Finding Cartan Subalgebras for Matrix Algebras

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SUMMARY

This discussion focuses on finding Cartan subalgebras for the matrix algebras ##\mathfrak{u}(n)##, ##\mathfrak{su}(n)##, ##\mathfrak{so}(n)##, and ##\mathfrak{so}(1,3)## as posed in Robin Ticciati's "Quantum Field Theory for Mathematicians." The Cartan subalgebra for ##\mathfrak{u}(n)## is established as having dimension ##n##, while for ##\mathfrak{su}(n)##, it is ##n-1## due to the zero trace condition. The discussion highlights the challenge in determining the Cartan subalgebra for ##\mathfrak{so}(n)##, where diagonalization is not straightforward. The dimensions of the Cartan subalgebras are confirmed as ##n##, ##n-1##, ##[n/2]##, and ##2## respectively.

PREREQUISITES
  • Understanding of Lie algebras, specifically ##\mathfrak{u}(n)## and ##\mathfrak{su}(n)##
  • Knowledge of anti-hermitian matrices and their properties
  • Familiarity with the concept of Cartan subalgebras
  • Basic understanding of diagonalization in linear algebra
NEXT STEPS
  • Study the properties of Cartan subalgebras in different Lie algebras
  • Learn about the structure and classification of Lie algebras
  • Explore the implications of zero trace in matrix algebras, particularly in ##\mathfrak{su}(n)##
  • Investigate methods for finding Cartan subalgebras in non-diagonalizable cases, such as ##\mathfrak{so}(n)##
USEFUL FOR

Mathematicians, physicists, and students studying quantum field theory or Lie algebras, particularly those interested in the structure and properties of matrix algebras.

leo.
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Homework Statement
Homework 6.2.30 (Quantum Field Theory for Mathematicians by Robin Ticciati): Find Cartan subalgebras of ##\mathfrak{u}(n), \mathfrak{su}(n),\mathfrak{so}(n)## and ##\mathfrak{so}(1,3)##. Show that these subalgebras have dimensions ##n,n-1,[n/2]## (the greatest integer less than ##n/2##), and ##2## respectively.
Relevant Equations
Definition of a Cartan subalgebra: A Cartan subalgebra of a Lie algebra ##\mathfrak{g}## is a maximal commutative Lie subalgebra of ##\mathfrak{g}##.
This is one problem from Robin Ticciati's Quantum Field Theory for Mathematicians essentially asking us to find Cartan subalgebras for the matrix algebras ##\mathfrak{u}(n), \mathfrak{su}(n),\mathfrak{so}(n)## and ##\mathfrak{so}(1,3)##. The only thing he gives is the definition of a Cartan subalgebra so I guess we should work from there.

The cases ##\mathfrak{u}(n)## and ##\mathfrak{su}(n)## I think I got correctly. Let's consider ##\mathfrak{u}(n)##, it is the Lie algebra of the unitary group ##U(n)## and so its elements are anti-hermitian matrices. Now let ##\{X_a\}\subset \mathfrak{u}(n)## be a set of linearly independent commuting matrices. Since the matrices are anti-hermitian we can diagonalize them simultaneously. This means from ##\{X_a\}## we can build ##\{X_a'\}## a set of linearly independent diagonal matrices. The maximal set cardinality seems intuitively to be the number of diagonal entries and we can take the set $$X_1 = \operatorname{diag}(i,0,\dots, 0),X_2 = \operatorname{diag}(0,i,\dots, 0),\ \dots \ ,X_n = \operatorname{diag}(0,\dots, 0, i).$$ So I guess for ##\mathfrak{u}(n)## the subalgebra generated by ##\{X_a\}## is a Cartan subalgebra and its dimension is ##n##.

For ##\mathfrak{su}(n)## everything goes the same, but now the matrices must have zero trace. A way to ensure this is to take as basis elements $$X_1 = \operatorname{diag}(i,-i,\dots, 0),X_2 = \operatorname{diag}(0,i,-i,\dots, 0),\ \dots \ , X_{n-1} = \operatorname{diag}(0,\dots, i,-i)$$
and clearly we have just one less generator. So we get ##\mathfrak{su}(n)## a Cartan subalgebra of dimension ##n-1##.

