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In [[mathematics]], if ''G'' is a [[group (mathematics)|group]] and &rho; is a [[representation theory|representation]] of it over the [[complex number|complex]] [[vector space]] V, then the '''complex conjugate representation''' &rho;* is defined over the [[conjugate vector space]] V* as follows:
 
:&rho;*(''g'') is the [[conjugate linear map|conjugate]] of &rho;(''g'') for all ''g'' in ''G''.
 
&rho;* is also a representation, as you may check explicitly.
 
If <math>\mathfrak{g}</math> is a [[real number|real]] [[Lie algebra]] and &rho; is a representation of it over the vector space ''V'', then the conjugate representation &rho;* is defined over the conjugate vector space ''V''* as follows:
 
:&rho;*(''u'') is the conjugate of &rho;(''u'') for all ''u'' in <math>\mathfrak{g}</math>.<ref>This is the mathematicians' convention. Physicists use a different convention where the [[Lie bracket of vector fields|Lie bracket]] of two real vectors is an imaginary vector. In the physicist's convention, insert a minus in the definition.</ref>
 
&rho;* is also a representation, as you may check explicitly.
 
If two real Lie algebras have the same [[complexification]], and we have a complex representation of the complexified Lie algebra, their conjugate representations are still going to be different. See [[spinor]] for some examples associated with spinor representations of the [[spin group]]s Spin(p+q) and Spin(p,q).
 
If <math>\mathfrak{g}</math> is a *-Lie algebra (a complex Lie algebra with a * operation which is compatible with the Lie bracket),
 
:&rho;*(''u'') is the conjugate of &minus;&rho;(''u''*) for all ''u'' in <math>\mathfrak{g}</math>
 
For a [[unitary representation]], the dual representation and the conjugate representation coincide.
 
==See also==
 
*[[Dual representation]]
 
==Notes==
<references/>
[[Category:Representation theory of groups]]

Revision as of 23:27, 16 January 2014

In mathematics, if G is a group and ρ is a representation of it over the complex vector space V, then the complex conjugate representation ρ* is defined over the conjugate vector space V* as follows:

ρ*(g) is the conjugate of ρ(g) for all g in G.

ρ* is also a representation, as you may check explicitly.

If is a real Lie algebra and ρ is a representation of it over the vector space V, then the conjugate representation ρ* is defined over the conjugate vector space V* as follows:

ρ*(u) is the conjugate of ρ(u) for all u in .[1]

ρ* is also a representation, as you may check explicitly.

If two real Lie algebras have the same complexification, and we have a complex representation of the complexified Lie algebra, their conjugate representations are still going to be different. See spinor for some examples associated with spinor representations of the spin groups Spin(p+q) and Spin(p,q).

If is a *-Lie algebra (a complex Lie algebra with a * operation which is compatible with the Lie bracket),

ρ*(u) is the conjugate of −ρ(u*) for all u in

For a unitary representation, the dual representation and the conjugate representation coincide.

See also

Notes

  1. This is the mathematicians' convention. Physicists use a different convention where the Lie bracket of two real vectors is an imaginary vector. In the physicist's convention, insert a minus in the definition.