> Lie groups are the reason why it is better to represent gamma matrices as 
(Lorentz, Spinor, Spinor), the (Lorentz)-matrix representation loses the 
spinor-type transformation properties.

Why? the spinor transformations appear in matrix form

S G(m) S**-1 = L(m, -n) G(n)


On Monday, September 16, 2013 7:03:55 PM UTC+2, F. B. wrote:
>
> Further considerations:
>
>
>    - soon there will be a PR to add auto-matrix indices capabilities. In 
>    the construction of a tensor, indices marked by True instead of an index 
>    symbol will be considered auto-matrix indices, they behave upon 
>    multiplication with other tensors as matrices or vectors (there can be 0, 
> 1 
>    or 2 automatrix indices for each TensorIndexType, 1 => vector behavior, 
> 2=> 
>    matrix behavior). A tensor can have many automatrix indices, it is 
>    important they are applied on different TensorIndexType.
>    - gamma matrices will have default auto-matrix behavior on their 
>    spinor indices.
>    - tensor indices are conceptually strictly related to representations 
>    of Lie groups, in the future we could generate TensorIndexType instances 
>    from an object representing a representation of a Lie group.
>    - Lie groups are the reason why it is better to represent gamma 
>    matrices as (Lorentz, Spinor, Spinor), the (Lorentz)-matrix representation 
>    loses the spinor-type transformation properties.
>    - What happens on numerical indices? My guess is that a tensor gets 
>    reduced in its rank. E.g. *GammaMatrix(U(3))*, this means that in a 
>    certain basis we are representing gamma^3 covariant. Operators U( ) and D( 
>    ) (up and down) need to be introduced.
>
>

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