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2. Recalling that the four-momentum of the particle is
 |
(52) |
one has the fact that these two sets of equations, (52) and (53), define implicitly the
phase space transformation
Being generated from the scalar function
,
this transformationis canonical, i.e. it leaves invariant the
representation of the antisymmetric tensor, Eq.(8):
Ulrich Gerlach
2005-11-07