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Canonical basis : ウィキペディア英語版 | Canonical basis In mathematics, a canonical basis is a basis of an algebraic structure that is canonical in a sense that depends on the precise context: * In a coordinate space, and more generally in a free module, it refers to the standard basis defined by the Kronecker delta. * In a polynomial ring, it refers to its standard basis given by the monomials, . * For finite extension fields, it means the polynomial basis. * In linear algebra, it refers to a set of ''n'' linearly independent generalized eigenvectors of an ''n''×''n'' matrix , if the set is composed entirely of Jordan chains. ==Representation theory==
In representation theory there are several basis that are called "canonical", e.g. Lusztig's canonical basis and closely related Kashiwara's crystal basis in quantum groups and their representations. There is a general concept underlying these basis: Consider the ring of integral Laurent polynomials with its two subrings 抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)』 ■ウィキペディアで「Canonical basis」の詳細全文を読む
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