What Is the Relationship Between the Lie-Algebra of SO(3,1) and SU(2)?

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Discussion Overview

The discussion centers on the relationship between the Lie algebra of the Lorentz group SO(3,1) and the group SU(2). Participants explore the implications of the commutation relations of the generators of these groups, the nature of their representations, and the concept of covering groups in the context of Lie algebras.

Discussion Character

  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant describes the generators of the Lie algebra of SO(3,1) and their commutation relations, suggesting a potential relationship to SU(2).
  • Another participant clarifies that the identity component of SO(3,1) is relevant and notes that SL(2,C) is the complexification of SU(2), which covers the identity component of SO(3,1).
  • A participant expresses confusion about the implications of the Lie algebra of SL(2,C) being a direct sum of the Lie algebra of SU(2), questioning whether this means the groups themselves are direct sums.
  • Another participant responds that an isomorphism of Lie algebras does not imply an isomorphism of the underlying groups, emphasizing that SL(2,C) is not a direct sum of SU(2) groups due to differences in compactness.
  • Participants discuss the concept of complexification and its relation to the structure of the Lie algebras involved.
  • There is a distinction made between representations of the group and its Lie algebra, with a note that lifting representations is generally not straightforward unless the group is simply connected.

Areas of Agreement / Disagreement

Participants generally agree on the definitions and relationships between the Lie algebras, but there is some disagreement regarding the implications for the underlying groups and the nature of representations. The discussion remains unresolved on certain aspects of these relationships.

Contextual Notes

Limitations include the need for clarification on the specific types of representations being discussed and the implications of covering groups in relation to the groups themselves.

Who May Find This Useful

This discussion may be useful for those interested in advanced topics in theoretical physics, particularly in the areas of group theory, representation theory, and the mathematical foundations of quantum mechanics and relativity.

Syrius
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Cheers everybody,

I have a question regarding the Lie-Algebra of the SO(3,1), i.e. the Lorentz group. The generators are denoted by M_{\mu \nu} with M_{\mu \nu} = - M_{\nu \mu} and fulfill the following commutation relations
[M_{\mu \nu}, M_{\rho \sigma}] = g_{\mu \rho} M_{\nu \rho} + g_{\nu \sigma} M_{\mu \rho} - g_{\mu \sigma} M_{\nu \rho} - g_{\nu \rho} M_{\mu \sigma},
where g_{\mu \nu} are metric coefficients.

I can now construct from these generators the operators
\mathbf{J} = (M_{23},M_{31},M_{12}),\ \mathbf{K} = (M_{01},M_{02},M_{03}),
which fulfill the relations
[J_i,J_j] = i \epsilon_{ijk} J_k,\ [K_i,K_j]= -i \epsilon_{ijk} J_k,\ [J_i,K_j]=i \epsilon_{ijk} K_k.

In a final step, I define
\mathbf{J}^\prime = \frac{1}{2} ( \mathbf{J} + i \mathbf{K}),\ \mathbf{K}^\prime = \frac{1}{2} (\mathbf{J} - i \mathbf{K})
with the commutation relations
[J_i^\prime,J_j^\prime] = i \epsilon_{ijk} J_k^\prime,\ [K_i^\prime,K_j^\prime]= i \epsilon_{ijk} K_k^\prime,\ [J_i^\prime, K_j^\prime]=0.

This means that I can construct generators that fulfill exactly the commutation relations of the Lie-Algebra of the SU(2). What does this mean for the group SO(3,1)? Can I deduce from this something like SU(2) x SU(2) is a representation of SO(3,1)?

Greetings, Syrius
 
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Okay, as always, I find the physicist take on these matters to be confusing. What do you mean by SO(3,1), exactly? Since you're concerned with its Lie algebra, I assume you're referring to the identity component of SO(3,1) (i.e. what some people call the "restricted" Lorentz group), since it's all that matters here.

You're noticing the commutation relations of (the Lie algebra of) SU(2) because:
(1) SL(2,C) is the complexification of SU(2), and
(1) SL(2,C) covers (the identity component of) SO(3,1) in the topological sense,
(2) so the (complexified) Lie algebras of SU(2) (which is the complex Lie algebra of SL(2,C)) and (the identity component of) SO(3,1) are the same.

Generally, if a Lie group G covers a Lie group H (both assumed to be connected), then the Lie algebras will be isomorphic, and in fact the differential of the covering map at the identity will implement the isomorphism.

What you can say about representations is a bit delicate. First of all, you really need to clarify whether you're looking for representations of the group or of its Lie algebra.
 
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Hello morphism,

Okay, as always, I find the physicist take on these matters to be confusing. What do you mean by SO(3,1), exactly? Since you're concerned with its Lie algebra, I assume you're referring to the identity component of SO(3,1) (i.e. what some people call the "restricted" Lorentz group), since it's all that matters here.

Yes, I mean the identity component.

You're noticing the commutation relations of (the Lie algebra of) SU(2) because:
(1) SL(2,C) is the complexification of SU(2), and
(1) SL(2,C) covers (the identity component of) SO(3,1) in the topological sense,
(2) so the (complexified) Lie algebras of SU(2) (which is the complex Lie algebra of SL(2,C)) and (the identity component of) SO(3,1) are the same.

Thank you, that helps a lot. So in my own words, since the Lie algebra of SL(2,C) is nothing else than the direct sum of the SU(2) Lie algebra, and SL(2,C) is covering the identity component of SO(3,1), I am getting 6 generators which are equivalent to two times the generators of the SU(2).

Maybe it is a dumb question, but if we find that the Lie Algebra of SL(2,C) is just a direct sum of the Lie algebra of SU(2), what does that mean for the underlying groups. Is the SL(2,C) group then also just the direct sum of SU(2)'s?

And another question: How can I see that SL(2,C) is the complexification of SU(2)?

What you can say about representations is a bit delicate. First of all, you really need to clarify whether you're looking for representations of the group or of its Lie algebra.

I mean here representations of the group.

Many thanks in advance,
Syrius
 
Syrius said:
Maybe it is a dumb question, but if we find that the Lie Algebra of SL(2,C) is just a direct sum of the Lie algebra of SU(2), what does that mean for the underlying groups. Is the SL(2,C) group then also just the direct sum of SU(2)'s?
No. An isomorphism of Lie algebras does not guarantee an isomorphism of the underlying Lie groups; all you get is a cover.

In this specific example it's easy to see that SL(2,C) isn't a direct sum of SU(2)'s: SL(2,C) isn't compact but SU(2) (and hence a direct sum of two SU(2)'s) is.

And another question: How can I see that SL(2,C) is the complexification of SU(2)?
There are a bunch of different definitions of "complexification", but here all we need to know is that SU(2) is a maximal compact subgroup of SL(2,C) and that at the Lie algebra level \mathfrak{sl}(2,\mathbb C) = \mathbb C \otimes \mathfrak{su}(2)= \mathfrak{su}(2) \oplus i \mathfrak{su}(2).

I mean here representations of the group.
In that case, you generally can't "lift" representations from the Lie algebra to the group - not unless the group is simply connected. Generally you will get a representation of some covering group (you can always guarantee a representation of the universal covering group, but sometimes a "smaller" cover might suffice). Do you have a specific question you want answered? (I'm having trouble following what you said towards the end of your original post.)
 
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