Choose the positive direction along the incident Electron. With the neglected lepton masses and the paper's natural units, the initial four-momenta are
The squared centre-of-mass energy is the Lorentz invariant
Producing the Upsilon meson as the sole final resonance requires . The threshold positron energy is therefore
At that beam setting, four-momentum conservation gives and . Hence
The resonance moves in the incident-Electron direction, with velocity approximately . The laboratory sum of beam energies exceeds the resonance rest energy because the asymmetric beams also give it laboratory kinetic energy.

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