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Tensor Algebra (Definition)

The algebra of tensors on a vector space.
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The statement of the theorem

Let VV be a vector space over a field KK. The Tensor Algebra T(V)T(V) is defined as the direct sum of the kk-th tensor powers of VV: \n\nT(V)=k=0Tk(V)=k=0VkT(V) = \bigoplus_{k=0}^{\infty} T^k(V) = \bigoplus_{k=0}^{\infty} V^{\bigotimes k} \n\nwhere T0(V)=KT^0(V) = K (the base field), T1(V)=VT^1(V) = V, and for k0k \neq 0, T^k(V) = V \big\otimes_{k} V. \n\nT(V)T(V) is equipped with a multiplication operation, denoted by μ:T(V)×T(V)T(V)\mu: T(V) \times T(V) \to T(V), which is the concatenation of tensor products. Specifically, for ATk(V)A \in T^k(V) and BTm(V)B \in T^m(V), the product is defined as:\n\nAB=ABA \cdot B = A \otimes B \n\nThis multiplication makes T(V)T(V) an associative, graded algebra, i.e., T(V)=k=0Tk(V)T(V) = \bigoplus_{k=0}^{\infty} T^k(V), satisfying the associativity axiom: (AB)C=A(BC)(A \cdot B) \cdot C = A \cdot (B \cdot C) for all A,B,CT(V)A, B, C \in T(V). The quotient algebra T/IT^*/I (where II is the ideal generated by the commutator [v1,v2]=v1v2v2v1[v_1, v_2] = v_1 v_2 - v_2 v_1) yields the universal enveloping algebra of the Lie algebra associated with VV.