Question about neutrino oscillations

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    Neutrino Oscillations
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Discussion Overview

The discussion centers on neutrino oscillations, specifically the relationship between mass eigenstates and flavor eigenstates, as well as the assumptions regarding momentum in neutrino beams. Participants explore theoretical implications and practical considerations in the context of neutrino physics.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants propose that the fundamental nature of neutrinos depends on the context: mass eigenstates may be seen as actual physical states, while flavor states may represent a more symmetric description of the theory.
  • There is a question about the validity of assuming that all mass eigenstates in a neutrino beam have the same momentum, with some participants suggesting that this assumption is acceptable due to the small mass of neutrinos compared to their energy in oscillation scenarios.
  • One participant notes that if neutrino masses were comparable to other particle masses, the approximation of equal momentum would not hold, implying that observable effects would have been detected through means other than oscillations.
  • A later reply seeks to quantify the distance over which solar neutrinos may oscillate into different flavors, referencing oscillation distances in modern experiments.

Areas of Agreement / Disagreement

Participants express differing views on the fundamental nature of mass and flavor eigenstates, and the discussion remains unresolved regarding the implications of momentum assumptions in neutrino oscillations.

Contextual Notes

Limitations include assumptions about the relationship between mass and momentum in neutrino beams and the lack of consensus on the implications of these assumptions for neutrino oscillations.

McLaren Rulez
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Hi.

I'm a college undergrad (junior year, so basic knowledge of QM but not much else) and I'm reading up on neutrino oscillations. I have a few questions.

For neutrinos, which is more fundamental: The mass eigenstates or the flavour eigenstates? In this paper http://www2.warwick.ac.uk/fac/sci/physics/teach/module_home/px435/bkayser.pdf the author says, "Suppose that there are N physical neutrinos (mass eigenstates), \nu_{m}..." So do the mass eigenstates represent physical particles which come together in different linear combinations to produce flavour? I am a bit confused about this issue.

Also, in the same paper, the author mentions in the first page, on the right side column: In the standard treatment it is supposed that we have a beam of neutrinos all having a common fixed momentum, p_{\mu}. So when he talks about momentum, is he saying that all the different mass eigenstates have the same momentum? If so, why is it valid to assume that they all have a fixed common momentum? Why can't different mass eigenstates have different momenta?

Thank you very much for your help.
 
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I'm afraid you may not like this answer; but, which set of states are more fundamental depends on what you mean by "fundamental." If you're asking about which set of state are more reasonable to think of as the "actual physical states," the best answer is the mass eigenstates; but, if you're asking which should show up in the simplest (or, pretty much equivalently, most symmetric) description of the theory, the answer is the flavor states.
 
Thank you for the reply, Parlyne.

Regarding the second part, do you know why it is ok to think of a beam of mass eigenstates all having the same momentum as the standard treatment for neutrino oscillations? I also see some other sources where they treat the energy of all the eigenstates as equal instead. Why are we allowed to do this?

Thank you.
 
McLaren Rulez said:
why it is ok to think of a beam of mass eigenstates all having the same momentum as the standard treatment for neutrino oscillations?

The neutrino masses are assumed to be much smaller (on the order of 1 eV/c^2) than the neutrino energies in oscillation situations: on the order of 1 MeV for solar neutrinos, and ranging up to the GeV range for accelerator experiments. In these sitations the energy equals the momentum, for all practical purposes, and changing the mass has practically no effect on the momentum, for a given energy.

If the neutrino masses were comparable to other particle masses, then this approximation wouldn't work; but in that case we would have observed the effects of neutrino mass a long time ago in other ways than neutrino oscillations!
 
jtbell said:
The neutrino masses are assumed to be much smaller (on the order of 1 eV/c^2) than the neutrino energies in oscillation situations: on the order of 1 MeV for solar neutrinos, and ranging up to the GeV range for accelerator experiments. In these sitations the energy equals the momentum, for all practical purposes, and changing the mass has practically no effect on the momentum, for a given energy.

If the neutrino masses were comparable to other particle masses, then this approximation wouldn't work; but in that case we would have observed the effects of neutrino mass a long time ago in other ways than neutrino oscillations!

So at what distance from the center of the sun can we expect the solar neutrinos to change into a different neutrino, if that makes sense? Or in other words, how many oscillations from the sun to the Earth?
 
Spinnor said:
So at what distance from the center of the sun can we expect the solar neutrinos to change into a different neutrino, if that makes sense? Or in other words, how many oscillations from the sun to the Earth?

From:

http://en.wikipedia.org/wiki/Neutrino_oscillation


"Oscillation distances, L, in modern experiments are on the order of kilometers"
 

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