University Physics Notes: Quantum Mechanics – The Pauli Exclusion Principle
The Pauli exclusion principle is a quantum mechanical principle
formulated by the Austrian physicist Wolfgang Pauli in 1925. In its
simplest form for electrons in a single atom, it states that no two
electrons can in an atom have the same four quantum numbers, that is,
if
are
the same, ms must be different such that the electrons have opposite
spins. More generally, no two identical fermions (particles with
half-integer spin) may occupy the same quantum state simultaneously.
A more rigorous statement of this principle is that, for two
identical fermions, the total wave function is anti-symmetric.
The Pauli exclusion principle is one of the most important principles in physics, mainly because the three types of particles from which the ordinary atom is made—electrons, protons, and neutrons—are all subject to it; consequently, all material particles exhibit space-occupying behavior. The Pauli exclusion principle underpins many of the characteristic properties of matter, from the large-scale stability of matter, to the existence of the periodic table of the elements.
Fermions, particles with antisymmetric wave functions, obey the
Pauli exclusion principle. Apart from the familiar electron, proton
and neutron, these include neutrinos and quarks (from which protons
and neutrons are made), as well as some atoms like helium-3. All
fermions possess "half-integer spin", meaning that they
possess an intrinsic angular momentum whose value is
times
a half-integer (1/2, 3/2, 5/2, etc.). In the theory of quantum
mechanics, fermions are described by "antisymmetric states"
such that if any two are interchanged, a phase change in the
wavefunction of
occurs.
is
antisymmetric sine
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Particles with integer spin have a symmetric wave function and are called bosons; in contrast to fermions, they may share the same quantum states. Examples of bosons include the photon, the Cooper pairs responsible for superconductivity, and the W and Z bosons.
is
antisymmetric sine
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