Euler-Lagrange equations from a complex Lagrangian I'm looking for generalizations of the Euler-Lagrange equations that would be derived from a complex-valued Lagrangian density. I realize that “minimum” and “maximum” don't have obvious meaning for a complex-valued action, so am looking for E-L equations that correspond to (a) constant amplitude of the action, (b) constant phase of the action, or (c) both.
The papers I've found mostly avoid the issue by allowing complex valued field variables within the Lagrangian but ensuring that the Lagrangian itself is real-valued.
This paper might be relevant: Non-standard complex Lagrangian dynamics
Any advice will be welcome.
 A: If you have a complex action, you need to decide what you require to be stationary. It can be a) action provided its amplitude is constant; b) action provided its phase is constant; c) amplitude of the action; d) phase of the action; e) real part of the action, etc. In each of these cases this is equivalent to requiring that some real action is stationary, for example, in case c) you can choose action equal to the amplitude of the "old" complex action.
So what happens if you require, say, that both the amplitude and the phase of the complex action are stationary? As each of these requirements is typically sufficient to get equations of motion, both of these requirements together typically yield an overdetermined system of equations. It is possible, however, that this overdetermined system is consistent and makes sense, but I cannot offer an example at the moment.
A: *

*A stationary action principle for a complex action $S_c=S_1+iS_2\in \mathbb{C}$ is equivalent to 2 real stationary action principles for the real and imaginary part, $S_1,S_2\in\mathbb{R} $. In other words, the EL equations for $S_c$ are precisely the EL equations for $S_1$ and the EL equations for $S_2$. It may be possible to organize the EL equations for $S_c$ as complex equations, especially if the Lagrangian is holomorphic.

*In the Feynman path integral $Z$, the action $S$ is real, at least in the Minkowskian formulation. However, when evaluating the semiclassical approximation via the method of steepest descent, one typically deforms the contour of integration into the complex plane, which may lead to complex contributions to $Z$. Stationary points in the complex plane may or may not have a straight-forward physical interpretation as solutions to the (analytic continued) EL equations.
