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mathematics-physics-wiki/docs/en/mathematics/differential-geometry/torsion.md

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Torsion

Let \mathrm{M} be a differential manifold with \dim \mathrm{M} = n \in \mathbb{N} used throughout the section. Let \mathrm{TM} and \mathrm{T^*M} denote the tangent and cotangent bundle, V and V^* the fiber and dual fiber bundle and \mathscr{B} the tensor fiber bundle.

Torsion operator

Definition 1: the torsion operator \Theta: \Gamma(\mathrm{TM}) \times \Gamma(\mathrm{TM}) \to \Gamma(\mathrm{TM}) is defined as

\Theta(\mathbf{u}, \mathbf{v}) = \nabla_\mathbf{u} \mathbf{v} - \nabla_\mathbf{v} \mathbf{u} - \mathscr{L}_\mathbf{u} \mathbf{v},

for all \mathbf{u}, \mathbf{v} \in \Gamma(\mathrm{TM}) and \mathscr{L} the Lie derivative.

Using this definition we obtain the following results.

Proposition 1: the decomposition of the torsion operator results into

\mathbf{k}(\bm{\omega}, \Theta(\mathbf{u}, \mathbf{v})) = \omega_i u^j v^k (\Gamma^i_{kj} - \Gamma^i_{jk}),

for all \bm{\omega} \in \Gamma(\mathrm{T}^*\mathrm{M}) and \mathbf{u}, \mathbf{v} \in \Gamma(\mathrm{TM}).

??? note "Proof:"

Will be added later.

Torsion tensor

As a result of proposition 1 we may view torsion as a locally defined mixed tensor of type \mathbf{T} \in \mathrm{T}_x \mathrm{M} \otimes \mathrm{T}_x^* \mathrm{M} \otimes \mathrm{T}_x^* \mathrm{M}.

Definition 2: the torsion tensor \mathbf{T}: \mathrm{T}_x^* \mathrm{M} \times \mathrm{T}_x \mathrm{M} \times \mathrm{T}_x \mathrm{M} \to \mathbb{K} with x \in \mathrm{M} is defined as

\mathbf{T}(\bm{\omega}, \mathbf{u}, \mathbf{v}) = \mathbf{k} \big(\bm{\omega}, \Theta(\mathbf{u}, \mathbf{v}) \big),

for all \bm{\omega} \in \mathrm{T}^*_x\mathrm{M} and \mathbf{u}, \mathbf{v} \in \mathrm{T}_x \mathrm{M}.