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P, CP and CPT symmetry in neutrino oscillation? (quick question)

  1. Apr 12, 2012 #1
    Just a quick question about notation really here. In neutrino oscillation we can calculate a probability of an oscillation occurring between two flavour eigenstates - invariably denoted [itex] P(\nu_{\alpha} \rightarrow \nu_{\beta}) [/itex]. I've got some confusion about what happens to this when we apply operators for P, CP and CPT.

    Charge conjugation turns particles to anti-particles, so I'm thinking this transformation would be denoted [itex] P(\nu_{\alpha} \rightarrow \nu_{\beta}) \rightarrow P(\overline{\nu_{\alpha}} \rightarrow \overline{\nu_{\beta}}) [/itex]

    Time reversal would presumably be [itex] P(\nu_{\alpha} \rightarrow \nu_{\beta}) \rightarrow P(\nu_{\beta} \rightarrow \nu_{\alpha}) [/itex]

    The combination of C and T operations would therefore be [itex] P(\nu_{\alpha} \rightarrow \nu_{\beta}) \rightarrow P(\overline{\nu_{\beta}} \rightarrow \overline{\nu_{\alpha}}) [/itex]

    My question is how would the parity transformation be incorporated here?

    ie. how would one write [itex] \hat{P} P(\nu_{\alpha} \rightarrow \nu_{\beta}), \hat{C}\hat{P} P(\nu_{\alpha} \rightarrow \nu_{\beta}) [/itex] and [itex] \hat{C}\hat{P}\hat{T} P(\nu_{\alpha} \rightarrow \nu_{\beta}) [/itex] ?
     
  2. jcsd
  3. Apr 12, 2012 #2
    The application of P will switch the chirality of a fermion. For neutrinos, this would be rather problematic, as, so far as we know, there are no right-handed neutrinos. (This is related to the fact that the weak force violates P maximally.) C, on the other hand, will reverse all charges, but will not reverse chirality; so, it will take you from a left-handed neutrino to a left-handed anti-neutrino. But, as you can check for yourself, the anti-neutrino state which must be included to allow spin-conservation in gauge interactions involving a left-handed neutrino is actually the right-handed anti-neutrino. (Equivalently, the existence of a left-handed anti-neutrino would require the existence of a right-handed neutrino.) So, again, we have a maximal violation, this time of C. It's only if we apply CP (turning a left-handed neutrino into a right-handed anti-neutrino) that we should expect to get a meaningful conjugation.

    Now, as it happens, we already know that the weak force slightly violates CP, as well; and, it's expected that there should be some CP violation in the neutrino sector; but, this ought to be a small effect compared to the size of the oscillation effects.

    CPT, on the other hand, should be an exact symmetry. There's a good deal of work showing that a violation of CPT necessarily entails a violation of local Lorentz symmetry.
     
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