Beam%20parameters%20for%205%20TeV%20operation%20in%202008 - PowerPoint PPT Presentation

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Beam%20parameters%20for%205%20TeV%20operation%20in%202008

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In particular, no crossing angle is assumed and the same values for beta ... final result depends on the value of the longitudinal parameters. LHCCWG - April ... – PowerPoint PPT presentation

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Title: Beam%20parameters%20for%205%20TeV%20operation%20in%202008


1
Beam parameters for 5 TeV operation in 2008
  • M. Giovannozzi
  • General assumptions
  • Aperture
  • Luminosity
  • Overall target parameters
  • Next steps
  • Acknowledgements E. Chapochnikova, W. Herr, J.
    Tuckmantel

2
General assumptions - I
  • The analysis is based on the general parameters
    for Phase A.
  • In particular, no crossing angle is assumed and
    the same values for beta.
  • Longitudinal parameters
  • Nominal at 7 TeV
  • Emittance 2.5 eVs (due to blow-up)
  • Bunch length 7.55 cm
  • Rms energy spread 1.13 10-4
  • At 5 TeV one can assume the same values. However

3
General assumptions - II
  • The hardware for generating the longitudinal
    blow-up will not be ready for the commissioning.
  • Hence, emittance will be of the order of 1 eVs
    even at top energy.
  • The corresponding set of beam parameters (5 TeV
    or 7 TeV) will have to be defined (discussions
    with Elena on-going).

4
Aperture - I
7 TeV
Aperture in IR1 at top energy with beta2 m and
no crossing angle
5 TeV
5
Aperture - II
IR8. Spectrometer at 7 TeV value
Aperture in IR2 and 8 at 5 TeV with beta10 m
and 2 m, respectively. No external crossing angle
IR2. Spectrometer at 7 TeV value
6
Aperture - III
Summary of aperture bottleneck at 5 TeV
Aperture in IR5 at 5 TeV with beta2 m. No
crossing angle
N1 min Location
IR1 14 Q2
IR2 24 Q6
IR5 14 Q2
IR8 14 Q2
7
Aperture - IV
  • Some additional remarks
  • Werner analysed in details the situation with the
    external crossing angle for IR8. Down to beta2
    m aperture and separations are enough until bunch
    spacing of 50 ns.
  • Simulations concerning aperture vs. beam energy
    with
  • beta as from Phase A
  • No crossing angle
  • Constant separation bump

8
Luminosity
  • Target values depend on bg
  • Re-scale values from Phase A by 0.71.
  • Luminous region
  • Assuming same longitudinal parameters, then it
    re-scales with respect to the nominal case by
    0.71.
  • Nominal case
  • The final result depends on the value of the
    longitudinal parameters

9
Overall target parameters
  • First iteration on target parameters made (43 and
    156 bunches).
  • Finalisation once the longitudinal parameters
    will be fixed.
  • Also the table for the synchrotron radiation
    effects will need to be updated.

10
Next steps
  • Define longitudinal parameters
  • Re-evaluate the global set of beam parameters
  • Evaluate the situation concerning the radiation
    damping
  • However, the optics configuration is already
    available from the official LHC web site
  • http//lhc.web.cern.ch/lhc/
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