The optimal path for the LHC luminosity upgrade includes an increase in the beam current ( i . e . the number of particles in the beams ) and the modification of the two high-luminosity interaction regions, ATLAS and CMS . To achieve these increases, the energy of the beams at the point that they are injected into the LHC should also be increased to.
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Accelerator systems for ion implantation are generally classified into medium current ( ion beam currents between 10 ?A and ~ 2 mA ), high current ( ion beam currents up to ~ 30 mA ), high energy ( ion energies above 200 keV and up to 10 MeV ), and very high dose ( efficient implant of dose greater than 10 16 ions / cm 2 ).
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Accelerator systems for ion implantation are generally classified into medium current ( ion beam currents between 10 ?A and ~ 2 mA ), high current ( ion beam currents up to ~ 30 mA ), high energy ( ion energies above 200 keV and up to 10 MeV ), and very high dose ( efficient implant of dose greater than 10 16 ions / cm 2 ).
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