrt{2} \theta \psi(y) - \theta\theta F(y)$$
$$ y^\mu = x^\mu + i\theta\sigma^\mu\bar{\theta}$$
choosing arbitrarily the $\phi$ and $\psi$ functions.
The question now become: does it work?
 A: This boils down to the fact that the supercharges are represented in superspace by 
$$
Q_{\alpha}=\frac{\partial}{\partial\theta^{\alpha}}-i(\sigma^{m}\bar\theta)_{\alpha}\frac{\partial}{\partial x^{m}}=\left(\frac{\partial}{\partial\theta^{\alpha}}\right)_{y}
$$
$$
Q^{\dot\alpha}=\frac{\partial}{\partial\theta_{\dot\alpha}}-i(\bar\sigma^{m}\theta)^{\dot\alpha}\frac{\partial}{\partial x^{m}}=\left(\frac{\partial}{\partial\theta_{\dot\alpha}}\right)_{y}-2i(\bar\sigma^{m}\theta)^{\dot\alpha}\frac{\partial}{\partial y^{m}}
$$
And the D-terms and F-terms are written as fermionic integrals:
$$
\mathcal{L}_{D}=\int d^{2}\theta V(y,\theta),\,\,\,\,\,\,\,\,\,\,\, \mathcal{L}_{F}=\int d^2\theta d^{2}\bar\theta V(x,\theta,\bar\theta)
$$
So if you act the supercharges in a D-term or a F-term, the first derivative of the supercharge, the $\theta$-derivative, will drop out because the fermionic integrals are only non-zero if it is saturated. This means that there will be only the $x$-derivatives, making a total derivative.  This means that by doing a supersymmetric transformation in the Lagrangian we obtain a total derivative!, so the action is invariant under supersymmetry. Then we say that this Lagrangian is supersymmetric in a manifest way, since there is no need to check the invariance explicitly.
Now, for a given superfield, it is possible to write an action that is supersymmetric out of components that are not $F$-terms or $D$-terms, but this will be make the supersymmetry not manifest. 
There is example for you. In pure spinor formalism for the second quantized superparticle in d=10 we can write the action as 
$$
\int d^{10}x \langle \psi \,Q\psi\rangle
$$
where $\psi(\lambda,\theta)$ is the pure spinor superfield, $Q=\lambda^{\alpha}D_{\alpha}$, and $\langle...\rangle$ is defined by picking just the $\langle\theta^5\lambda^3\rangle=1$, and zero otherwise. This means that it does not pick the last component of the superfields $\theta^{16}$. Nonetheless, this action describes linearized $d=10$ Super-Yang-Mills, so it is supersymmetric, although  not in a manifest way.
Back to $d=4$, it is always possible to find an manifest supersymmetric formulation for a given non-manifest supersymmetric $N=1$ action. For large dimensions or extended supersymmetry things start to be more complicated, and the superspace should be generalized some how, e.g. harmonic superspace, pure spinors etc.
