Can the Direct Sum of Non-Commuting Lie Algebras be Used in L(SO(4))?

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Homework Help Overview

The discussion revolves around the structure of the Lie algebra L(SO(4)) and its relationship to the Lie algebras L(SU(2)). The original poster attempts to understand whether the direct sum of two non-commuting Lie algebras can be used in this context.

Discussion Character

  • Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • Participants explore the properties of the direct sum of Lie algebras and question the necessity of commutation between the algebras involved. The original poster presents a specific case involving matrices and commutation relations, while another participant provides a general framework for forming direct sums and defining commutators.

Discussion Status

The discussion includes attempts to clarify the conditions under which direct sums of Lie algebras can be formed. Some participants provide insights into the vector space structure and commutator definitions, while others seek further understanding of the implications for the specific case of L(SO(4)).

Contextual Notes

The original poster references a hint involving antisymmetric matrices and specific commutation relations, indicating a focus on the algebraic structure of L(SO(4)) in relation to L(SU(2)).

deadringer
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We are asked to show that L(SO(4)) = L(SU(2)) (+) L(SU(2))

where L is the Lie algebra and (+) is the direct product.

We are given the hint to consider the antisymmetric 4 by 4 matrices where each row and column has a single 1/2 or -1/2 in it.

By doing this we generate four matrices, call them S1, S2, T1, T2
we can show that the commutator of S1, S2 generates another matrix S3 and that the same occurs for the T's. We can show that the 6 matrices form a general basis for L(SO(4))

we then get the following commutation relations:

[Sa, Sb] = epsilon(a,b,c) Sc
[Ta, Tb] = epsilon(a,b,c) Tc
and [Ta, Sb] = 0

We can then see that the S and T matrices form a basis for L(SU(2)) as they obey the correct commutation relations, and therefore the direct sum of these two Lie algebras forms the lie algebra for L(SO(4)).

My question is if we require the two L(SU(2))'s to commute (as they in this case do) in order use their direct sum, or is it okay to take a direct sum of two non-commuting lie algebras. thanks
 
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Let L_1 and L_2 be any Lie algebras. Since L_1 and L_2 are vector spaces, the external vector space direct sum L_1 \oplus L_2 can be formed. The underlying set for the vector space direct sum is

L_1 \times L_2 = \left\{ \left( x,y \right) | x \in L_1, y \in L_2 \right\}.

In order for this set to have vector space structure, scalar multiplication and addition of ordered pairs must be defined. This is done in a natural way:

c \left( x,y \right) := \left( cx,cy \right);

\left( x_1,y_1 \right) + \left( x_2,y_2 \right) := \left( x_1 + x_2,y_1 + y_2 \right).

Now in order to get a Lie algebra, a commutator must be defined on ordered pairs:

\left[\left( x_1,y_1 \right) , \left( x_2,y_2 \right)\right] := \left( \left[x_1,x_2\right] , \left[y_1,y_2\right]\right).

Note that

\left[\left( x , 0 \right) , \left( 0,y \right)\right] = \left( \left[x , 0\right] , \left[0,y\right \right)] = 0.
 
Last edited:
thanks, I've got it now
 
How would you show those 6 matrices forma a basis in so(4) ?
 

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