How Many Parameters Define O(N) and SO(N) Groups?

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SUMMARY

The number of group parameters for O(N) and SO(N) is defined as \(\frac{N(N-1)}{2}\). This conclusion arises from the analysis of the matrix equation \(O^T O = 1\), which generates \(n^2\) parameters and imposes \(\frac{n(n+1)}{2}\) constraints. The determinant conditions for O(N) and SO(N) do not impose additional constraints beyond those already accounted for. The discussion highlights the derivation of constraints through symmetry and arithmetic series, confirming the established formula for any N.

PREREQUISITES
  • Understanding of group theory concepts, specifically O(N) and SO(N)
  • Familiarity with matrix operations and properties, particularly orthogonal matrices
  • Basic knowledge of determinants and their implications in linear algebra
  • Experience with mathematical proofs and constraints in theoretical physics
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  • Study the derivation of constraints in O(N) and SO(N) using linear algebra techniques
  • Explore advanced group theory texts, focusing on applications in quantum field theory
  • Investigate the implications of determinants in the context of Lie groups and algebras
  • Learn about the role of symmetry in physics and its mathematical representation
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Physicists, mathematicians, and students of theoretical physics who are interested in group theory, particularly in its applications to quantum field theory and the mathematical foundations of symmetry in physical systems.

Norman
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A little intro: This is for a whirlwind intro to Group Theory as part of another class (QFT) in which we are not proving anything, simply introducing definitions and theorems. We are not using a textbook, simply some notes the professor has written up for this intro and the notes are very incomplete. They also do not give any proof or explanation. So here is the problem:

Show that the number of group parameters for [tex]O(N)[/tex] and [tex]SO(N)[/tex] are [tex]\frac{N(N-1)}{2}[/tex]

Does this make sense as the solution:

We have [tex]n^2[/tex] parameters. For [tex]O(N)[/tex] we have the condition that [tex]O^T O = 1[/tex]. This condition places [tex]\frac{n(n+1)}{2}[/tex] constraints on the parameters. This leaves [tex]n^2 - \frac{n(n+1)}{2} = \frac{n(n-1)}{2}[/tex]

Since [tex]O(N)[/tex] has [tex]detO(N) = \pm 1[/tex] and [tex]SO(N)[/tex] has [tex]detSO(N)=+1[/tex], simply picking the sign of the determinent doesn't force any additional constraint on the parameters.

I can only show this statement: "This condition places [tex]\frac{n(n+1)}{2}[/tex] constraints on the parameters." for specific examples, like N=2 and 3. I can see how it is extended to higher orders, but I cannot prove it in the general case for N. Any ideas? Also, any good books on Group Theory and Lie Algebras for Physicists?
Thanks,
Ryan
 
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The matrix equation O^T O = 1 gives n^2 scalar equations - one for each element of the identity matrix. By symmetry, the equations for the elements below the main diagonal are the same as the equations above the main diagonal, so the number of constraint equations is the the number of elements on the main diagonal, n, plus the number of elements above the main diagonal, say x. x equals the total number of elements in the matrix minus the number of elements on the diagonal, all divided by 2, i.e., x = (n^2 - n)/2.

Cosequently, the number of contraint equations is

n + x = n(n + 1)/2.

Another way to calculate this is using an arithmetic series. The number of constraint equation for the top row of the identity matrix is n. The number of constraint equations for the second row of the identity matrix is n - 1, the number of elements in this row starting with the main diagonal and moving right, etc. So the total number of constraint equations is

n + (n -1) + (n - 2) + ... + 2 + 1 = n(n + 1)/2.

Regards,
George
 

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