Neutral pseudo meson decay into neutrino antineutrino

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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I'm following this paper by Kitaev on SL(2,R) representations and I'm having a problem in the normalization of the continuous eigenfunctions (eqs. (67)-(70)), which satisfy \langle f_s | f_{s'} \rangle = \int_{0}^{1} \frac{2}{(1-u)^2} f_s(u)^* f_{s'}(u) \, du. \tag{67} The singular contribution of the integral arises at the endpoint u=1 of the integral, and in the limit u \to 1, the function f_s(u) takes on the form f_s(u) \approx a_s (1-u)^{1/2 + i s} + a_s^* (1-u)^{1/2 - i s}. \tag{70}...

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