How do electrons choose their path?                     Wire A
                  -----R-----    
                 /           \
------I--->-[P]--             ---------I-->
                 \           /
                  -----R-----    
                    Wire B

Wire A and B both have a resistance of $R$ and a current of $\frac{I}{2}$ flows through each of the wires. How come electrons know which wire path to choose in this configuration?
What I am thinking is if we consider electrons at point P are in a state
$\frac{|A\rangle + |B\rangle}{\sqrt{2}}$ and at the junction some kind of measurement occurs which leaves half of the electrons in the state $|A\rangle$ and the other half in the state $|B\rangle$.
Could you please explain how exactly does this work? Please point out why the argument given above is right or wrong (or at all relevant) in this situation.
EDIT:
How can one derive basic laws for series and parallel circuits from more basic principles?
 A: To speak of quantum state, the electrons should be coherent, have a non-negliglible de Broglie wavelength. On the other hand, a non-zero resistance imply a nonnegligible dissipation and is sure to break any coherence. Your pure quantum state is then quickly turned into a classical probabilistic mixture, and your electron behaves exactly like a water drop in a river which separates itself into to branch in front of an island: its trajectory depends on its position inside the cable, relative to impurity.
Edited :
To be more quantitative, the quantum effect can roughly be seen on a length of the scale Λ, where Λ is the thermal de Broglie wavelength, given by :
$$
   \Lambda
   =
   \frac{h}{\sqrt{2\pi mkT}}
   \simeq 10^{-11}\mathrm{ m} 
$$
where the numerical application is for an electron at room temperature. The quantum effects are therefore already negligible at the nanometric scale.
A: Think of it as a queue of people trying to enter a building with two entrances, both the same size and length. As people push each other, and as the people on the front move, queue proceeds, and statistically on equal amount in both entrances provided they are identical.
Same principle applies for different R's, R and 2R, where one entrance is smaller than the other one.
As for your argument. It is correct mathematically, in my opinion.
A: Quantum effects, as others have pointed out are negligible in most wires. If you want to derive from a particle like description of the wires, you'd be best off thinking in terms of gas/fluid dynamics (which is believed to in the continuous limit turn into the transport diffusion equations). You can simulate this on a computer by having an many electrons move ballistically through the material, and randomly scatter with some probability $p$ each time step. This model will give you Ohm's law.
Now granted, if you actually wanted to figure out what the probability $p$ is, and the effective resistance of the wire, things get really complicated and do indeed require quantum mechanics. If you want the math, you'd want to look into the theory of quantum mechanical scattering. The main idea is that an electron will be in a pure momentum p eigenstate, and get randomly placed into a new p' momentum eigenstate. Averaged over a bunch semi-classical particles, the I-V characteristics work out. The justification for this is in truth, somewhat sketchy (the above described simulation has not been formally proved to be the same as using the Boltzmann Transport and Diffusion Equations, we just think it does for appropriate limits).
