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Markiewicz, T.W.

Paper Title Page
WE6PFP078 Functional Requirements on the Design of the Detectors and the Interaction Region of an e+e- Linear Collider with a Push-Pull Arrangement of Detectors 2679
 
  • T.W. Markiewicz, M. Oriunno, A. Seryi
    SLAC, Menlo Park, California
  • K. Buesser
    DESY, Hamburg
  • P. Burrows
    OXFORDphysics, Oxford, Oxon
  • J.M. Hauptman
    ISU, Ames
  • A.A. Mikhailichenko
    CLASSE, Ithaca, New York
  • B. Parker
    BNL, Upton, Long Island, New York
  • T. Tauchi
    KEK, Ibaraki
 
 

Funding: Work supported in part by US DOE contract DE-AC02-76-SF00515.


The Interaction Region of the International Linear Collider* is based on two experimental detectors working in a push-pull mode. A time efficient implementation of this model sets specific requirements and challenges for many detector and machine systems, in particular the IR magnets, the cryogenics and the alignment system, the beamline shielding, the detector design and the overall integration. This paper attempts to separate the functional requirements of a push pull interaction region and machine detector interface from the conceptual and technical solutions being proposed by the ILC Beam Delivery Group and the three detector concepts**. As such, we hope that it provides a set of ground rules for interpreting and evaluation the MDI parts of the proposed detector concept’s Letters of Intent, due March 2009. The authors of the present paper are the leaders of the IR Integration Working Group within Global Design Effort Beam Delivery System and the representatives from each detector concept submitting the Letters Of Intent.


*ILC Reference Design Report, ILC-Report-2007-01.
**Materials of IR Engineering Design Workshop, 2007, http://www-conf.slac.stanford.edu/ireng07

 
WE6RFP030 Recent Progress on the Design of a Rotatable Copper Collimator for the LHC Collimation Upgrade 2853
 
  • J.C. Smith, L. Keller, S.A. Lundgren, T.W. Markiewicz
    SLAC, Menlo Park, California
  • L. Lari
    EPFL, Lausanne
 
 

Funding: Work supported in part by the U.S. Department of Energy contract DE-AC02-76SF00515


The Phase II upgrade to the LHC collimation system calls for complementing the 30 high robust Phase I graphite collimators with 30 high Z Phase II collimators. One option is to use metallic rotatable collimators and this design will be discussed here. The Phase II collimators must be robust in various operating conditions and accident scenarios. Design issues include: 1) Collimator jaw deflection due to heating and sagita must be small when operated in the steady state condition, 2) Collimator jaws must withstand transitory periods of high beam impaction with no permanent damage, 3) Jaws must recover from accident scenario where up to 7 full intensity beam pulses impact on the jaw surface and 4) The beam impedance contribution due to the collimators must be small to minimize coherent beam instabilities. The current design will be presented.

 
TH5PFP008 Accelerator Physics Concept for Upgraded LHC Collimation Performance 3202
 
  • R.W. Assmann, G. Bellodi, J.M. Jowett, E. Métral, Th. Weiler
    CERN, Geneva
  • L. Keller, T.W. Markiewicz
    SLAC, Menlo Park, California
 
 

The LHC collimation system is implemented in phases, in view of the required extrapolation by 2-3 orders of magnitude beyond Tevatron and HERA experience in stored energy. All available simulations predict that the LHC proton beam intensity with the "phase 1" collimation system may be limited by the impedance of the collimators or cleaning efficiency. Maximum efficiency requires collimator materials very close to the beam, generating the dominant resistive impedance in the LHC. Above a certain intensity the beam is unstable. On the other hand, even if collimators are set very close to the beam, the achievable cleaning efficiency is predicted to be inadequate, requiring either beam stability beyond specifications or reduced intensity. The accelerator physics concept for upgrading cleaning efficiency, for both proton and heavy ion beams, and reducing collimator-related impedance is described. Besides the "phase 2" secondary collimators, new collimators are required in a few super-conducting regions.