The fundamental tenet of quantum mechanics is that many basic phenomena at the atomic level (such as energy emission and angular momentum) appear to be quantized. “Quantized” means that when certain properties of a system are measured, a continuous range of results are not observed, but rather a set of discrete (separate) values. If “quanta” come in discrete units then it makes sense to count them with integers.
The idea of a spin = ½ particle was at first met with skepticism by much of the scientific community. It was not until 1928 when Paul Dirac directly derived this result for the electron from relativistic quantum mechanics that half-integer quantum numbers became widely accepted.
The idea of a spin = ½ particle was at first met with skepticism by much of the scientific community. It was not until 1928 when Paul Dirac directly derived this result for the electron from relativistic quantum mechanics that half-integer quantum numbers became widely accepted.
Some appreciation for why both integer and half-integer quantum numbers crop up may be gained by considering the properties of simple standing waves, such as vibrations of a guitar string. It is well recognized that standing waves only occur when their harmonics are either whole or half-integral multiples of the string length.
The guitar string example is only an analogy, not a proof, of why both whole and half-integer spin values might be reasonable at the quantum level. I present this to provide you with some comfort that all quantum features are not entirely foreign to our experience in the macroscopic world. |
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From a purely mathematical perspective, half-integer spins are direct consequence of advanced group theory intrinsic to the quantum mechanical formulation. Specifically, the spin operators and associated (Hilbert) space of spin states are governed by Lie SO(3) algebra, with resultant eigenvalues of ± ½. I don’t pretend to understand all the details but the reference below contains a mathematical proof for those capable and interested.
Veltman MJG, de Wit BQPJ, 't Hooft G. Topics in theoretical physics. Lie groups in physics (pdf), 2007. (Formal proof of how spin = ½ results from group theory using ladder operators - only for those with very strong mathematical backgrounds and/or interest. The correct pronunciation is "Lee".)
References
Wolfe J. Music Acoustics: Strings, standing waves, and harmonics (link). Sydney: University of New South Wales (accessed 2014)
Wolfe J. Music Acoustics: Strings, standing waves, and harmonics (link). Sydney: University of New South Wales (accessed 2014)
Related Questions
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What is spin?
How do you predict the value of nuclear spin (I) based on the number of protons and neutrons?
What is the difference between "spin" and "spin state"?