WW Fusion in Higgs Production: Is it Possible in the Lab Frame?

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e^- + e^+\rightarrow\overline{\nu}_e + \nu_e + H
Can it possible for this process happen in lab frame? i.e. the positron is accelerated to collide with the electron target.
 
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if the process is allowed in one frame, it's allowed in ANY frame (that's Einstein's principle of relativity!). You can have this with the e+e- making a virtual Z, which then Higgsstrahlung's,with the Z decaying to neutrinos. It would be nearly impossible to see, though...
 
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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