Non-Commutative Hilbert Nullstellensatz?

  • Thread starter Thread starter "pi"mp
  • Start date Start date
  • Tags Tags
    Hilbert
Click For Summary
SUMMARY

The discussion revolves around the existence of a non-commutative analog of Hilbert's Nullstellensatz, a fundamental theorem in algebraic geometry that connects commutative algebra with algebraic varieties. Participants explore the challenges of defining non-commutative spaces using algebras such as the Heisenberg algebra and the angular momentum algebra (SU(2)). Key points include the necessity of a "symbol map" to relate non-commutative algebras to functions on commutative manifolds, and the complexities involved in establishing well-defined correspondences between these mathematical structures.

PREREQUISITES
  • Understanding of Hilbert's Nullstellensatz in commutative algebra.
  • Familiarity with non-commutative algebra, specifically the Heisenberg algebra and SU(2) algebra.
  • Basic knowledge of algebraic geometry and its terminology.
  • Concept of "symbol maps" in the context of non-commutative geometry.
NEXT STEPS
  • Research the implications of Hilbert's Nullstellensatz in non-commutative algebra.
  • Study the properties and applications of the Heisenberg algebra in geometry.
  • Explore the concept of "fuzzy geometry" and its mathematical foundations.
  • Investigate the role of symbol maps in relating non-commutative algebras to commutative manifolds.
USEFUL FOR

Mathematicians, algebraic geometers, and researchers interested in the intersections of non-commutative algebra and geometry, particularly those exploring advanced concepts in algebraic structures.

"pi"mp
Messages
129
Reaction score
1
Hi,
In my very naive understanding of algebraic geometry, I get the impression that it's written in language of commutative algebra and the main theorem (at least at the basic level) is Hilbert's Nullstellensatz. I'm curious if there's an analog of the Nullstellensatz for non-commutative algebra/geometry?

What I'm envisioning would be a correspondence between some operator/matrix algebra and a "fuzzy" geometry.
Thanks!
 
Physics news on Phys.org
(nonsense removed)
 
Last edited:
Thanks! But I still have some confusions:

--I had never thought of the Nullstellensatz as having to do with functions defined on a variety. I had thought it was just a correspondence between commutative rings and algebraic varieties. Is there a direct analog of the vanishing set of polynomials in the non-commutative case?

--Also, you talk about defining a non-commutative space by starting with a non-commutative algebra as the functions on the space. But I vaguely remember reading somewhere that the problem with this is that not all non-commutative geometries will have functions defined on them that form a non-commutative algebra. Is this wrong?
 
I think.you are right, I took too much of a shortcut here. Interesting question, need to think about this.

Edit : actually, what I said is just wrong, sorry about that.
 
Last edited:
No worries, thank you. It seems like the standard procedure is to start with some non-commutative algebra, like the Heisenberg algebra or the angular momentum algebra, and define a "symbol map" that associates an element in this algebra to a function on the ordinary commutative manifold. Now, from what I read this certainly isn't a unique map, but I don't even understand how it can be well defined! It seems like you need to know before hand what the fuzzy geometry is going to be in order to use this. i.e. you need to know that the Heisenberg algebra will yield the non-commutative plane and that the angular momentum SU(2) algebra will yield the non-commutative sphere.

I'm not very clever with mathematical details, but I can usually appreciate the general program of some field. This I'm completely lost on!
 
I am studying the mathematical formalism behind non-commutative geometry approach to quantum gravity. I was reading about Hopf algebras and their Drinfeld twist with a specific example of the Moyal-Weyl twist defined as F=exp(-iλ/2θ^(μν)∂_μ⊗∂_ν) where λ is a constant parametar and θ antisymmetric constant tensor. {∂_μ} is the basis of the tangent vector space over the underlying spacetime Now, from my understanding the enveloping algebra which appears in the definition of the Hopf algebra...

Similar threads

Replies
2
Views
2K
  • · Replies 3 ·
Replies
3
Views
1K
  • · Replies 4 ·
Replies
4
Views
2K
  • · Replies 26 ·
Replies
26
Views
5K
Replies
2
Views
2K
  • · Replies 2 ·
Replies
2
Views
3K
  • · Replies 2 ·
Replies
2
Views
14K
  • · Replies 5 ·
Replies
5
Views
2K
  • Poll Poll
  • · Replies 4 ·
Replies
4
Views
8K
  • Poll Poll
  • · Replies 3 ·
Replies
3
Views
8K