Applied Quantum Mechanics, Second Edition

In classical mechanics the constants of motion of an isolated system are energy, linear momentum, and angular momentum. So far in this book we have not considered angular momentum. In this chapter we start by considering classical angular momentum and then proceed to find the corresponding quantum operators. Following this we consider a hydrogenic atom as a prototype application.
Suppose, as illustrated in Fig. 11.1, we have a point-particle of mass m, linear velocity v at instant t = 0, and momentum p = m v. Angular momentum L about a point r = 0 is defined as [1.]
where r is the position of particle. Angular momentum is measured in units of J s.
This equation can be written in terms of angular velocity vector ?, normal to the plane of rotation, to give
Making use of the vector relationship a ( b c) = ( a c) b ? ( a b) c, the expression for L may be rewritten as
where the inertia tensor is
In Eq. (11.4) 1 is the unit matrix. If ? = ? n where n is the unit vector in the direction of ? then the...