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Published byNorma Poole Modified over 6 years ago
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Some results on the LHC multibunch modes at 7 TeV/c
N. Mounet and E. Métral From Sacherer theory with the dipolar impedance (= the right impedance to put in a stability diagram) and synchrotron mode m=0, using a complete 25ns filling (3564 bunches), zero chromaticity and nominal LHC design parameters. N. Mounet and E. Métral - ICE meeting - 01/09/2010
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Coupled-bunch modes from the beam screens only w. r
Coupled-bunch modes from the beam screens only w.r.t all the machine elements in the model (Collimators + MBWs/MQWs magnets + beam screens + warm pipe + broad band) In horizontal, beam screens = 55% of the imaginary tune shift (i.e. -1/rise time), 1% of the real tune shift But pessimistic model of the beam screens in horizontal (used a factor 2 for the weld, see Carlo Zannini) N. Mounet and E. Métral - ICE meeting - 01/09/2010
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Coupled-bunch modes from the beam screens only w. r
Coupled-bunch modes from the beam screens only w.r.t all the machine elements in the model (Collimators + MBWs/MQWs magnets + beam screens + warm pipe + broad band) In vertical, beam screens = 49% of the imaginary tune shift (i.e. -1/rise time), 1% of the real tune shift N. Mounet and E. Métral - ICE meeting - 01/09/2010
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Coupled-bunch modes from all the machine elements in the model: effect of the bunch length
For the real tune shift, dependence in power law with a exponent of ~ -0.4 N. Mounet and E. Métral - ICE meeting - 01/09/2010
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Coupled-bunch modes from all the machine elements in the model: effect of the bunch length
For the imaginary tune shift (= -1/rise time), small linear dependence For the real tune shift, power law with a exponent of ~ -0.4 N. Mounet and E. Métral - ICE meeting - 01/09/2010
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