Neutral pion decay: JPC conservation

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Discussion Overview

The discussion revolves around the decay of neutral pions (\(\pi^0\)) into two photons and the implications for the conservation of quantum numbers, specifically JPC (total angular momentum, parity, and charge conjugation). Participants explore the theoretical aspects of this decay process, including the roles of polarization and parity in the context of particle physics.

Discussion Character

  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant notes that the JPC of the pion is \(0^{-+}\) and of a photon is \(1^{--}\), leading to a question about how the decay to two photons, which can have JPC states of \(0^{++}\), \(1^{-+}\), and \(2^{++}\), can occur.
  • Another participant discusses the polarization state of the photons, indicating that it is odd under parity, and relates this to the decay process.
  • There is a clarification regarding the parity of a two-photon state, which depends on their relative polarizations, with a focus on the transverse nature of the photons in the decay.
  • A participant raises the idea of combining quantum numbers from two \(1^{--}\) systems to achieve a \(0^{-+}\) state, questioning the uniqueness of photons in this context.
  • Discussion includes the helicity states of the photons emitted in the decay, with an emphasis on how these states relate to parity eigenstates and the conditions under which odd parity is achieved.
  • Participants explore the implications of photon polarization and helicity on the parity of the two-photon system, noting that the parity can vary depending on the decay process.

Areas of Agreement / Disagreement

Participants express varying viewpoints on the implications of photon polarization and parity in the decay process. There is no consensus on the interpretation of how the quantum numbers combine or the specific conditions under which the decay occurs.

Contextual Notes

The discussion includes assumptions about the nature of photon states and their polarizations, as well as the dependence on the specific decay conditions of the pion. Some mathematical steps regarding the combination of helicity states and their relation to parity remain unresolved.

bayners123
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\pi^0s decay to two photons via the EM interaction. The J^{PC} of the pion is 0^{-+} and of a \gamma is 1^{--}.
\gamma\gamma therefore has J^{PC} = 0^{++}, 1^{-+}, 2^{++}.
This does not match the pion, so how can this decay occur?
 
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The polarization state is E1 x E2, and as you can see, this is odd under parity.
 
Vanadium 50 said:
The polarization state is E1 x E2, and as you can see, this is odd under parity.

Sorry, I don't quite understand your answer. Are you referring to the polarization of a single photon? If so, then yes I agree: that's why I put the Parity eigenvalue of the photon as -1, making the parity of a two photon system (-1) \times (-1)^L = (-1)^{L+1}
 
The parity of a two-photon state depends on their relative polarizations. They are both transverse, of course, and in the case of a pion decay the photon polarization vectors are also perpendicular to each other. This is what V50 means by E1 x E2, and such a state has odd space parity.
 
Hmm ok. Is it possible to think of this in terms of combining quantum numbers? So adding two 1^{--} systems and obtaining a 0^{-+}? If not, what's special about photon which makes this possible?

Also, does this imply that a two photon system can have either parity depending on what decayed?
 
The states you wrote down have the photons polarization vectors all pointing in the same direction. In this case, they are perpendicular to each other.
 
Consider the case where the pion decays at rest, and the two photons are emitted along the ± z-axis. A photon can either have helicity + (spin parallel to momentum) or helicity - (spin antiparallel to momentum) Since the total Jz of the two photons must be zero, they are either both helicity + or both helicity -. Call these states |++> and |-->.

Now the parity operation reverses helicity, so neither of these states is an eigenstate of parity. Rather the eigenstates are (|++> + |-->)/√2 (even parity) and (|++> - |-->)/√2 (odd parity). The odd parity state is the one we want.

bayners123 said:
does this imply that a two photon system can have either parity depending on what decayed?
So yes.

If you write the helicity states in terms of the states of transverse polarization, i.e. |±> = (|x> ± i |y>)/√2, you'll see that in the odd parity state the polarizations of the two photons come out perpendicular.
 
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Brilliant, thanks for both your help in understanding this!
 

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