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Hi friend,

spin is just an extra degree of freedom introduced when you realise the "wavefunction"/"state-vector" of a particle requires more than one complex component to describe it, Levy-Leblond's famous 1967 paper (free download) explained this (so, in particular, Dirac's relativistic corrections are not needed to introduce spin)

You can think of this as a type of "linearisation of the Schrödinger Equation", and if you're really cool (like me) you'll extend the wave function of every particle to ~10^80 components.

spin is just an extra degree of freedom introduced when you realise the "wavefunction"/"state-vector" of a particle requires more than one complex component to describe it, Levy-Leblond's famous 1967 paper (free download) explained this (so, in particular, Dirac's relativistic corrections are not needed to introduce spin)

You can think of this as a type of "linearisation of the Schrödinger Equation", and if you're really cool (like me) you'll extend the wave function of every particle to ~10^80 components.

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tom.stoer

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Constructing a theory of gravity coupled to spin-half fields it becomes clear that this is not possible by using the metric formalism; one must enlarge the formalism to so-called tetrads. These are something like basis vectors of a four-dim. tangent space attached to each point in spacetime. Using these tangent spaces one can "gauge" the Lorentz symmetry, i.e. one can introduce a

b/c of this local SL(2,C) gauge symmetry one can say that locally a curved Riemann manifold = spacetime has the same symmetry structure as flat Minkowski space and that this allowes for the same construction of spinor fields as in Minkowski spacetime.

However there may be a global obstruction to introducing spin. A Riemann manifold that allows for a spin structure, i.e. the introduction of spinor fields, must have a certain property: it must be orientable (a Möbius strip isn't orientable) and its second Stiefel-Whitney class must vanish (unfortunately I cannot explain lucidly what this means). Therefore not all Riemann manifolds allow for the construction of spinor fields.

Assuming that the topology of spacetime remains invariant during expansion (time evolution) of the universe (which is the case in general relativity except for the formation of black holes) the spin structure does not change. It's a topological invariant.

The relation to the standard model is simply the fact that our universe allows for a spin structure and that therefore a plethora of elementary particles with spin (spin 1/2) can exist. The different particle species (electron, quarks, neutrinos, ...) in the standard model cannot be restricted or derived from the symmetry structure of spacetime. All what we can say is that spin 1/2 seems to exist and that we have a mathematical classification of manifolds which allow for spin to exist.

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Hi Tom,

Constructing a theory of gravity coupled to spin-half fields it becomes clear that this is not possible by using the metric formalism; one must enlarge the formalism to so-called tetrads. These are something like basis vectors of a four-dim. tangent space attached to each point in spacetime. Using these tangent spaces one can "gauge" the Lorentz symmetry, i.e. one can introduce alocalSL(2,C) gauge symmetry. This gauge symmetry means that one can rotate the tetrads at each spacetime differently b/c there is a connection, a gauge-field so to speak, which plays a similar role as a gauge field in ordinary gauge theories: it compensates the effect of local gauge transformations and makes the theory gauge invariant (this symmetry and the gauge field is not visible in the metric formalism).

b/c of this local SL(2,C) gauge symmetry one can say that locally a curved Riemann manifold = spacetime has the same symmetry structure as flat Minkowski space and that this allowes for the same construction of spinor fields as in Minkowski spacetime.

However there may be a global obstruction to introducing spin. A Riemann manifold that allows for a spin structure, i.e. the introduction of spinor fields, must have a certain property: it must be orientable (a Möbius strip isn't orientable) and its second Stiefel-Whitney class must vanish (unfortunately I cannot explain lucidly what this means). Therefore not all Riemann manifolds allow for the construction of spinor fields.

Assuming that the topology of spacetime remains invariant during expansion (time evolution) of the universe (which is the case in general relativity except for the formation of black holes) the spin structure does not change. It's a topological invariant.

