Angular Momentum: Difference between revisions
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In this chapter, we will discuss the treatment of angular momentum in quantum mechanics. The quantization of angular momentum was first observed in the [[Stern-Gerlach Experiment|Stern-Gerlach experiment]] in 1922 through the deflection of silver atoms passing through a spatially inhomogeneous magnetic field. We will show how this quantization is formulated mathematically within the framework of modern quantum mechanics, as opposed to the old quantum theory that the Stern-Gerlach experiment was intended to test. | In this chapter, we will discuss the treatment of angular momentum in quantum mechanics. The quantization of angular momentum was first observed in the [[Stern-Gerlach Experiment|Stern-Gerlach experiment]] in 1922 through the deflection of silver atoms passing through a spatially inhomogeneous magnetic field. We will show how this quantization is formulated mathematically within the framework of modern quantum mechanics, as opposed to the old quantum theory that the Stern-Gerlach experiment was intended to test. | ||
We begin by deriving the commutation relations among the components of the angular momentum operator, and then by showing how one may see that it is quantized. |
Revision as of 22:49, 18 August 2013
In this chapter, we will discuss the treatment of angular momentum in quantum mechanics. The quantization of angular momentum was first observed in the Stern-Gerlach experiment in 1922 through the deflection of silver atoms passing through a spatially inhomogeneous magnetic field. We will show how this quantization is formulated mathematically within the framework of modern quantum mechanics, as opposed to the old quantum theory that the Stern-Gerlach experiment was intended to test.
We begin by deriving the commutation relations among the components of the angular momentum operator, and then by showing how one may see that it is quantized.