How can I write a normalized spin superposition in a simplified form?

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The discussion focuses on simplifying a normalized spin superposition |ψ> = (a1+a2i) |1> + (b1+b2i) |2> into the form |ψ> = cosθ|1> + eiΦsinθ|2>. Participants emphasize the importance of factoring out the common phase factor to make the coefficient of |1> real. It is established that while one can adjust the global phase of the superposition, the two expressions cannot be directly equated. A recommended method involves multiplying by the conjugate of the coefficient of |1>, specifically (a1 - a2i), to eliminate the complex component.

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If I have an normalized spin superposition |ψ> = (a1+a2i) |1> + (b1+b2i) |2>, and asked to write it in the form |ψ> = cosθ|1> + esinθ|2>, how do I proceed?
My main problem is that no matter what I try, I can't seem to get rid of some complex component that shows up in the coefficient of |1>. I can try to get rid of that after taking the common phase factor from both the vecotrs but after I take it out, am I allowed to just ignore it?
 
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Ananthan9470 said:
I can try to get rid of that after taking the common phase factor from both the vecotrs but after I take it out, am I allowed to just ignore it?
If the question does not say anything about that, I would factor out the common phase factor to make the coefficient of ##|1\rangle## real. No matter what you try, the two expressions given in the question cannot be equated.
 
You're probably allowed to adjust the superposition's global phase (since the global phase is an unobservable artifact of the representation).

Try multiplying by the expression by the conjugate of $| 1 \rangle$'s coefficient, i.e. by $a_1 - a_2 i$. That's how you normally cancel out the phase of a complex coefficient. Then it's just a matter of renormalizing the length.
 

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