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A unital algebra <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/q/q120/q120030/q1200301.png" /> that is a co-module for a quantum group <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/q/q120/q120030/q1200302.png" /> (cf. [[Quantum groups|Quantum groups]]) and for which the structure mapping <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/q/q120/q120030/q1200303.png" /> is an algebra homomorphism, i.e., <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/q/q120/q120030/q1200304.png" /> is a co-module algebra [[#References|[a1]]]. Here, <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/q/q120/q120030/q1200305.png" /> is a deformation of the [[Poisson algebra|Poisson algebra]] <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/q/q120/q120030/q1200306.png" />, of a Poisson–Lie group <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/q/q120/q120030/q1200307.png" />, endowed with the structure of a Hopf algebra with a co-multiplication <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/q/q120/q120030/q1200308.png" /> and a co-unit <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/q/q120/q120030/q1200309.png" />. Often, both <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/q/q120/q120030/q12003010.png" /> and <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/q/q120/q120030/q12003011.png" /> can also be equipped with a <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/q/q120/q120030/q12003013.png" />-involution. The left co-action <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/q/q120/q120030/q12003014.png" /> satisfies
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A [[unital algebra]] <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/q/q120/q120030/q1200301.png" /> that is a [[co-module]] for a quantum group <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/q/q120/q120030/q1200302.png" /> (cf. [[Quantum groups|Quantum groups]]) and for which the structure mapping <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/q/q120/q120030/q1200303.png" /> is an algebra homomorphism, i.e., <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/q/q120/q120030/q1200304.png" /> is a co-module algebra [[#References|[a1]]]. Here, <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/q/q120/q120030/q1200305.png" /> is a deformation of the [[Poisson algebra|Poisson algebra]] <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/q/q120/q120030/q1200306.png" />, of a Poisson–Lie group <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/q/q120/q120030/q1200307.png" />, endowed with the structure of a Hopf algebra with a co-multiplication <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/q/q120/q120030/q1200308.png" /> and a co-unit <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/q/q120/q120030/q1200309.png" />. Often, both <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/q/q120/q120030/q12003010.png" /> and <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/q/q120/q120030/q12003011.png" /> can also be equipped with a <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/q/q120/q120030/q12003013.png" />-involution. The left co-action <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/q/q120/q120030/q12003014.png" /> satisfies
  
 
<table class="eq" style="width:100%;"> <tr><td valign="top" style="width:94%;text-align:center;"><img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/q/q120/q120030/q12003015.png" /></td> </tr></table>
 
<table class="eq" style="width:100%;"> <tr><td valign="top" style="width:94%;text-align:center;"><img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/q/q120/q120030/q12003015.png" /></td> </tr></table>

Revision as of 16:13, 12 April 2017

A unital algebra that is a co-module for a quantum group (cf. Quantum groups) and for which the structure mapping is an algebra homomorphism, i.e., is a co-module algebra [a1]. Here, is a deformation of the Poisson algebra , of a Poisson–Lie group , endowed with the structure of a Hopf algebra with a co-multiplication and a co-unit . Often, both and can also be equipped with a -involution. The left co-action satisfies

These relations should be modified correspondingly for a right co-action. In the dual picture, if is the deformed universal enveloping algebra of the Lie algebra and is a non-degenerate dual pairing between the Hopf algebras and , then the prescription , with and , defines a right action of on () and one has

where is the multiplication in and is the co-multiplication in . Typically, is a deformation of the Poisson algebra (frequently called the quantization of ), where is a Poisson manifold and, at the same time, a left homogeneous space of with the left action a Poisson mapping.

It is not quite clear how to translate into purely algebraic terms the property that is a homogeneous space of . One possibility is to require that only multiples of the unit satisfy . A stronger condition requires the existence of a linear functional such that while the linear mapping be injective. Then can be considered as a base point.

The still stronger requirement that, in addition, be a homomorphism (a so-called classical point) holds when is a quantization of a Poisson homogeneous space with a Poisson–Lie subgroup. The quantum homogeneous space is defined as the subalgebra in formed by -invariant elements , where is a Hopf-algebra homomorphism.

A richer class of examples is provided by quantization of orbits of the dressing transformation of , acting on its dual Poisson–Lie group (also called the generalized Pontryagin dual) . The best studied cases concern the compact and solvable factors and ( and are mutually dual) in the Iwasawa decomposition , where is a simple complex Lie group. One obtains this way, among others, the quantum sphere and, more generally, quantum Grassmannian and quantum flag manifolds.

There is a vast amount of literature on this subject. The survey book [a2] contains a rich list of references.

References

[a1] E. Abe, "Hopf algebras" , Cambridge Univ. Press (1977)
[a2] V. Chari, A. Pressley, "A guide to quantum groups" , Cambridge Univ. Press (1994)
How to Cite This Entry:
Quantum homogeneous space. Encyclopedia of Mathematics. URL: http://encyclopediaofmath.org/index.php?title=Quantum_homogeneous_space&oldid=11401
This article was adapted from an original article by Pavel Štovíček (originator), which appeared in Encyclopedia of Mathematics - ISBN 1402006098. See original article