The relation to the standard model is simply the fact that our universe allows for a spin structure and that therefore a plethora of elementary particles with spin (spin 1/2) can exist. The different particle species (electron, quarks, neutrinos, ...) in the standard model cannot be restricted or derived from the symmetry structure of spacetime. All what we can say is that spin 1/2 seems to exist and that we have a mathematical classification of manifolds which allow for spin to exist.

except Spin isn't a relativistic property - look at Levy-Leblond's paper (see my post above, sorry we posted simultaneously) - you just need a multi component wave function to incorporate spin.

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tom.stoer

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The OP was asking for spacetime, expansion, curvature and things like that. That's why I was thinking that one should explain spin on Riemann manifolds in the context of GR. Besides that you are right, the construction of spin via SL(2,C) i.e. via SR may be too complicated to start with and a non-rel. approach should be sufficient.

However I was not aware of this paper, so thanks for the reference.

Regarding

There are manifolds which do not allow for half-integer spin due the above mentioned topological obstruction to the existence of spin structures. I do not know whether there are Riemann manifolds which may be relevant on GR and what exactly goes wrong when trying to construct spinors, I only know the general statement that w/o vanishing of the second Stiefel-Whitney class "there is no spin". Of course integer spin i.e. vector and tensor fields are allowed, but half-integer ius ruled out.

However I was not aware of this paper, so thanks for the reference.

Regarding

This is not possible in general for Riemann manifolds.... you just need a multi component wave function to incorporate spin.

There are manifolds which do not allow for half-integer spin due the above mentioned topological obstruction to the existence of spin structures. I do not know whether there are Riemann manifolds which may be relevant on GR and what exactly goes wrong when trying to construct spinors, I only know the general statement that w/o vanishing of the second Stiefel-Whitney class "there is no spin". Of course integer spin i.e. vector and tensor fields are allowed, but half-integer ius ruled out.

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Yes sorry, your reply contained cool and relevant info which i didn't mean to dismiss :-)The OP was asking for spacetime, expansion, curvature and things like that. That's why I was thinking that one should explain spin on Riemann manifolds in the context of GR. Besides that you are right, the construction of spin via SL(2,C) i.e. via SR may be too complicated to start with and a non-rel. approach should be sufficient.

However I was not aware of this paper, so thanks for the reference.

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tom.stoer

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I tried to find a reference: except for the fact that differential topology and characteristic classes are difficult to understand anyway, the paper from Haefliger regarding the non-existence of spin structures is in French ;-(

A. Haefliger (1956). "Sur l’extension du groupe structural d’un espace fibré". C. R. Acad. Sci. Paris 243: 558–560.

A. Haefliger (1956). "Sur l’extension du groupe structural d’un espace fibré". C. R. Acad. Sci. Paris 243: 558–560.

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Yeah, I wouldn't bother with continuous multi-dimensional geometry models, they're the epicycles of our age, maybe good for approximate modeling in simplistic situations but otherwise not reality.This is not possible in general for Riemann manifolds.

There are manifolds which do not allow for half-integer spin due the above mentioned topological obstruction to the existence of spin structures. I do not know whether there are Riemann manifolds which may be relevant on GR and what exactly goes wrong when trying to construct spinors, I only know the general statement that w/o vanishing of the second Stiefel-Whitney class "there is no spin". Of course integer spin i.e. vector and tensor fields are allowed, but half-integer ius ruled out.

Reality = linear algebra + probability

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tom.stoer

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so the short answer is that spin exists b/c everything there is is a spin network; vertam ergo sum!Reality = linear algebra + probability

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eh? (I don't know latin)so the short answer is that spin exists b/c everything there is is a spin network; vertam ergo sum!

no, spin exists cos of all the complex (universe wide) linear algebraic evolution going on every 10^-43 secs or whatever

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marcus

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I spin therefore I existso the short answer is that spin exists b/c everything there is is a spin network; vertam ergo sum!

Witty echo of Decartes "Cogito ergo sum". Could be deeper than Decartes.

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tom.stoer

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"I spin, therefore I am"

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tom.stoer

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Lots of stuff to consider. Thanks.

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post #8 was the best post in the thread

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tom.stoer

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no, #11

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