Author: Plate, S.R.
Paper Title Page
TUOCA2 Commissioning RHIC's Electron Lens 416
 
  • X. Gu, Z. Altinbas, M. Anerella, D. Bruno, M.R. Costanzo, W.C. Dawson, K.A. Drees, W. Fischer, B. Frak, D.M. Gassner, K. Hamdi, J. Hock, L.T. Hoff, A.K. Jain, J.P. Jamilkowski, R.F. Lambiase, Y. Luo, M. Mapes, A. Marone, C. Mi, R.J. Michnoff, T.A. Miller, M.G. Minty, C. Montag, S. Nemesure, W. Ng, D. Phillips, A.I. Pikin, S.R. Plate, P.J. Rosas, P. Sampson, J. Sandberg, L. Snydstrup, Y. Tan, R. Than, C. Theisen, P. Thieberger, J.E. Tuozzolo, P. Wanderer, W. Zhang
    BNL, Upton, Long Island, New York, USA
 
  Funding: Work supported by U.S. DOE under contract No DE-AC02-98CH10886 with the U.S. Department of Energy.
In the 2013 RHIC polarized proton run, it was found that the RHIC bunch intensity has reached a limit due to the head-on beam-beam interaction at 2x1011, as expected by simulations. To overcome this limitation, two electron lenses will be used for compensation. We report on the commissioning of new lattices that reduce beam-beam driven resonance driving terms, and bunch-by-bunch proton diagnostic during 2013 run. The effect of electron beam transport solenoids on the proton orbit was tested. The instrumentation for Blue electron lens was tested and electron beam was propagated from the gun to the collector. A timing system was implemented for the electron beam. Control software, machine protection and synoptic display were developed and tested during commissioning. Both Blue and Yellow electron lens superconducting magnets are installed and their field straightness was measured and corrected in the tunnel using a magnetic needle. The Yellow vacuum system and backscattered electron detectors installation are also completed now.
 
slides icon Slides TUOCA2 [3.466 MB]  
 
THPBA08 Partial Return Yoke for MICE - Engineering Design 1244
 
  • H. Witte, S.R. Plate
    BNL, Upton, Long Island, New York, USA
  • A.D. Bross
    Fermilab, Batavia, USA
  • J.S. Tarrant
    STFC/RAL, Chilton, Didcot, Oxon, United Kingdom
 
  Funding: Work supported by Brookhaven Science Associates, LC under Contract No. DE-AC02-98CH10886 with the U.S. Department of Energy.
MICE, which is an acronym for Muon Ionization Cooling Experiment, is a technology demonstration which is presently assembled at the Rutherford Appleton Laboratory in Didcot, UK. MICE aims to demonstrate ionization cooling experimentally, which is an essential technology for potential future accelerators such as a muon collider. The MICE channel consists of up to 18 large bore superconducting solenoids, which produce a substantial stray field. This stray field can jeopardize the operation of electrical and electronic equipment in the MICE hall. The concept of a partial flux return yoke has been developed, which reduces the stray field in the MICE hall to a safe level. This paper discusses the engineering design of the partial return yoke.
 
 
THPBA09 Partial Return Yoke for MICE - General Concept and Performance 1247
 
  • H. Witte, S.R. Plate
    BNL, Upton, Long Island, New York, USA
  • A.D. Bross
    Fermilab, Batavia, USA
  • J.S. Tarrant
    STFC/RAL, Chilton, Didcot, Oxon, United Kingdom
 
  Funding: Work supported by Brookhaven Science Associates, LC under Contract No. DE-AC02-98CH10886 with the U.S. Department of Energy.
MICE, which is an acronym for Muon Ionization Cooling Experiment, is a technology demonstration which is presently assembled at the Rutherford Appleton Laboratory in Didcot, UK. MICE aims to demonstrate ionization cooling experimentally, which is an essential technology for potential future accelerators such as a muon collider. The MICE channel consists of up to 18 large bore superconducting solenoids, which produce a substantial stray field. This stray field can jeopardize the operation of electrical and electronic equipment in the MICE hall. The concept of a partial flux return yoke has been developed, which reduces the stray field in the MICE hall to a safe level. This paper discusses the general concept and expected performance.