Neutrino Oscillation Survival Probability

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Homework Help Overview

The discussion revolves around deriving the survival probability of a neutrino species during oscillation, specifically aiming to express it in a particular mathematical form involving sine and cosine functions. The subject area includes concepts from quantum mechanics and particle physics, particularly related to neutrino behavior.

Discussion Character

  • Exploratory, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss various steps in the derivation process, questioning the correctness of specific terms and suggesting alternative forms. There is an emphasis on maintaining a learning-oriented dialogue, with one participant expressing a desire for hints rather than direct answers.

Discussion Status

The discussion is ongoing, with participants actively engaging in mathematical reasoning and exploring different interpretations of the expressions involved. Some guidance has been offered, particularly regarding the simplification of terms, but no consensus has been reached on the final form of the probability expression.

Contextual Notes

Participants are working within the constraints of homework rules, aiming to derive results independently while seeking clarification on specific steps in their calculations.

Dahaka14
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Homework Statement


I'm lost at how to derive the probability of a neutrino species surviving an oscillation. After performing calculations, I can't seem to get it into the nice tidy form
1-\sin^{2}2\theta\sin^{2}\left(\frac{\Delta m^{2}t}{4p}\right)

Homework Equations


Whatev...
|\langle\nu_{e}|\psi(t)\rangle|^{2}
E_{i}=\sqrt{p^{2}+m_{i}^{2}}\approx p+\frac{m_{i}^{2}}{2p},~\text{where}~p\gg m
\text{and}~\Delta m^{2}=m_{2}^{2}-m_{1}^{2}

The Attempt at a Solution


\begin{align*}<br /> P_{e\rightarrow\nu_{e}}=\langle\nu_{e}|\psi(t)\rangle&amp;=\langle\nu_{e}|\nu_{e}\rangle e^{-iEt/\hbar}=\left|<br /> \left(<br /> \begin{array}{ccc}<br /> \cos\theta &amp; \sin\theta<br /> \end{array} \right)<br /> \left(<br /> \begin{array}{ccc}<br /> \cos\theta e^{-iE_{1}t/\hbar} \\<br /> \sin\theta e^{-iE_{2}t/\hbar}<br /> \end{array} \right)<br /> \right|^{2} \\<br /> &amp;=|\cos^{2}\theta e^{-iE_{1}t/\hbar}+\sin^{2}\theta e^{-iE_{2}t/\hbar}|^{2} \\<br /> &amp;=|e^{-iE_{1}t/\hbar}(\cos^{2}\theta+\sin^{2}\theta e^{-(iE_{2}-E_{1})t/\hbar})|^{2} \\<br /> &amp;=(\cos^{2}\theta+\sin^{2}\theta e^{-i(E_{2}-E_{1})t/\hbar})(\cos^{2}\theta+\sin^{2}\theta e^{i(E_{2}-E_{1})t/\hbar}) \\<br /> &amp;=\frac{1}{2}\sin^{2}2\theta\left(\cos\frac{\Delta m^{2}t}{2p}-i\sin\frac{\Delta m^{2}t}{2p}+\cos\frac{\Delta m^{2}t}{2p}+i\sin\frac{\Delta m^{2}t}{2p}\right)+\cos^{4}\theta+\sin^{4}\theta \\<br /> &amp;=\sin^{2}2\theta\cos\frac{\Delta m^{2}t}{2p}+\cos^{4}\theta+\sin^{4}\theta \\<br /> &amp;=...? \\<br /> &amp;=1-\sin^{2}2\theta\sin^{2}\left(\frac{\Delta m^{2}t}{4p}\right)<br /> \end{align*}
Can someone help me fill in the blank? It would be best if I could do it on my own, so if possible just give me hints. If it is too explicit, then just tell me I guess. But as we all know, in order for me to truly own the idea, I should only be gently pushed toward the answer :smile:.
 
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Dahaka14 said:
<br /> &amp;=\frac{1}{2}\sin^{2}2\theta\left(\cos\frac{\Delta m^{2}t}{2p}-i\sin\frac{\Delta m^{2}t}{2p}+\cos\frac{\Delta m^{2}t}{2p}+i\sin\frac{\Delta m^{2}t}{2p}\right)+\cos^{4}\theta+\sin^{4}\theta<br />

Shouldn't

\frac{1}{2}\sin^{2}2\theta

be

\left( \frac{1}{2}\sin2\theta \right)^2 ?

Then, I think it works.
 
Okay, so now I have
\begin{align*}<br /> &amp;=\frac{1}{2}\sin^{2}2\theta\cos\frac{\Delta m^{2}t}{2p}+\cos^{4}\theta+\sin^{4}\theta \\<br /> &amp;=\frac{2\sin^{2}2\theta\cos\frac{\Delta m^{2}t}{2p}}{4}+\frac{3+\cos4\theta}{4}<br /> \end{align*}

I'm sorry if it might be obvious, but I can't see it. I've just looked at it for too long.
 
There could be more than one way to show this. Here's one way: what does \left( \cos^2 \theta + \sin^2 \theta \right)^2 equal?
 
Thanks a lot!
 

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