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Sesquilinear form
In mathematics, a sesquilinear form is a generalization of a bilinear form that, in turn, is a generalization of the concept of the dot product of Euclidean space. A bilinear form is linear in each of its arguments, but a sesquilinear form allows one of the arguments to be "twisted" in a semilinear manner, thus the name; which originates from the Latin numerical prefix ''sesqui-'' meaning "one and a half". The basic concept of the dot product – producing a scalar from a pair of vectors – can be generalized by allowing a broader range of scalar values and, perhaps simultaneously, by widening the definition of what a vector is.
A motivating special case is a sesquilinear form on a complex vector space, . This is a map that is linear in one argument and "twists" the linearity of other argument by complex conjugation (referred to as being antilinear in the other argument). This case arises naturally in mathematical physics applications. Another important case allows the scalars to come from any field and the twist is provided by a field automorphism. Many authors assume that this automorphism is an involution (has order two) to stay in analogy with the complex case, but others prove this property when introducing Hermitian forms.
An application in projective geometry requires that the scalars come from a division ring (skewfield), , and this means that the "vectors" should be replaced by elements of a . In a very general setting, sesquilinear forms can be defined over -modules for arbitrary rings .
==Convention==
Conventions differ as to which argument should be linear. We shall take the first to be linear, as is common in the mathematical literature, except in the section devoted to sesquilinear forms on complex vector spaces. There we use the other convention and take the first argument to be conjugate-linear (i.e. antilinear) and the second to be linear. This is the convention used mostly by mathematical physicists〔footnote 1 in ( Anthony Knapp ''Basic Algebra'' (2007) pg. 255 )〕 and originates in Dirac's bra–ket notation in quantum mechanics.
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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