Understanding the PMNS matrix?

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SUMMARY

The PMNS (Pontecorvo-Maki-Nakagawa-Sakata) matrix governs neutrino oscillation and is commonly represented by a specific parameterization involving rotation matrices and complex phases. The matrix includes terms such as e^{i\delta} related to CP violation and e^{i\alpha} associated with the Majorana nature of neutrinos. Despite its significance in particle physics, there is a notable lack of comprehensive derivations and explanations in existing literature, leading to confusion among researchers. This gap highlights the need for more detailed resources on the derivation and implications of the PMNS matrix components.

PREREQUISITES
  • Understanding of neutrino oscillation theory
  • Familiarity with complex numbers and exponential functions
  • Knowledge of rotation matrices in three-dimensional space
  • Basic concepts of CP violation and Majorana particles
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  • Study the derivation of the PMNS matrix from first principles in particle physics
  • Explore the implications of CP violation in neutrino physics
  • Research the role of Majorana neutrinos and their impact on the PMNS matrix
  • Examine the relationship between the PMNS matrix and the CKM (Cabibbo-Kobayashi-Maskawa) matrix
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Particle physicists, researchers in neutrino physics, and students seeking a deeper understanding of the PMNS matrix and its implications in experimental physics.

Doofy
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I have been trying to find out about the MNS / PMNS matrix that governs neutrino oscillation:

\left( \begin{array}{c} \nu_{e} \\ \nu_{\mu} \\ \nu_{\tau} \end{array} \right) = \left( \begin{array}{ccc} U_{e1} & U_{e2} & U_{e3} \\ U_{\mu 1} & U_{\mu 2} & U_{\mu 3} \\ U_{\tau 1} & U_{\tau 2} & U_{\tau 3} \end{array} \right) \left( \begin{array}{c} \nu_{1} \\ \nu_{2} \\ \nu_{3} \end{array} \right)

I am aware that there is more than one parameterization exists, but the most common one seems to be the one stated on wikipedia:

\left( \begin{array}{ccc} c_{12}c_{13} & s_{12}c_{13} & s_{13}e^{-i\delta} \\ -s_{12}c_{23} -c_{12}s_{23}s_{13}e^{-i\delta} & c_{12}c_{23}-s_{12}s_{23}s_{13}e^{-i\delta} & s_{23}c_{13} \\ s_{12}s_{23} -c_{12}c_{23}s_{13}e^{-i\delta} & -c_{12}s_{23} - s_{12}c_{23}s_{13}e^{-i\delta} & c_{23}c_{13} \end{array} \right) \left( \begin{array}{ccc} e^{i\alpha_{1}/2} & 0 & 0 \\ 0 & e^{i\alpha_{2}/2} & 0 \\ 0 & 0 & 1 \end{array} \right)

My problem is that every paper, every website, every textbook I have consulted all just seem to state that this is what the matrix looks like, but offer no derivation / explanation of where it comes from. I feel uncomfortable just blindly accepting this.

The s_{ij}, c_{ij} parts I am fine with, they are just abbreviations for sin\theta_{ij}, cos\theta_{ij} and come from having multiplied together rotation matrices for rotations around 3 axes. Nothing unusual there.

My issue is with the e^{i\delta} and e^{i\alpha} parts. I am aware that the e^{i\delta} part has something to do with allowing for possible CP violation, but I need to understand how it got there as it means very little to me at this moment.
I know even less about the e^{i\alpha} parts - something to do with the possible Majorana-ness of neutrinos?

I'm so surprised by how little information there is out there on this little topic, especially given the amount of money being spent on experiments to measure these matrix elements. What's going on here?
 
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