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ISBN-10: 1275068162

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4. These errors have not been used for simulations reported here and only serve for reference purposes. The errors for the IPN-Novosibirsk built warm Dl are shown in Tab. 5. ,f = 17 mm). ) denote the mean, mean uncertainty and rms of the harmonics. resoectivelv. 0. Rrej = 17 mm). 01 - - factory. The BNL built cold Dl magnets have the same coil design as the RHIC arc dipoles and their field quality is well established. These errors are shown in Tab. 6. In the next section we evaluate the dynamic aperture un.

The results are summarized in Table 2 for several fields of interest for Dl dipoles in LHC. 3 Current dependence of harmonics As the dipole field is increased, the iron in the yoke begins to saturate. Since the field strength is not uniform -10 -8 -6 -4 Nomml -2 0 2 4 6 Sextupole (1SOOA) between the geometric sextupole Fig. 85 T) in RHIC arc dipoles. R,,= 25 mm. 44 Workshop on LHC Interaction Region Correction Systems, BNL, Upton, New York, 1999 Table 3 Changes in harmonics at high fields in RHIC arc dipoles.

6] J. Wei, R. Gupta, M. Harrison, A. Jain, et al, PAC99 (1999). [7] J. Shi, Nuclear Jnstruments and Methods A (1999). [8] J-P Koutchouk, private communications. [9] W. , “LHC interaction region correction scheme studies”, these proceedings. 53 Workshop on LHC Interaction Region Correction Systems, BNL, Upton, New York, 1999 Sorting of High-Gradient Quadrupoles in LHC Interaction Regions Department J. Shi* of Physics & Astronomy, University Abstract of Kansas, Lawrence, reference harmonics Sorting of superconducting high-gradient quadrupoles in the LHC interaction regions with the vector sorting scheme is found to be quite effective in enlargement of the dynamic aperture and improvement of the linearity of the phasespace region occupied by beams.

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Arguments of the Hon. Edward Stanly, of Counsel for the Receiver, and T. W. Park, Esq., of Counsel for Alvin Adams, with the Charge of the Court by Anonymous


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