In my experiment, I use a laser beam with wavelength $\lambda=894 \text{nm}$ for some magnetic resonance experiment. Right now, I'm doing some calculation using Quantum Mechanics, which requires the amplitude of the electric field to be inserted to my Hamiltonian.
My question is basically: How do I go from a power, measured in $\mu W$ to an Electric Field amplitude $E_0$ to use it in a QM's Hamiltonian?
So I think that I need to use the Poynting vector, which is defined as:
$$\vec{S}=\frac{1}{\mu_0} \vec{E}\times \vec{B}$$
where I'm using $\mu_0$ because the interactions happen in a vacated, dilute gas cell. If I take the magnitude of the last equation I get
$$S=\frac{EB}{\mu_0}=\frac{E^2}{c \mu_0}$$
where I used the fact that $E_0=c B_0$ according to Maxwell equations.
However, the Poynting vector is energy per unit area per unit time, or power per unit area. This means that I have to know the area of my laser beam, and that's my problem now.
The laser beam in my experiment comes out of a multi-mode fiber, and then it goes to a linear polarizer, and then a quarter wave plate, where we use the latter to get circularly polarized light, and then a collimator lens. And after that it interacts with my atoms.
I know the core-diameter of my multi-mode fiber, let's call it $r_F$, but I don't know what transverse modes are produced in it. How can I know the effective area of my laser beam (call it $A_L$), so that I could substitute that in my Poynting vector and calculate the electric field amplitude of my laser beam?
I imagine that eventually I should be able to calculate $A_L$, and I can use the following relation to get my electric field amplitude, which I get from the Poynting vector definition
$$E=\sqrt{\frac{\mu_0 c S}{B}}=\sqrt{\frac{\mu_0 c P}{B A_L}}$$
where $P$ is the power of my beam.
Is my reasoning correct? Please advise. If I'm missing something in the problem, let me know.
Please note: this is a real experiment, so all practical approximations are allowed.