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Pauli's Principle

Pauli's principle, also known as Pauli's exclusion principle, was proposed by Wolfgang Pauli in 1925. The starting point was the problem of the completion of atomic shells and the structure of the periodic system of the chemical elements.
On the basis of the multiplet structure of the atomic spectra and the anomalous Zeeman effect, which was not able to be interpreted for a long time, Pauli realized that the peculiar, classically non-describable type of ambiguity of the quantum theoretical properties of the luminous electron demands for its description a fourth quantum number. So he added a spin quantum number, as it was later known, to the three known quantum numbers, principal quantum number, orbital quantum number and magnetic quantum number.


According to this postulate, two electrons in an atomic structure can never have all four quantum numbers in common. If one electron in an atom assumes a state described by all four quantum numbers, then this state is occupied.

Periodensystem
 
For a long time, the exclusion principle remained an unexplained supplement to quantum theory. But Pauli never gave up his goal of connecting his principle to other physical principles. It took almost another 15 years of dealing with the problem until he found the final explanation.
It turned out that the exclusion principle applies to particles with half-integral spin, e.g. electrons and protons. If these particles are described quantum statistically, then the so-called Fermi-Dirac statistics are employed. Such particles are known as fermions. On the other hand, particles with integral spin, e.g. photons, do not obey the exclusion principle and follow Bose-Einstein statistics. Such particles are known as bosons.
In 1945 Wolfgang Pauli was awarded the Nobelpreis for his discovery of the exclusion principle.
 
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