Dimension of SO(n) and its generators

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SUMMARY

The dimension of the special orthogonal group ##SO(n)## is definitively established as ##\frac{n(n-1)}{2}##, derived from the properties of antisymmetric ##n \times n## matrices. The Lie algebra ##so(n)##, consisting of these antisymmetric matrices, spans the same dimension, confirming that the degrees of freedom correspond directly to the generators of the group. Furthermore, representations of ##SO(n)##, while potentially varying in form, do not alter the fundamental dimensionality of the group, which is intrinsically linked to the underlying manifold.

PREREQUISITES
  • Understanding of antisymmetric matrices and their properties
  • Familiarity with Lie algebras, specifically ##so(n)##
  • Knowledge of group homomorphisms and representations in linear algebra
  • Basic concepts of differential geometry related to manifolds
NEXT STEPS
  • Study the properties of antisymmetric matrices in depth
  • Learn about the structure and applications of Lie algebras, focusing on ##so(n)##
  • Explore the concept of group representations, particularly finite-dimensional irreducible representations
  • Investigate the relationship between manifolds and their associated Lie groups
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Mathematicians, physicists, and students in advanced linear algebra or differential geometry who are interested in the properties and applications of special orthogonal groups and their representations.

spaghetti3451
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The generators of ##SO(n)## are pure imaginary antisymmetric ##n \times n## matrices.

How can this fact be used to show that the dimension of ##SO(n)## is ##\frac{n(n-1)}{2}##?

I know that an antisymmetric matrix has ##\frac{n(n-1)}{2}## degrees of freedom, but I can't take this idea any further in the demonstration of the proof.

Thoughts?
 
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Consider its tangent space, the Lie Algebra ##so(n)##, or the short exact sequence ##SO(n) → SO(n-1) → S^{n-1}## and prove it by induction.
 
Well, I know that the Lie algebra ##so(n)## is the space of antisymmetric matrices, so that the basis vectors of the algebra are given by the ##\frac{n(n-1)}{2}## degrees of freedom of an ##n \times n## antisymmetric matrix. Therefore, the space ##so(n)## of the antisymmetric matrices is spanned by ##\frac{n(n-1)}{2}## generators. Therefore, the dimension of ##so(n)## is ##\frac{n(n-1)}{2}##. Therefore, the dimension of ##SO(n)## is also ##\frac{n(n-1)}{2}##.

But then, we considered the defining representation of the ##so(n)## algebra, i.e., the representation in terms of ##n \times n## matrices. Does that mean that if we consider representations of other dimensions, they are not necessarily all antisymmetric and hence do not lead to the required number of degrees of freedom?
 
failexam said:
Does that mean that if we consider representations of other dimensions, they are not necessarily all antisymmetric and hence do not lead to the required number of degrees of freedom?

No. Since orthogonality means the transposed matrix is as well the inverse matrix, transposing respects group homomorphisms and therefore any representation of the special orthogonal group is orthogonal of determinate 1 again. One can trivially build

##SO(n) → GL(n) → GL(n+1) → ...##

but that won't change dimensions. Moreover the dimension of ##SO(n)## is defined by the dimension of its underlying manifold which isn't affected by any representations of ##SO(n)##.
 
So, what you are saying is that representations of any dimension are possible for ##SO(n)## and that they are all not necessarily antisymmetric.

But, since the number of dimensions of ##SO(n)## is a property of the underlying manifold of ##SO(n)##, the number of dimensions of ##SO(n)## remains is the same for all representations.

Is that it?
 
Yes and ("... and that they are all not necessarily antisymmetric.") NO!

For any representation φ you can always build a representation

$$\begin{pmatrix}
1 & 0 & ... & 0\\
0 & 1 & ... & 0\\
...& ...& ... & ...\\
0 & 0 & 0 & φ
\end{pmatrix}$$

However you should look up your definition of representation. Strictly speaking its an analytic group homomorphism ##φ : SO(n) → GL(V)##. But sometimes it's required to be in ##GL(V)_ℝ## the real Lie group underlying the complex Lie group ##GL(V)##.

Nevertheless if you read my post again, I've proved that still ##φ(X) φ(X)^τ = 1## holds!
 
When I asked if representations of any dimension are possible and if they are not necessarily antisymmetric, I was referring to finite-dimensional irreducible representations actually!
 
failexam said:
When I asked if representations of any dimension are possible and if they are not necessarily antisymmetric, I was referring to finite-dimensional irreducible representations actually!
What has irreducibility to do with it?

(https://en.wikipedia.org/wiki/Spin_representation)
 
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