Neutrino oscillation with very low energy neutrinos

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Discussion Overview

The discussion revolves around the behavior of neutrinos, particularly focusing on neutrino oscillation at very low energies and the implications of non-relativistic motion. Participants explore theoretical aspects of neutrino mass eigenstates, their velocities, and the effects on detection and mixing.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • One participant suggests that if neutrinos have different masses, non-relativistic oscillation would imply a substantial change in velocity to conserve momentum, raising questions about spontaneous speed changes.
  • Another participant argues that non-relativistic motion leads to decoherence of mass eigenstates, resulting in the detection of the lightest mass eigenstate first, without speed changes.
  • A hypothetical scenario is presented regarding a beta decay atom moving near the speed of light, questioning whether a detected muon neutrino would correspond to its mass rather than the speed of an electron neutrino.
  • Discussion includes the clarification that flight times pertain only to mass eigenstates, and that neutrino mixing complicates the association of mass and flavor eigenstates.
  • One participant emphasizes the need to consider neutrinos as distinct mass eigenstates with specific coupling strengths, and that identifying a mass eigenstate during flight breaks interference, akin to the double-slit experiment.
  • Another participant questions the implications of different velocities for mass eigenstates over long distances, suggesting this might hinder neutrino mixing.
  • A response clarifies that while mass eigenstates may separate, mixing remains a fundamental property, though coherence is lost, affecting oscillatory behavior.

Areas of Agreement / Disagreement

Participants express differing views on the implications of non-relativistic neutrino oscillation, the behavior of mass eigenstates, and the nature of neutrino mixing. The discussion remains unresolved regarding the consequences of these factors on detection and oscillation.

Contextual Notes

Participants note limitations in understanding related to the definitions of mass and flavor eigenstates, as well as the conditions under which neutrino mixing occurs. There are unresolved questions about the effects of distance on coherence and oscillatory behavior.

Who May Find This Useful

This discussion may be of interest to those studying neutrino physics, particle physics, or electroweak theory, particularly in relation to the behavior of neutrinos in various energy regimes.

PAllen
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This question just occurred to me recently. Assuming the different neutrinos (electron, muon, tau) do not have the same mass, then if their energy is very low, such that they are moving non-relativistically, an oscillation must substantially change the velocity (to conserve momentum). It seems this must be the case, because any neutrino ascillation could be viewed in a frame where neutrinos are slow moving. Yet this is certainly an odd mental image - spontaneous speed change.

Just checking that this is expected?
 
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If they are moving non-relativistically, the three mass eigenstates quickly get decoherent, and you don't see oscillation any more. You'll either detect the lightest mass eigenstate arriving first, or the middle mass eigenstate arriving a bit later, or the heaviest eigenstate arriving even later. No speed change.
Note: every plausible detection mechanism sees flavor eigenstates - but you can calculate the probability to see them for each mass eigenstate separately.
 
So, hypothetically, if an atom undergoing beta decay is moving near c away from me, and also is very far away, and its neutrino happens to be heading toward me at extremely low energy, I might detect a muon neutrino at a time consistent with its always having that mass, rather than a time corresponding to part of the flight at electron neutrino speed?
 
Flight times exist for the mass eigenstates only. There is no "speed of an electron neutrino", just a "speeds of the three mass eigenstates". Neutrino mixing is strong, you cannot even make an approximate association of mass and flavor eigenstates like you can do for quarks.
 
PAllen said:
might detect a muon neutrino at a time consistent with its always having that mass

That object doesn't exist.

The way to think of it that minimizes conceptual misunderstandings is that there are three neutrinos, nu1, nu2 and nu3. They have definite masses. Nu3 has about half the coupling strength to muons and taus that it would if it only coupled to one, and a tiny coupling to electrons. Nu2 has equal couplings, again, one-third the maximum, and nu1 has about three-quarters of the maximum coupling to electrons, and 10% of the maximum to the other two. Those are the particles in the theory, not nu_e, nu_mu and nu_tau.

If I set up an experiment where I produce neutrinos of a given flavor and detect neutrinos of a given flavor, I do not know if the neutrino in flight is a nu1, nu2 or nu3, so I need to add amplitudes, not intensities, so I get interference - which we call oscillations. (This is not the greatest terminology.) Asking what mass eigenstate was in flight is exactly equivalent to asking "which slit did the electron go through"?

If I have some other measurement, like timing, it tells me which mass eigenstate it was, and that breaks the interference, just as identifying which slit breaks the interference. You will know you had a nu2 and that you always had a nu2. A nu2 was emitted and a nu2 was detected.
 
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Thank to both of you. That is very clear now.
 
mfb please

If the three neutrino mass eigenstates have different velocities, then, as they propagate over the lightyears, won’t the mass eigenstates draw away from each other. Wouldn’t that make the neutrino mixing impossible. Obviously, I’m missing something. I only got as far as Merzbacher.
 
MRBlizzard said:
If the three neutrino mass eigenstates have different velocities, then, as they propagate over the lightyears, won’t the mass eigenstates draw away from each other
Yes. Heuristically, the wave packets of the different mass eigenstates will separate. You do not need to go to lightyear distances (depending on neutrino energy). This occurs for solar neutrinos that reach the Earth.

MRBlizzard said:
Wouldn’t that make the neutrino mixing impossible.
No. Mixing is not something that happens because the state wave packets overlap, it is a fundamental property - the mismatch in weak interactions between the mass eigenstates of neutrinos and those of charged leptons.

However, as the states separate you lose coherence between them and therefore the oscillatory behaviour disappears. The flavor transition probabilities then become constant in distance - where the constants are given by the mixing matrix.
 
Thank you.
Could you point me towards a reading list towards Electroweak Theory.
 

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