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Linearly disjoint
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Linearly disjoint : ウィキペディア英語版
Linearly disjoint
In mathematics, algebras ''A'', ''B'' over a field ''k'' inside some field extension \Omega of ''k'' (e.g., universal field) are said to be linearly disjoint over ''k'' if the following equivalent conditions are met:
*(i) The map A \otimes_k B \to AB induced by (x, y) \mapsto xy is injective.
*(ii) Any ''k''-basis of ''A'' remains linearly independent over ''B''.
*(iii) If u_i, v_j are ''k''-bases for ''A'', ''B'', then the products u_i v_j are linearly independent over ''k''.
Note that, since every subalgebra of \Omega is a domain, (i) implies A \otimes_k B is a domain (in particular reduced).
One also has: ''A'', ''B'' are linearly disjoint over ''k'' if and only if subfields of \Omega generated by A, B, resp. are linearly disjoint over ''k''. (cf. tensor product of fields)
Suppose ''A'', ''B'' are linearly disjoint over ''k''. If A' \subset A, B' \subset B are subalgebras, then A' and B' are linearly disjoint over ''k''. Conversely, if any finitely generated subalgebras of algebras ''A'', ''B'' are linearly disjoint, then ''A'', ''B'' are linearly disjoint (since the condition involves only finite sets of elements.)
== See also ==

*Tensor product of fields

抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
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