MHB Eigenvectors of 2*2 rotation matrix

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SUMMARY

The eigenvalues of the 2x2 rotation matrix \(\begin{bmatrix}\cos \theta & \sin \theta \\ -\sin \theta & \cos \theta\end{bmatrix}\) are \(\lambda_1 = e^{i \theta}\) and \(\lambda_2 = e^{-i \theta}\). The corresponding eigenvectors are \(\begin{bmatrix}1 \\ i\end{bmatrix}\) for \(\lambda_1\) and \(\begin{bmatrix}1 \\ -i\end{bmatrix}\) for \(\lambda_2\). The inner product of these eigenvectors is calculated incorrectly without considering the complex conjugate, leading to confusion regarding their orthogonality. When \(\theta = 0\), the matrix simplifies to the identity matrix, resulting in a repeated eigenvalue of 1.

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bugatti79
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Hi Folks,

I calculate the eigenvalues of \begin{bmatrix}\cos \theta& \sin \theta \\ - \sin \theta & \cos \theta \end{bmatrix} to be \lambda_1=e^{i \theta} and \lambda_2=e^{-i \theta}

for \lambda_1=e^{i \theta}=\cos \theta + i \sin \theta I calculate the eigenvector via A \lambda = \lambda V as

\begin{bmatrix}\cos -(\cos \theta+ i \sin \theta) & \sin \theta \\ - \sin \theta & \cos -(\cos \theta+ i \sin \theta)\end{bmatrix} \begin{bmatrix}v_1\\ v_2\end{bmatrix}=\vec{0}

which reduces to

- i \sin \theta v_1+ \sin \theta v_2=0
-\sin \theta v_1-i \sin \theta v_2=0

I am stumped at this point...how shall I proceed?
 
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bugatti79 said:
Hi Folks,

I calculate the eigenvalues of \begin{bmatrix}\cos \theta& \sin \theta \\ - \sin \theta & \cos \theta \end{bmatrix} to be \lambda_1=e^{i \theta} and \lambda_2=e^{-i \theta}

for \lambda_1=e^{i \theta}=\cos \theta + i \sin \theta I calculate the eigenvector via A \lambda = \lambda V as

\begin{bmatrix}\cos -(\cos \theta+ i \sin \theta) & \sin \theta \\ - \sin \theta & \cos -(\cos \theta+ i \sin \theta)\end{bmatrix} \begin{bmatrix}v_1\\ v_2\end{bmatrix}=\vec{0}

which reduces to

- i \sin \theta v_1+ \sin \theta v_2=0
-\sin \theta v_1-i \sin \theta v_2=0

I am stumped at this point...how shall I proceed?
Divide those equations by $\sin\theta$ (assuming that $\sin\theta\ne0$).
 
Opalg said:
Divide those equations by $\sin\theta$ (assuming that $\sin\theta\ne0$).

Then we get

- i v_1+ v_2=0 (1)
- v_1-i v_2=0 (2)

v_2=i v_1 from 1

v_2=-v_1/i from 2

1) These contradict? How is the eigenvector obtained from this?

2) what if we have a situation where \theta=0? Then \sin \theta=0
 
bugatti79 said:
Then we get

- i v_1+ v_2=0 (1)
- v_1-i v_2=0 (2)

v_2=i v_1 from 1

v_2=-v_1/i from 2

1) These contradict? How is the eigenvector obtained from this?

2) what if we have a situation where \theta=0? Then \sin \theta=0
1) They don't contradict, because $i^2=-1$ and so $-1/i = i$.

2) If $\theta=0$ then the matrix becomes $\begin{bmatrix}1&0 \\0&1 \end{bmatrix}$ (the identity matrix), with a repeated eigenvalue $1$.
 
Opalg said:
1) They don't contradict, because $i^2=-1$ and so $-1/i = i$.

2) If $\theta=0$ then the matrix becomes $\begin{bmatrix}1&0 \\0&1 \end{bmatrix}$ (the identity matrix), with a repeated eigenvalue $1$.

1) Ok, so the eigenvector for

\lambda_1=e^{i \theta} is \begin{bmatrix}1\\ i\end{bmatrix}

and

\lambda_2=e^{-i \theta} is \begin{bmatrix}1\\ 1/i\end{bmatrix}

To show these 2 vectors are orthogonal I get the inner product

<v_1,v_2>=(1*1)+(i*1/i)\ne 0 but I expect 0...?
 
bugatti79 said:
1) Ok, so the eigenvector for

\lambda_1=e^{i \theta} is \begin{bmatrix}1\\ i\end{bmatrix}

and

\lambda_2=e^{-i \theta} is \begin{bmatrix}1\\ 1/i\end{bmatrix}

To show these 2 vectors are orthogonal I get the inner product

<v_1,v_2>=(1*1)+(i*1/i)\ne 0 but I expect 0...?
The definition of the inner product of two complex vectors is that you have to take the complex conjugate of the second one: if $x = ( x_1,x_2)$ and $y = (y_1,y_2)$ then $\langle x,y\rangle = x_1\overline{y_1} + x_2\overline{y_2}.$
 
I am studying the mathematical formalism behind non-commutative geometry approach to quantum gravity. I was reading about Hopf algebras and their Drinfeld twist with a specific example of the Moyal-Weyl twist defined as F=exp(-iλ/2θ^(μν)∂_μ⊗∂_ν) where λ is a constant parametar and θ antisymmetric constant tensor. {∂_μ} is the basis of the tangent vector space over the underlying spacetime Now, from my understanding the enveloping algebra which appears in the definition of the Hopf algebra...

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