In case you're still a little leery about the neutrino's existence or
conservation of lepton number, take a look at the decay of a neutron:
\[
n \rightarrow p + e^- + \overline{\nu}_e
\]
If lepton number conservation weren't a requirement, we could also see the
reaction
\[
n \rightarrow p + e^-
\]
These look pretty similar at first, but it turns out they're easily
distinguishable. If the neutron starts at rest, then momentum conservation
dictates that the momenta of the products (three in the reaction we
observe, two in the second one above) sum to zero. In the second reaction,
since there are only two products, they go ricocheting off in exactly
opposite directions. In the first, while we are very unlikely to detect the
neutrino, the electron and positron no longer have opposite momenta, which
is easily detectable (assuming you start with a slow enough neutron). And
it turns out (physics is, after all is said and done, an empirical science)
that the first reaction occurs and the second doesn't. This demonstrates the existence of the little neutral particle, and other similar experiments allow physicists to conclude that lepton number is always conserved.
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