Neutral pseudo meson decay into neutrino antineutrino

In summary, the decay of K0, Do, and B0 mesons into a pair of neutrino and anti-neutrino is highly suppressed due to involving FCNC. The experimental upper limit for B0 -> nu nu is 2.2*10-4 from BaBar, but theoretically, the branching fraction is likely to be even smaller due to spin-flip suppression. A naive estimate suggests that the branching fraction would be 2 x 10^-11, much smaller than the already small experimental limits.
  • #1
shakeel
23
0
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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  • #2
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
 
  • #3
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

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

so much smaller than the already-small branching ratios.
 

1. What is a neutral pseudo meson?

A neutral pseudo meson is a type of subatomic particle that is composed of a quark and an antiquark, both of which have opposite charges. It is a type of meson that is considered to be "neutral" because it has no net electric charge.

2. How does a neutral pseudo meson decay into a neutrino and an antineutrino?

Neutral pseudo mesons decay into a neutrino and an antineutrino through a weak interaction process known as beta decay. In this process, one of the quarks in the meson transforms into a different type of quark, emitting a W boson. The W boson then decays into a neutrino and an antineutrino.

3. Why is this decay process important in particle physics?

This decay process is important in particle physics because it allows scientists to study the fundamental properties of subatomic particles, such as their mass and spin. It also helps to understand the behavior of the weak interaction, which is one of the four fundamental forces of nature.

4. How is the decay of a neutral pseudo meson into a neutrino and an antineutrino detected?

The decay of a neutral pseudo meson into a neutrino and an antineutrino is detected through the measurement of the energy and momentum of the particles produced in the decay. This can be done using specialized particle detectors, such as a scintillation detector or a bubble chamber.

5. Can this decay process occur in reverse?

Yes, the decay of a neutral pseudo meson into a neutrino and an antineutrino can also occur in reverse, known as inverse beta decay. In this process, a neutrino and an antineutrino combine to form a W boson, which then transforms into a quark-antiquark pair, producing a neutral pseudo meson.

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