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Gschwendtner, E.

Paper Title Page
WEPE019 The CLIC Post-Collision Line 3386
 
  • E. Gschwendtner, A. Apyan, K. Elsener, A. Sailer, J.A. Uythoven
    CERN, Geneva
  • R. Appleby, M.D. Salt
    UMAN, Manchester
  • A. Ferrari, V.G. Ziemann
    Uppsala University, Uppsala
 
 

The 1.5TeV CLIC beams, with a total power of 14MW per beam, are disrupted at the interaction point due to the very strong beam-beam effect. As a result, some 3.5MW reach the main dump in form of beamstrahlung photons. About 0.5MW of e+e- pairs with a very broad energy spectrum need to be disposed along the post-collision line. The conceptual design of this beam line will be presented. Emphasis will be on the optimization studies of the CLIC post-collision line design with respect to the energy deposition in windows, dumps and scrapers, on the design of the luminosity monitoring for a fast feedback to the beam steering and on the background conditions for the luminosity monitoring equipment.

 
WEPE020 Background at the Interaction Point from the CLIC Post-Collision Line 3389
 
  • E. Gschwendtner, K. Elsener
    CERN, Geneva
  • R. Appleby, M.D. Salt
    UMAN, Manchester
  • A. Apyan
    Fermilab, Batavia
  • A. Ferrari
    Uppsala University, Uppsala
 
 

The 1.5TeV CLIC beams, with a total power of 14MW per beam, are disrupted at the interaction point due to the very strong beam- beam effect. The resulting spent beam products are transported to suitable dumps by the post-IP beam line, which generates beam losses and causes the production of secondary cascades towards the interaction region. In this paper the electromagnetic background at the IP are presented, which were calculated using biased Monte Carlo techniques. Also, a first estimate is made of neutron back-shine from the main beam dump.

 
THPEC046 Performance and Operational Experience of the CNGS Facility 4164
 
  • E. Gschwendtner, K. Cornelis, I. Efthymiopoulos, A. Ferrari, A. Pardons, W. Treberspurg, H. Vincke, J. Wenninger
    CERN, Geneva
  • D. Autiero
    IN2P3 IPNL, Villeurbanne
  • A. Guglielmi
    INFN/LNL, Legnaro (PD)
  • P.R. Sala
    Istituto Nazionale di Fisica Nucleare, Milano
 
 

The CNGS facility (CERN Neutrinos to Gran Sasso) aims at directly detecting muon to tau neutrino oscillations. An intense muon-neutrino beam (1017 muon neutrinos/day) is generated at CERN and directed over 732km towards the Gran Sasso National Laboratory, LNGS, in Italy, where two large and complex detectors, OPERA and ICARUS, are located. CNGS is the first long-baseline neutrino facility in which the measurement of the oscillation parameters is performed by observation of the tau-neutrino appearance. The facility is approved for a physics program of five years with a total of 22.5·1019 protons on target. Having resolved successfully some initial issues that occurred since its commissioning in 2006, the facility had its first complete year of physics in 2008. By the end of the 2009 physics run the facility will have delivered in total more than 5·1019 protons on target corresponding to ~2-3 tau neutrino events in the OPERA detector. The experiences gained in operating this 500 kW neutrino beam facility along with highlights of the beam performance in 2008 and 2009 are discussed.