Short Example
A conventional Josephson junction, which consists of a superconductor-insulator-superconductor (SIS) sandwich and is biased by a constant current $I$, has the following action: $$S_{SIS}\left[\phi(t)\right]=\int_{t_i}^{t_f} dt\left[\frac{(\hbar \dot\phi)^2}{4E_C}+E_J\left(\cos\phi+\frac{I}{I_c}\phi\right)\right]$$ where $\phi(t)$ is a generalized coordinate, whose meaning is the difference between an order parameter phase $\phi_1$ of the first superconductor and a phase $\phi_2$ of the second one (i.e. $\phi = \phi_1-\phi_2$).
If one needs to include quasiparticle dissipation, a second-quantized hamiltonian can be used to determine the effective action:
$$S_{SIS}^{\text{eff}}\left[\phi(t),\chi(t)\right]=\int_{t_i}^{t_f} dt\left[-\frac{\hbar ^2\ddot\phi}{2E_C}\cdot\chi+E_J\left(\cos(\phi+\chi/2)-\cos(\phi-\chi/2)+\frac{I}{I_c}\chi\right)\right]+S_{SIS}^{\text{dissipation}}\left[\phi(t),\chi(t)\right]$$
where $\phi(t)$ is now an average phase difference and $\chi(t)$ characterizes some fluctuations near the average. I don't write a large expression for $S_{SIS}^{\text{dissipation}}$ explicitly, but it's known quantity (for details see Gerd Schön, A.D. Zaikin, the formulas (3.47), (3.48), (3.70)).
My Question
I wonder how to write down an (effective?) action $S_{NS}$ describing normal metal-superconductor (NS or NIS) connection biased by a voltage/current. I don't understand Green functions yet, so I'd like to see the answer in a form similar to the equations above.
Possible but Incomplete Answer
So far, I've found something describing Andreev conductance (Keldysh action for disordered superconductors, the formula (6.8)):
$$S_{A}\left[\phi(\omega),\chi(\omega)\right]=\frac{iG_A}{2}\int_{-\infty}^{\infty} \frac{d\omega}{2\pi}\hbar\omega\sin\chi(\omega)\cdot\\\cdot\left[\sin\left\{\phi(\omega)-\phi(-\omega)\right\}\cos\chi(-\omega)+\coth\left(\frac{\hbar\omega}{2T}\right)e^{i\phi(-\omega)-i\phi(\omega)}\sin\chi(-\omega)\right]\tag{6.8}$$
where $G_A$ is Andreev conductance, $T$ is temperature of the superconductor, $\phi$ (or $\theta_1$) is an average superconducting phase and $\chi$ (or $\theta_2$) characterizes some fluctuations near the average.
As can be seen, the dimension of the action $S_A$ is not $[\hbar]$. If I understand right the formulas (6.11) and (6.13) from the same article, $G_A$ is dimensionless. Then the dimension of $S_A$ is $[\hbar/t^2]$.
Moreover, there is no integration over time in $S_A$, so a real action $S_{NS}\left[\phi(t),\chi(t)\right]$ has to be determined somehow from $S_A$. It seems a procedure I need was used to obtain (6.11):
$$S_A\left[\phi(t),\chi(t)\right]=-eG_A\int_{-\infty}^{+\infty}dtV(t)\chi(t)+o[\chi]\tag{6.11}$$
where $V(t) = \frac{\hbar}{2e}\cdot\frac{d\phi(t)}{dt}$ is the voltage bias. But the first order on $\chi$ is not sufficient for me, so I have to understand what steps to perform from (6.8) to (6.11). Are they some integral transformation $S_{NS}=\int dt\int dt'S_A f(t,t')$?