Completeness relation for SO(N)

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In summary, the conversation discusses the completeness relation for the fundamental representation of SO(N) and its non-existence in contrast to the existence in SU(N). The conversation also mentions a paper by C.C. Nishi which explains this further, along with a formula for the generators in the fundamental representation.
  • #1
Einj
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Hello everyone,
I was wondering if anyone knows what the completeness relation for the fundamental representation of SO(N) is.
For example, in the SU(N) we know that, if [itex]T^a_{ij}[/itex] are the generators of the fundamental representation then we have the following relation
$$
T^a_{ij}T^a_{km}=\frac{1}{2}\left(\delta_{im}\delta_{jk}-\frac{1}{N}\delta_{ij}\delta_{km}\right)
$$
This follows from the fact that the [itex]T^a[/itex], together with the identity form a complete basis for the [itex]N\times N[/itex] complex matrices.

Does anyone know how to find the analogous for SO(N) (if any)?

Thanks a lot!
 
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  • #2
There is not an analogue. See http://repositorio.unesp.br/bitstream/handle/11449/23433/WOS000234099500010.pdf?sequence=1 by C. C. Nishi
equation 22 and the paragraph following it.
 
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  • #3
Einj said:
Hello everyone,
I was wondering if anyone knows what the completeness relation for the fundamental representation of SO(N) is.
For example, in the SU(N) we know that, if [itex]T^a_{ij}[/itex] are the generators of the fundamental representation then we have the following relation
$$
T^a_{ij}T^a_{km}=\frac{1}{2}\left(\delta_{im}\delta_{jk}-\frac{1}{N}\delta_{ij}\delta_{km}\right)
$$
This follows from the fact that the [itex]T^a[/itex], together with the identity form a complete basis for the [itex]N\times N[/itex] complex matrices.

Does anyone know how to find the analogous for SO(N) (if any)?

Thanks a lot!

Such a relation you can obtain in fundamental rep by yourself just using definition of generators
$$
(\lambda_{ab})_{cd}=-i(\delta_{ac}\delta_{bd}-\delta_{ad}\delta_{bc}) \in so(n).
$$
By contracting with an other $\lambda_{ab})_{$ you get
$$
(\lambda_{ab})_{cd}(\lambda_{ab})_{ef}=-2(\delta_{ce}\delta_{df}-\delta_{cf}\delta_{de}).
$$

In spinor rep it's going to be more complicated.
 

Related to Completeness relation for SO(N)

1. What is the completeness relation for SO(N)?

The completeness relation for SO(N) is a mathematical expression that states that any vector in a vector space can be represented as a linear combination of a set of basis vectors. In the case of SO(N), these basis vectors are the generators of the special orthogonal group of dimension N.

2. How is the completeness relation for SO(N) used in physics?

The completeness relation for SO(N) is used in physics to describe the properties of symmetries and transformations in physical systems. It is often used in quantum mechanics to represent the state of a system and to calculate the probability of various outcomes.

3. Can the completeness relation for SO(N) be generalized to other groups?

Yes, the completeness relation for SO(N) can be generalized to other groups, such as the special unitary group (SU(N)) or the special linear group (SL(N)). These groups also have a set of basis vectors that can be used to represent any vector in the vector space.

4. What is the significance of the completeness relation for SO(N) in mathematics?

The completeness relation for SO(N) is significant in mathematics because it provides a way to decompose a vector into its fundamental components. This allows for simpler calculations and a better understanding of the structure of a vector space.

5. How does the completeness relation for SO(N) relate to the concept of orthogonality?

The completeness relation for SO(N) is closely related to the concept of orthogonality. In SO(N), the basis vectors are orthogonal to each other, meaning they are perpendicular in the vector space. This allows for the representation of any vector as a linear combination of these orthogonal basis vectors.

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