After a brief introduction of Born’s reciprocal relativity theory is presented, we review the construction of the
quaplectic group that is given by the semi-direct product of
with the
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After a brief introduction of Born’s reciprocal relativity theory is presented, we review the construction of the
quaplectic group that is given by the semi-direct product of
with the
(noncommutative) Weyl–Heisenberg group corresponding to
fiber coordinates and momenta
;
. This construction leads to more general algebras given by a two-parameter family of deformations of the quaplectic algebra, and to further algebraic extensions involving antisymmetric tensor coordinates and momenta of higher ranks
;
. We continue by examining algebraic extensions of the Yang algebra in extended noncommutative phase spaces and compare them with the above extensions of the deformed quaplectic algebra. A solution is found for the exact analytical mapping of the noncommuting
operator variables (associated to an 8D curved phase space) to the canonical
operator variables of a flat 12D phase space. We explore the geometrical implications of this mapping which provides, in the
limit, the embedding functions
of an 8D curved phase space into a flat 12D phase space background. The latter embedding functions determine the functional forms of the base spacetime metric
, the fiber metric of the vertical space
, and the nonlinear connection
associated with the 8D cotangent space of the 4D spacetime. Consequently, we find a direct link between noncommutative curved phase spaces in lower dimensions and commutative flat phase spaces in higher dimensions.
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