Does the Picard Group Vanish for Semilocal Rings?

  • Thread starter Thread starter Hurkyl
  • Start date Start date
  • Tags Tags
    Group Rings
Click For Summary
In the discussion on whether the Picard group vanishes for dimension 1 regular semi-local rings, it is concluded that the Picard group does indeed vanish. A dimension 1 regular ring is identified as a Dedekind domain, which implies that a semi-local Dedekind domain is a principal ideal domain (PID). Since the Picard group of a PID is known to vanish, this supports the conclusion. The conversation also raises questions about the behavior of the Picard group in non-regular cases and higher dimensions, but the primary focus remains on dimension 1 regular semi-local rings. Overall, the consensus affirms the vanishing of the Picard group in this specific case.
Hurkyl
Staff Emeritus
Science Advisor
Gold Member
Messages
14,922
Reaction score
28
For a dimension 1 regular semi-local ring, does the Picard group vanish?

What if it is not regular? (and what if I ask for the ideal class group?)
What if it's dimension greater than 1?
 
Physics news on Phys.org
Hurkyl said:
For a dimension 1 regular semi-local ring, does the Picard group vanish?

What if it is not regular? (and what if I ask for the ideal class group?)
What if it's dimension greater than 1?

I don't know very much about this. But I think that the Picard group does vanish. A dimension 1 regular ring is a Dedekind domain. And it's known that a semi-local Dedekind domain is a PID. And the Picard group of a PID vanishes.
 
micromass said:
I don't know very much about this. But I think that the Picard group does vanish. A dimension 1 regular ring is a Dedekind domain. And it's known that a semi-local Dedekind domain is a PID. And the Picard group of a PID vanishes.

Excellent. I thought my first question was an easy one, but for the life of me I couldn't find any references for it, and I kept getting tripped up in my attempts to prove it (e.g. that a semi-local Dedekind domain is a PID).
 
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 4 ·
Replies
4
Views
2K
  • · Replies 3 ·
Replies
3
Views
883
  • · Replies 1 ·
Replies
1
Views
534
  • · Replies 6 ·
Replies
6
Views
1K
  • · Replies 17 ·
Replies
17
Views
6K
  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 21 ·
Replies
21
Views
1K
  • · Replies 10 ·
Replies
10
Views
2K
  • · Replies 5 ·
Replies
5
Views
1K
  • · Replies 3 ·
Replies
3
Views
1K