Eigenvalues of an orthogonal matrix

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etotheipi
Homework Statement
Show that the three eigenvalues of a real orthogonal 3x3 matrix are ##e^{i\alpha}##, ##e^{-i\alpha}##, and ##+1## or ##-1##, where ##\alpha \in \mathbb{R}##.
Relevant Equations
N/A
I'm fairly stuck, I can't figure out how to start. I called the matrix ##\mathbf{A}## so then it gives us that ##\mathbf{A}\mathbf{A}^\intercal = \mathbf{I}## from the orthogonal bit. I tried 'determining' both sides... $$(\det(\mathbf{A}))^{2} = 1 \implies \det{\mathbf{A}} = \pm 1$$I don't think this helps me, since I need to show that ##\det{(\mathbf{A} - \lambda \mathbf{I})} = 0## for the values of ##\lambda## in the question and as far as I'm aware there is no rule for ##\det{(\mathbf{a}+\mathbf{b})}##.

I don't know if there is a general form of an orthogonal matrix I can use as a way in (I suspect there isn't, though this might be wrong!). I wondered whether anyone could give me a hint! Thank you.
 
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etotheipi said:
Homework Statement:: Show that the three eigenvalues of a real orthogonal 3x3 matrix are ##e^{i\alpha}##, ##e^{-i\alpha}##, and ##+1## or ##-1##, where ##\alpha \in \mathbb{R}##.
Relevant Equations:: N/A

I'm fairly stuck, I can't figure out how to start. I called the matrix ##\mathbf{A}## so then it gives us that ##\mathbf{A}\mathbf{A}^\intercal = \mathbf{I}## from the orthogonal bit. I tried 'determining' both sides... $$(\det(\mathbf{A}))^{2} = 1 \implies \det{\mathbf{A}} = \pm 1$$I don't think this helps me, since I need to show that ##\det{(\mathbf{A} - \lambda \mathbf{I})} = 0## for the values of ##\lambda## in the question and as far as I'm aware there is no rule for ##\det{(\mathbf{a}+\mathbf{b})}##.

I don't know if there is a general form of an orthogonal matrix I can use as a way in (I suspect there isn't, though this might be wrong!). I wondered whether anyone could give me a hint! Thank you.
Hint: what sort of characteristic equation do you get for a 3x3 matrix?
 
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PeroK said:
Hint: what sort of characteristic equation do you get for a 3x3 matrix?

I get

$$\det \left( \begin{pmatrix}a & b & c\\d & e & f\\g & h & i\\\end{pmatrix} - \begin{pmatrix}\lambda & 0 & 0\\0 & \lambda & 0\\0 & 0 & \lambda\\\end{pmatrix} \right) = 0 $$ $$= (a-\lambda)[(e-\lambda)(i-\lambda) - hf] - b[d(i-\lambda) - gf] + c(dh - g(e-\lambda)) = 0$$

:nb)
 
etotheipi said:
I get

$$\det \left( \begin{pmatrix}a & b & c\\d & e & f\\g & h & i\\\end{pmatrix} - \begin{pmatrix}\lambda & 0 & 0\\0 & \lambda & 0\\0 & 0 & \lambda\\\end{pmatrix} \right) = 0 $$ $$= (a-\lambda)[(e-\lambda)(i-\lambda) - hf] - b[d(i-\lambda) - gf] + c(dh - g(e-\lambda)) = 0$$

:nb)
How would you, in general, describe any such equation?
 
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PeroK said:
How would you, in general, describe any such equation?

I expanded it all out (hope I didn't mess anything up!) and got

##\lambda^{3} -(a+e+i)\lambda^{2} + (ai + ea + ei - hf - bd - gc)\lambda + (aei + gfb + cdh - hfa - bdi - cga) = 0##
The coefficient of ##\lambda^{2}## I can tell to be the trace of ##\mathbf{A}##, the final constant term is I think the determinant, whilst the coefficient of ##\lambda## I can't assign to anything of meaning.
 
etotheipi said:
I expanded it all out (hope I didn't mess anything up!) and got

##\lambda^{3} -(a+e+i)\lambda^{2} + (ai + ea + ei - hf - bd - gc)\lambda + (aei + gfb + cdh - hfa - bdi - cga) = 0##
The coefficient of ##\lambda^{2}## I can tell to be the trace of ##\mathbf{A}##, the final constant term is I think the determinant, whilst the coefficient of ##\lambda## I can't assign to anything of meaning.
It's a cubic equation!
 
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PeroK said:
It's a cubic equation!

Right so then we have 2 complex roots and 1 real root. The coefficients are real so that fixes ##e^{i\alpha}## and ##e^{-i\alpha}## to be two arbitrary solutions, so all that remains is to show that ##\pm 1## is the other solution. And I think we don't need to prove that algebraically, a geometrical argument should do?
 
etotheipi said:
Right so then we have 2 complex roots and 1 real root. The coefficients are real so that fixes ##e^{i\alpha}## and ##e^{-i\alpha}## to be two arbitrary solutions, so all that remains is to show that ##\pm 1## is the other solution. And I think we don't need to prove that algebraically, a geometrical argument should do?
Not quite. It means you have one real root and a pair of conjugate roots.

