To see it, let us consider two spinless particles with masses m

_{1}and m

_{2}coupled with any central potential, say, with . The quasi-particle with the reduced mass describes the relative particle motion and depends on

**particles in a two-particle compound system. It is its orbital momentum which is quantized in terms of integer numbers, namely, ranges from to .**

*both*The particle-1 and particle-2 orbital (angular) momenta and , calculated relative to the system center of inertia, are just certain, generally non-integer fractions of .

In particular, and are not obliged to have integer values! Why? Because they are simply non-integer functions of operator and are determined with its eigenvalues. For example, in the non-relativistic Positronium (where the particle masses are equal), if , the electron orbital momentum has the following values of projections:

**-1/2, 0, +1/2**.

Surprise! And the same statement is valid for the positron projections in Positronium. "Half-integer" projections of a particle orbital momentum are thus possible and there is no kidding in it.

The particle orbital momenta in a bound system with respect to the system center of inertia are not momenta of independent, non-correlated subsystems. On the contrary, they are related and the rule of addition of

*independent*angular momenta, usually taught in courses of Quantum Mechanics, is not applicable to them.

## Comments