Now for ##\mathfrak{so}(n)## I have no idea what to do. The thing is that for ##\mathfrak{u}(n),\mathfrak{su}(n)## since the matrices were anti-hermitian, commuting sets are in a sense equivalent to sets of simultaneously diagonal matrices. So we could look for sets of diagonal matrices which are much simpler. For ##\mathfrak{so}(n)## this is not the case.

So how can I proceed to solve this? Is my solution for ##\mathfrak{u}(n),\mathfrak{su}(n)## correct? Can the argument be improved? And what about ##\mathfrak{so}(n)##? How do we proceed to find a Cartan subalgebra without resorting to diagonalization?
 
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leo. said:
Homework Statement: Homework 6.2.30 (Quantum Field Theory for Mathematicians by Robin Ticciati): Find Cartan subalgebras of ##\mathfrak{u}(n), \mathfrak{su}(n),\mathfrak{so}(n)## and ##\mathfrak{so}(1,3)##. Show that these subalgebras have dimensions ##n,n-1,[n/2]## (the greatest integer less than ##n/2##), and ##2## respectively.
Homework Equations: Definition of a Cartan subalgebra: A Cartan subalgebra of a Lie algebra ##\mathfrak{g}## is a maximal commutative Lie subalgebra of ##\mathfrak{g}##.

This is one problem from Robin Ticciati's Quantum Field Theory for Mathematicians essentially asking us to find Cartan subalgebras for the matrix algebras ##\mathfrak{u}(n), \mathfrak{su}(n),\mathfrak{so}(n)## and ##\mathfrak{so}(1,3)##. The only thing he gives is the definition of a Cartan subalgebra so I guess we should work from there.

The cases ##\mathfrak{u}(n)## and ##\mathfrak{su}(n)## I think I got correctly. Let's consider ##\mathfrak{u}(n)##, it is the Lie algebra of the unitary group ##U(n)## and so its elements are anti-hermitian matrices. Now let ##\{X_a\}\subset \mathfrak{u}(n)## be a set of linearly independent commuting matrices. Since the matrices are anti-hermitian we can diagonalize them simultaneously. This means from ##\{X_a\}## we can build ##\{X_a'\}## a set of linearly independent diagonal matrices. The maximal set cardinality seems intuitively to be the number of diagonal entries and we can take the set $$X_1 = \operatorname{diag}(i,0,\dots, 0),X_2 = \operatorname{diag}(0,i,\dots, 0),\ \dots \ ,X_n = \operatorname{diag}(0,\dots, 0, i).$$ So I guess for ##\mathfrak{u}(n)## the subalgebra generated by ##\{X_a\}## is a Cartan subalgebra and its dimension is ##n##.
Unitary means ##U^\dagger U=1## which becomes ##A^\dagger + A = 0## for the Lie algebra. This means skew symmetric matrices. ##\mathfrak{u}(n)## is of dimension ##\dfrac{n(n-1)}{2}##. The CSA is of dimension ##n-1## (I think), but still a subalgebra, so the main diagonal has to be zero.
For ##\mathfrak{su}(n)## everything goes the same, but now the matrices must have zero trace.
Yes. It is basically the same CSA as ##\det U=\pm 1## becomes the only condition ##\operatorname{tr}A=0##. Hence it is the same Lie algebra, although not the same Lie group.
A way to ensure this is to take as basis elements $$X_1 = \operatorname{diag}(i,-i,\dots, 0),X_2 = \operatorname{diag}(0,i,-i,\dots, 0),\ \dots \ , X_{n-1} = \operatorname{diag}(0,\dots, i,-i)$$
and clearly we have just one less generator. So we get ##\mathfrak{su}(n)## a Cartan subalgebra of dimension ##n-1##.

Now for ##\mathfrak{so}(n)## I have no idea what to do. The thing is that for ##\mathfrak{u}(n),\mathfrak{su}(n)## since the matrices were anti-hermitian, commuting sets are in a sense equivalent to sets of simultaneously diagonal matrices. So we could look for sets of diagonal matrices which are much simpler. For ##\mathfrak{so}(n)## this is not the case.

So how can I proceed to solve this? Is my solution for ##\mathfrak{u}(n),\mathfrak{su}(n)## correct? Can the argument be improved? And what about ##\mathfrak{so}(n)##? How do we proceed to find a Cartan subalgebra without resorting to diagonalization?

If you want to read more about Lie algebras, see
https://www.physicsforums.com/insights/lie-algebras-a-walkthrough-the-basics/#toggle-id-1
 

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