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Almost-contact manifold

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Geometric structure on a smooth manifold
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In the mathematical field of differential geometry, an almost-contact structure is a certain kind of geometric structure on a smooth manifold. Such structures were introduced by Shigeo Sasaki in 1960.

Precisely, given a smooth manifold M {\displaystyle M} , an almost-contact structure consists of a hyperplane distribution Q {\displaystyle Q} , an almost-complex structure J {\displaystyle J} on Q {\displaystyle Q} , and a vector field ξ {\displaystyle \xi } which is transverse to Q {\displaystyle Q} . That is, for each point p {\displaystyle p} of M {\displaystyle M} , one selects a codimension-one linear subspace Q p {\displaystyle Q_{p}} of the tangent space T p M {\displaystyle T_{p}M} , a linear map J p : Q p Q p {\displaystyle J_{p}:Q_{p}\to Q_{p}} such that J p J p = id Q p {\displaystyle J_{p}\circ J_{p}=-\operatorname {id} _{Q_{p}}} , and an element ξ p {\displaystyle \xi _{p}} of T p M {\displaystyle T_{p}M} which is not contained in Q p {\displaystyle Q_{p}} .

Given such data, one can define, for each p {\displaystyle p} in M {\displaystyle M} , a linear map η p : T p M R {\displaystyle \eta _{p}:T_{p}M\to \mathbb {R} } and a linear map φ p : T p M T p M {\displaystyle \varphi _{p}:T_{p}M\to T_{p}M} by η p ( u ) = 0  if  u Q p η p ( ξ p ) = 1 φ p ( u ) = J p ( u )  if  u Q p φ p ( ξ ) = 0. {\displaystyle {\begin{aligned}\eta _{p}(u)&=0{\text{ if }}u\in Q_{p}\\\eta _{p}(\xi _{p})&=1\\\varphi _{p}(u)&=J_{p}(u){\text{ if }}u\in Q_{p}\\\varphi _{p}(\xi )&=0.\end{aligned}}} This defines a one-form η {\displaystyle \eta } and (1,1)-tensor field φ {\displaystyle \varphi } on M {\displaystyle M} , and one can check directly, by decomposing v {\displaystyle v} relative to the direct sum decomposition T p M = Q p { k ξ p : k R } {\displaystyle T_{p}M=Q_{p}\oplus \left\{k\xi _{p}:k\in \mathbb {R} \right\}} , that η p ( v ) ξ p = φ p φ p ( v ) + v {\displaystyle {\begin{aligned}\eta _{p}(v)\xi _{p}&=\varphi _{p}\circ \varphi _{p}(v)+v\end{aligned}}} for any v {\displaystyle v} in T p M {\displaystyle T_{p}M} . Conversely, one may define an almost-contact structure as a triple ( ξ , η , φ ) {\displaystyle (\xi ,\eta ,\varphi )} which satisfies the two conditions

  • η p ( v ) ξ p = φ p φ p ( v ) + v {\displaystyle \eta _{p}(v)\xi _{p}=\varphi _{p}\circ \varphi _{p}(v)+v} for any v T p M {\displaystyle v\in T_{p}M}
  • η p ( ξ p ) = 1 {\displaystyle \eta _{p}(\xi _{p})=1}

Then one can define Q p {\displaystyle Q_{p}} to be the kernel of the linear map η p {\displaystyle \eta _{p}} , and one can check that the restriction of φ p {\displaystyle \varphi _{p}} to Q p {\displaystyle Q_{p}} is valued in Q p {\displaystyle Q_{p}} , thereby defining J p {\displaystyle J_{p}} .

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