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A. Belkacem, H. Gould, B. Feinberg, R. R. Bossingham, and W. E. Meyerhof, Phys. Rev. A 56, 2806 (1997).PLRAAN
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Scaled from an extrapolation in Ref
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Scaled from an extrapolation in Ref. 12.
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10
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85037243539
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The luminosity, which is proportional to the product of the density of ions in colliding bunches, does not follow a single exponential because the rate of loss declines faster than the number of ions remaining. We take the luminosity half-life as the time at which the luminosity has dropped by 50% from the initial luminosity. The initial luminosity per bunch and number of ions per bunch are (Formula presented) and (Formula presented) respectively, for the RHIC (57 bunches), from Ref
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The luminosity, which is proportional to the product of the density of ions in colliding bunches, does not follow a single exponential because the rate of loss declines faster than the number of ions remaining. We take the luminosity half-life as the time at which the luminosity has dropped by 50% from the initial luminosity. The initial luminosity per bunch and number of ions per bunch are (Formula presented) and (Formula presented) respectively, for the RHIC (57 bunches), from Ref. 5, and (Formula presented) and (Formula presented) respectively, for the LHC (608 bunches), from CERN Report No. CERN/AC/95-05 (LHC), 1995 (unpublished).
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11
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0000774155
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PRVCAN
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Capture from pair production cross sections for LHC are taken directly from Refs. 67 and by scaling by (Formula presented) from the cross sections in Refs. 812. An electromagnetic dissociation cross section of 220 b is taken from M. Vidović, M. Greiner, and G. Soff, Phys. Rev. C 48, 2011 (1993), and from Ref. 6.PRVCAN
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N. Claytor, A. Belkacem, T. Dinneen, B. Feinberg, and H. Gould, Phys. Rev. A 55, R842 (1997).PLRAAN
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