Problem with neutrino oscillations

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    Neutrino Oscillations
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Discussion Overview

The discussion revolves around the concept of neutrino oscillations, specifically addressing the relationship between mass eigenstates and flavor eigenstates. Participants explore the theoretical implications of these states and their independence in different Hilbert spaces, as well as the mechanisms that might lead to oscillations. The conversation includes technical reasoning and conceptual clarifications regarding quantum states and their interactions.

Discussion Character

  • Exploratory, Technical explanation, Conceptual clarification, Debate/contested

Main Points Raised

  • One participant expresses confusion about how neutrino oscillations arise from the independence of mass and flavor eigenstates in different Hilbert spaces.
  • Another participant questions the clarity of the original query, asking whether the confusion lies in the difference between mass and flavor eigenstates or in the mechanism of oscillations themselves.
  • A participant elaborates on the lack of interaction between different Hilbert spaces unless specific conditions, such as Hamiltonian cross terms or symmetry requirements, are met, suggesting that neutrino oscillations do not fit these criteria.
  • Another participant asserts that the eigenstates are indeed different and questions the validity of deriving physical phenomena based solely on their differences.
  • One participant notes that the derivation of the neutrino oscillation formula focuses exclusively on flavor space, drawing an analogy to spin precession in magnetic fields.
  • A different perspective suggests that neutrino oscillations might be better understood as interference rather than oscillations, linking to an external resource for further reading.
  • Another participant argues against the assumption that the spatial wave function is relevant to oscillations, clarifying that the distance in the oscillation formula serves as a proxy for time for ultrarelativistic neutrinos, and discusses the relationship between mass and flavor eigenstates.

Areas of Agreement / Disagreement

Participants express differing views on the relationship between mass and flavor eigenstates and their implications for neutrino oscillations. There is no consensus on the clarity of the original question or the mechanisms behind oscillations, indicating ongoing debate and exploration of the topic.

Contextual Notes

Some participants highlight limitations in understanding the independence of Hilbert spaces and the conditions under which different quantum states may interact. The discussion reflects a range of interpretations regarding the nature of neutrino oscillations and the role of spatial wave functions.

ShayanJ
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The phenomena of neutrino oscillations (as I understand it) is based on the idea that neutrino mass eigenstates are not the same as the flavor eigenstates and being in a definite mass eigenstate means the paticle has no definite flavor and vice versa. But this doesn't make sense to me, because the quantum state of a particle is the combination of its state in several Hilbert spaces, the Hilbert space of complex functions over spatial coordinates, the flavor Hilbert space, etc. As long as the interactions in the Hamiltonian don't couple flavor with spatial coordinates, these Hilbert spaces are completely independent and have nothing to do with each other. So I don't understand this effect that arises from the supposed inter-dependency of these two independent Hilbert spaces. Can anyone make things clear?
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It is unclear to me which part is unclear to you. Are you saying that you do not understand how the mass eigenstates can be different from the flavour eigenstates (this is also the case in the quark sector) or are you saying that you do not understand how it can give rise to neutrino oscillations?
 
I don't understand how this can give rise to neutrino oscillations. Because the only ways I know that different parts of a quantum state(I mean parts in different Hilbert spaces) can affect each other, is either with the mixing of these parts through a Hamiltonian that has a cross term between these Hilbert spaces or something like having a state that has to be either completely symmetric or completely anti-symmetric w.r.t. particle exchange that is the product of a spin state and a spatial state. Then the symmetry properties of one of these parts determines the symmetry properties of the other. But it doesn't seem to me that neutrino oscillations is of any of the above types.
 
Also, of course those eigenstates are different! They're two sets of vectors in two different Hilbert spaces. It doesn't even make sense to ask the question whether they're different or not, let alone concluding a specific physical phenomenon on the basis of them being different!
 
The typical way of deriving the neutrino oscillation formula does not bother at all with the spatial part of the wave function. It only deals with flavour space. It is completely analogous to spin precession where you are interested in the z-component of the spin of a spin-1/2 particle in an external magnetic field in the x-direction. The interaction basis in that case is the z-basis and the evolution basis is the x-basis.
 
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@ShayanJ I think you are deceiving yourself in some way from the ##L## dependence that the spatial wave function has anything to do with the oscillations (you can study the effects of spatial wave packets rather than plane waves, but in essence that just leads to decoherence and it is not really relevant to what you are looking at). The ##L## in the standard oscillation formula is a proxy for time as ##L \simeq t## (in units of ##c = 1##) for ultrarelativistic neutrinos and does not a priori have anything to do with the spatial wave function. The mass eigenstates and flavour eigenstates span the same Hilbert space* and are related by a unitary rotation. The mass eigenstates are the propagation eigenstates that acquire a definite phase from the time evolution and the flavour eigenstates are the ones that produce a particular charged lepton via charged current interactions.

* The flavour states are not really well defined as they are not asymptotic states of the propagation Hamiltonian. It is a good approximation for ultrarelativistic neutrinos though.
 
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