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<table><TR><TD valign="top">[1]</TD> <TD valign="top">  G.B. Gurevich,  "Foundations of the theory of algebraic invariants" , Noordhoff  (1964)  (Translated from Russian)</TD></TR><TR><TD valign="top">[2]</TD> <TD valign="top">  D. Mumford,  "Geometric invariant theory" , Springer  (1965)</TD></TR><TR><TD valign="top">[3]</TD> <TD valign="top">  J.A. Dieudonné,  "La géométrie des groups classiques" , Springer  (1955)</TD></TR></table>
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<table><TR><TD valign="top">[1]</TD> <TD valign="top">  G.B. Gurevich,  "Foundations of the theory of algebraic invariants" , Noordhoff  (1964)  (Translated from Russian) {{MR|0183733}} {{ZBL|0128.24601}} </TD></TR><TR><TD valign="top">[2]</TD> <TD valign="top">  D. Mumford,  "Geometric invariant theory" , Springer  (1965) {{MR|0214602}} {{ZBL|0147.39304}} </TD></TR><TR><TD valign="top">[3]</TD> <TD valign="top">  J.A. Dieudonné,  "La géométrie des groups classiques" , Springer  (1955) {{MR|}} {{ZBL|0221.20056}} </TD></TR></table>

Revision as of 10:02, 24 March 2012

concomitant of a group acting on sets and

A mapping such that

for any , . In this case one also says that commutes with the action of , or that is an equivariant mapping. If acts on every set of a family , then a comitant is called a simultaneous comitant of .

The notion of a comitant originates from the classical theory of invariants (cf. Invariants, theory of) in which, however, a comitant is understood in a narrower sense: is the general linear group of some finite-dimensional vector space , and are tensor spaces on of specified (generally distinct) types, on which acts in the natural way, while is an equivariant polynomial mapping from into . If, in addition, is a space of covariant tensors, then the comitant is called a covariant of , while if is a space of contravariant tensors, the comitant is called a contravariant of .

Example. Let be a binary cubic form in the variables and :

Its coefficients are the coordinates of a covariant symmetric tensor. The coefficients of the Hessian form of , that is, of the form

are also the coefficients of a covariant symmetric tensor, while the mapping

of the corresponding tensor spaces is a comitant (the so-called comitant of the form ). The Hessian of an arbitrary form can similarly be defined; this also provides an example of a comitant (see Covariant).

In the modern geometric theory of invariants, by a comitant one often means any equivariant morphism , where and are algebraic varieties endowed with a regular action of an algebraic group . If and are affine, then giving a comitant is equivalent to giving a homomorphism of -modules of regular functions on the varieties and , respectively (where is the ground field).

References

[1] G.B. Gurevich, "Foundations of the theory of algebraic invariants" , Noordhoff (1964) (Translated from Russian) MR0183733 Zbl 0128.24601
[2] D. Mumford, "Geometric invariant theory" , Springer (1965) MR0214602 Zbl 0147.39304
[3] J.A. Dieudonné, "La géométrie des groups classiques" , Springer (1955) Zbl 0221.20056
How to Cite This Entry:
Comitant. Encyclopedia of Mathematics. URL: http://encyclopediaofmath.org/index.php?title=Comitant&oldid=15732
This article was adapted from an original article by V.L. Popov (originator), which appeared in Encyclopedia of Mathematics - ISBN 1402006098. See original article