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During the last twenty-five years quite remarkable relations
between nonas sociative algebra and differential geometry have been
discovered in our work. Such exotic structures of algebra as
quasigroups and loops were obtained from purely geometric
structures such as affinely connected spaces. The notion ofodule
was introduced as a fundamental algebraic invariant of differential
geometry. For any space with an affine connection loopuscular,
odular and geoodular structures (partial smooth algebras of a
special kind) were introduced and studied. As it happened, the
natural geoodular structure of an affinely connected space al lows
us to reconstruct this space in a unique way. Moreover, any smooth
ab stractly given geoodular structure generates in a unique manner
an affinely con nected space with the natural geoodular structure
isomorphic to the initial one. The above said means that any
affinely connected (in particular, Riemannian) space can be treated
as a purely algebraic structure equipped with smoothness. Numerous
habitual geometric properties may be expressed in the language of
geoodular structures by means of algebraic identities, etc.. Our
treatment has led us to the purely algebraic concept of affinely
connected (in particular, Riemannian) spaces; for example, one can
consider a discrete, or, even, finite space with affine connection
(in the form ofgeoodular structure) which can be used in the old
problem of discrete space-time in relativity, essential for the
quantum space-time theory."
During the last twenty-five years quite remarkable relations
between nonas sociative algebra and differential geometry have been
discovered in our work. Such exotic structures of algebra as
quasigroups and loops were obtained from purely geometric
structures such as affinely connected spaces. The notion ofodule
was introduced as a fundamental algebraic invariant of differential
geometry. For any space with an affine connection loopuscular,
odular and geoodular structures (partial smooth algebras of a
special kind) were introduced and studied. As it happened, the
natural geoodular structure of an affinely connected space al lows
us to reconstruct this space in a unique way. Moreover, any smooth
ab stractly given geoodular structure generates in a unique manner
an affinely con nected space with the natural geoodular structure
isomorphic to the initial one. The above said means that any
affinely connected (in particular, Riemannian) space can be treated
as a purely algebraic structure equipped with smoothness. Numerous
habitual geometric properties may be expressed in the language of
geoodular structures by means of algebraic identities, etc.. Our
treatment has led us to the purely algebraic concept of affinely
connected (in particular, Riemannian) spaces; for example, one can
consider a discrete, or, even, finite space with affine connection
(in the form ofgeoodular structure) which can be used in the old
problem of discrete space-time in relativity, essential for the
quantum space-time theory."
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