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I found an interesting case where it seems like an equality sign works wrong.

Let's consider the following construction:

$\frac{1+\Lambda}{2} e^{i\Lambda \phi}$ where $\Lambda = \pm1$, so $\Lambda^2=1$.

Then I apply Euler formula:

$\frac{1+\Lambda}{2} e^{i\Lambda \phi} = \frac{1+\Lambda}{2} (\cos \phi + i\Lambda \sin \phi)= \frac{1}{2} \cos \phi + \frac{\Lambda}{2} \cos \phi + \frac{i\Lambda}{2} \sin \phi + \frac{i}{2} \sin \phi = \frac{1+\Lambda}{2} e^{i\phi}$

where I have used $\sin(\Lambda \phi) = \Lambda \sin \phi$ and $\cos (\Lambda \phi) = \cos \phi$.

However, this is just wrong! $e^{i\Lambda \phi}\neq e^{i \phi}$ even though the equality sign was not broken anywhere in between (at least it doesn't seem to be broken to me). What am I doing wrong?

MsTais
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    How'd you get $\cos \phi + i\Lambda\sin \phi = e^{i\phi}$? – Brian Tung Oct 19 '16 at 17:10
  • Your are forgetting the $\Lambda$ in the second term, hence the LHS does not contain $e^{i\phi}$ – b00n heT Oct 19 '16 at 17:11
  • @b00n heT I hope it is more obvious now. – MsTais Oct 19 '16 at 17:13
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    @BrianTung : Don't forget that $\Lambda$ is only $\pm 1$ – MPW Oct 19 '16 at 17:15
  • $\frac{1+\Lambda}{2}$ is a projection operator into the subspace where $\Lambda = 1$. On that subspace, $e^{i\Lambda\phi}$ is $e^{i\phi}$ times the identity. – achille hui Oct 19 '16 at 17:17
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    There are three $\cos$ and a single $\sin$ in your expansion. Fix that. –  Oct 19 '16 at 17:17
  • @achille hui so should I treat $e^{i\Lambda \phi}$ as a vector then? What is the correct machinery for this problem? – MsTais Oct 19 '16 at 17:25
  • The complex exponential is just cosmetic, your identity reduces to $(1+\Lambda)(a+\Lambda b)=(1+\Lambda)(a+b)$, which was explained by @Lucas. –  Oct 19 '16 at 17:27
  • @MPW: I didn't; OP's expansion still does not make this clear (even with the $\cos$ fixed to $\sin$). – Brian Tung Oct 19 '16 at 17:32

3 Answers3

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The problem is the division by zero:

The identity $\tfrac{1+\Lambda}{2}e^{i\Lambda\phi}=\tfrac{1+\Lambda}{2}e^{i\phi}$ holds as you have shown.

For $\Lambda=1$, this implies $e^{i\Lambda\phi}=e^{i\phi}$, which is obviously correct. However, for $\Lambda=-1$, this means that $\tfrac{1+\Lambda}{2}=0$ and therefore, the last implication $\tfrac{1+\Lambda}{2}e^{i\Lambda\phi}=\tfrac{1+\Lambda}{2}e^{i\phi}\implies e^{i\Lambda\phi}=e^{i\phi}$ is not correct in this case.

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Your third term should be $\frac{i\Lambda}{2}\sin \phi$, not $\frac{i\Lambda}{2}\cos\phi$.

MPW
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You are correct that $e^{i\Lambda \phi}\neq e^{i \phi}$.

But your computation doesn't show that $e^{i\Lambda \phi}= e^{i \phi}$; it shows that $\frac{1+\Lambda}{2}e^{i\Lambda \phi}= \frac{1+\Lambda}{2}e^{i \phi}$, which is true for $\Lambda=\pm 1$.

TonyK
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  • But usually I can just cancel $\frac{1+\Lambda}{2}$ on both sides, which I obviously can't do here. It seems like an analogue of circular equation, which makes me think that I have to use a vector description here, rather than treating it as a double-valued function... – MsTais Oct 20 '16 at 16:46
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    @MsTais: As Lukas has pointed out, you can only cancel a non-zero multiplier on both sides. I really don't see your problem. – TonyK Oct 20 '16 at 16:54