What's the total angular momentum operator for a system of two particles?

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Suppose we're in two dimensions, and both particles have mass 1.

Particle 1's location is given by its polar coordinates (r_1,\theta_1); likewise for Particle 2 (r_2,\theta_2).

Is it true that the total angular momentum \vec{L} is just the sum of the individual angular momenta of the particles: \vec{L} = \vec{L}_1 + \vec{L}_2? If that's the case, can you give me the total angular momentum operator \vec{L} as a differential operator?
 
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yeah, just add it up: L_j^z = -i\hbar \left[y_j\partial/\partial{x_j} - {x_j}\partial/\partial{y_j}\right] where j is the particle index. Keep in mind L_2 does not act on the coordinates for the first particle.
 
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