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Landau–Yang theorem
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Landau–Yang theorem

In quantum mechanics, the Landau–Yang theorem is a selection rule for particles that decay into two on-shell photons. The theorem states that a massive particle with spin 1 cannot decay into two photons.[original 1][original 2]

Assumptions

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A photon here is any particle with spin 1, without mass and without internal degrees of freedom. The photon is the only known particle with these properties.

Consequences

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The theorem has several consequences in particle physics. For example:

  • The ρ meson cannot decay into two photons, differently from the neutral pion, that almost always decays into this final state (98.8% of times).[1]
  • The Z boson cannot decay into two photons.
  • The Higgs boson, whose decay into two photons was observed in 2012,[2][3] cannot have spin 1 in models that assume the Landau–Yang theorem. Measurements taken in 2013 have since confirmed that the Higgs has spin 0.[4]

Original references

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Additional references

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