Can antimatter(positron) can be converted into a matter(electron)

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Can antimatter(positron) can be converted into a matter(electron) . If yes what other particles are created in that reaction
 
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For leptons (muons, electrons, etc.), the sum of the number of leptons plus the number of anti-leptons is a constant. So if a positron disappears, an electron will have to disappear also. So there is no "conversion". A negative muon can decay into an electron plus neutrinos. A positive (anti-) muon can decay into a positron plus neutrinos. When Fermilab creates say 10^12 anti-protons, there are 10^12 protons or neutrons also created. If you want to check on the number of anti-protons in the Tevatron right now, look at
http://www-bd.fnal.gov/notifyservlet/www?project=outside
 
Toponium is a hadron which is the bound state of a valance top quark and a valance antitop quark. Oversimplified presentations often state that top quarks don't form hadrons, because they decay to bottom quarks extremely rapidly after they are created, leaving no time to form a hadron. And, the vast majority of the time, this is true. But, the lifetime of a top quark is only an average lifetime. Sometimes it decays faster and sometimes it decays slower. In the highly improbable case that...
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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