Haelfix said:
Actually it does have very deep roots. Its full derivation is a consequence of the mix of quantum mechanics and special relativity, quantum field theory. Without either one of those elements, you cannot logically have the so called spin-statistics theorem.
In its first (usually chemical useful) formulation,Pauli postulated the fact that 2 electrons could not be in the same quantum state.In the Dirac version of QM (the traditional formulation) is still kept as a postulate.Von Neumann used it to invent quantum statistical mechanics.And it was again Pauli who used indirectly (see below) to prove his theorem:the spin-statistics theorem (1940) is proven in the context of QED and a generalization to particle physics has been given by Lueders.
So my guess is it is the other way around.First postulate the symmetrization/antisymmetrization principle,then use it together with special relativity and quantization method to find out that there is a connection between spin ans statistics.
Allow me to quote from W.Pauli's famous article:"The Connection between spin and statistics."Phys.Rev.,58,p.716-722(1940) found in:"Wolfgang Pauli:<<Collected Scientific Papers>>",edited by R.Kronig and V.F.Weisskopf (1964,Interscience Pulblishers),Volume 2;p911-918:
Abstract:
"In the following paper we conclude for the relativistically invariant wave equation for free particles:From Postulate (I),according to which the energy must be positive,the necessity of Fermi-Dirac statistics for particles with arbitrary half-integer spin;from postulate (II),according to which observables on different space-time points with a space-like distance are commutable,the necessity of Einstein-Bose statistics for particles with arbitrary integer spin [...]"
Haelfix said:
In my opinion, this is the single most compelling experimental reason to believe in all the weirdness of special relativity and quantum mechanics.
In the same article,Pauli says:
"In conclusion we wish to state,that according to our opinion the connection between spin and statisics is one of the most important apllications of the special relativity theory".
