Abstract
We write: \({\mathcal M}\) group; 
subgroup; \({\textsc {M}}\) semigroup; \({\mathsf M}\) set; \({\mathtt M}\) complex; M (transformation) matrix; \(\mathbb {M}\) (Minkowski) space.
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Notes
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- 2.
Here it is possible to use the same symbol as for the tensor product, cp. Eq. (898), namely \(\otimes \).
- 3.
A more specific discussion of this procedure is contained, e.g. in the textbook of Fick (1968).
- 4.
Here the observable A should be explicitly time independent, i.e. the measuring process for this observable does not change temporally, \(\partial A/\partial t = 0 \).
the subgroup of rotations. Then the cosets a 
are transformations consisting of proper Author information
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Günther, H., Müller, V. (2019). Representations of the Lorentz Group Weyl Equation and Dirac Equation. In: The Special Theory of Relativity. Springer, Singapore. https://doi.org/10.1007/978-981-13-7783-9_10
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DOI: https://doi.org/10.1007/978-981-13-7783-9_10
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