Neutral pseudo meson decay into neutrino antineutrino

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SUMMARY

The discussion focuses on the theoretical limits of neutral meson decays, specifically K0, D0, and B0 mesons, into neutrino-antineutrino pairs, which are highly suppressed due to flavor-changing neutral currents (FCNC). The experimental upper limit for the decay B0 → νν is established at 2.2 × 10-4 by BaBar, indicating that experimental limits exceed theoretical predictions. The decay process is further complicated by helicity suppression and requires a spin-flip of one outgoing fermion, leading to a significant reduction in decay rates. A naive estimation suggests that the branching ratios for these decays are exceedingly small, approximately 2 × 10-11 when compared to electron-positron decays.

PREREQUISITES
  • Understanding of flavor-changing neutral currents (FCNC)
  • Familiarity with meson decay processes
  • Knowledge of particle physics, specifically neutrino interactions
  • Basic grasp of angular momentum conservation in particle decays
NEXT STEPS
  • Research the implications of flavor-changing neutral currents in particle physics
  • Study the experimental techniques used by BaBar and LHCb for measuring meson decays
  • Explore the theoretical frameworks surrounding helicity suppression in particle decays
  • Investigate the branching ratios of other meson decay processes, such as K0 → e+e-
USEFUL FOR

Particle physicists, researchers in neutrino physics, and students studying advanced topics in meson decay and flavor physics will benefit from this discussion.

shakeel
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what are standards model limits on decay of K0, Do, B0 meson into a pair of neutrino and anti neutrino. I know that these highly suppressed due to involve FCNC. but if someone can tell me about theoretical limits on these reactions.
 
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I'm not sure if there are any calculations of that process - I would expect a branching fraction similar to the decay in two muons or less*, but experimentally it is probably the worst thing you can study.*
##B^0 \to \nu \nu## has an experimental upper limit of 2.2*10-4 from BaBar.*there, the experimental limits are still above theory, with the Bs measurement from LHCb and KL as exceptions
 
Should be helicity suppressed as well, correct?

Any Pseudoscalar (spin 0) going to two spin 1/2 particles requires a spin-flip on one of the outgoing fermions to conserve angular momentum. This spin flip introduces a proportionality to the mass of the outgoing fermion, in this case a neutrino, which is very very small in relationship to the decaying particle, thus highly suppressed.

A naive estimate, I would take the predicted rate for {K,D,B}_0 -> e+e-, and multiply it by the mass of the neutrino over the mass of the electron squared.

So

<br /> \frac{m_{\nu_e}^2}{m_{e}^2} = \left(\frac{2.2\,eV}{511\,keV}\right)^2 = 2 \times 10^{-11}<br />

so much smaller than the already-small branching ratios.
 

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