Do you know the properties of an orthogonal matrix? There's a key (alternative defining) property.
 
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PeroK said:
Not quite. It means you have one real root and a pair of conjugate roots.

Do you know the properties of an orthogonal matrix? There's a key (alternative defining) property.

Yeah, I just realized I forgot about the modulus, so at the moment we're stuck with a real solution an two complex ones of the form ##\beta e^{i \alpha}## and ##\beta e^{-i \alpha}##.

I went onto Wikipedia and found that for a vector ##\vec{v}## and its transpose ##\vec{v}^\intercal##, if ##Q## is orthogonal then

##\vec{v}^\intercal \vec{v} = \vec{v}^\intercal Q^\intercal Q \vec{v}##

I'll play around with that for a little bit and see if I can get anything useful, assuming that's the one you were making reference to!
 
etotheipi said:
Yeah, I just realized I forgot about the modulus, so at the moment we're stuck with a real solution an two complex ones of the form ##\beta e^{i \alpha}##.

I went onto Wikipedia and found that for a vector ##\vec{v}## and its transpose ##\vec{v}^\intercal##, if ##Q## is orthogonal then

##\vec{v}^\intercal \vec{v} = \vec{v}^\intercal Q^\intercal Q \vec{v}##

I'll play around with that for a little bit and see if I can get anything useful, assuming that's the one you were making reference to!
Yes, although I would think of that it terms of the inner product (and the the norm).
 
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PeroK said:
Yes, although I would think of that it terms of the inner product (and the the norm).

Yeah that makes more sense, because then ##||A\vec{v}||^{2} = ||\vec{v}||^{2}## since the ##A## and its transpose do some cancelling if ##A## is orthogonal.

In that case, can't we just say the square of the norm is going to just be ##\lambda^{2} ||\vec{v}||^{2}##, which is just ##\lambda^{2}## times itself so the modulus of lambda has to be 1, and this gives us all of our results?
 
etotheipi said:
Yeah that makes more sense, because then ##||A\vec{v}||^{2} = ||\vec{v}||^{2}## since the ##A## and its transpose do some cancelling if ##A## is orthogonal.

In that case, can't we just say the square of the norm is going to just be ##\lambda^{2} ||\vec{v}||^{2}##, which is just ##\lambda^{2}## times itself so the modulus of lambda has to be 1, and this gives us all of our results?
Yes need to be careful because ##\lambda## may be complex. The simplest approach is to consider ##A## as a unitary matrix with real coefficients.
 
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PeroK said:
Yes need to be careful because ##\lambda## may be complex. The simplest approach is to consider ##A## as a unitary matrix with real coefficients.

Yes, completely forgot about that part! I should really write ##||\vec{v}||^2 = ||A \vec{v}||^2 = ||\lambda \vec{v}||^2 = \lambda \lambda^* ||\vec{v}||^2 = |\lambda|^2 ||\vec{v}||^2##. Thanks for the help!
 
vela said:
How did you conclude that two of the roots are complex? A cubic could have three real roots.

I suppose you're right, I just assumed from how the question was phrased that there were only two possibilities for real roots (##1## and ##-1##), and this indeed turned out to be the case since there are only two re`als with modulus 1.

But the point stands, I should have been more careful at that stage :wink:.
 
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etotheipi said:
I suppose you're right, I just assumed from how the question was phrased that there were only two possibilities for real roots (##1## and ##-1##), and this indeed turned out to be the case since there are only two re`als with modulus 1.

But the point stands, I should have been more careful at that stage :wink:.
There are the degenerate cases where ##\lambda = \pm 1## only. Although these do meet the criteria in each case.
 
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PeroK said:
There are the degenerate cases where ##\lambda = \pm 1## only.

Oh, do you mean if we got something like ##\alpha = \pi## or ##\alpha = 0## so that we would indeed have three real roots, which might be ##(\lambda_1, \lambda_2, \lambda_3) = (1,1,1), (1,1,-1), (1,-1,-1), (-1,-1,-1)##. Hadn't thought of that either!
 
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etotheipi said:
Oh, do you mean if we got something like ##\alpha = \pi## or ##\alpha = 0## so that we would indeed have three real roots, which might be ##(\lambda_1, \lambda_2, \lambda_3) = (1,1,1), (1,1,-1), (1,-1,-1), (-1,-1,-1)##. Hadn't thought of that either!
I didn't think of the degenerate cases, but yes you can make it work like that for those as well.
 
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PeroK said:
There are the degenerate cases where ##\lambda = \pm 1## only. Although these do meet the criteria in each case.
These occur iff the real orthogonal matrix is symmetric. I don't really view involutions as "degenerate" though. In fact involutions are quite nice.