“…The spread must be limited to those values that avoid crossing the dangerous resonance in the operation tune space of the machine. This crossing may also produce instabilities in the beam, limiting the performance of the machine (beam lifetime and luminosity) and creating radiation problems in the detectors (beam-halo) [11,12]. To obtain a high beam-beam parameter, with a small effect on the luminosity, and considering the experience gained from experiments at the LHC and Tevatron [13][14][15], the full crossing angle θ c is chosen to provide a beam-beam separation of n s = 10-12 RMS beam sizes for the parasitic crossings [8,16]:…”