A   B   C   D   E   F   G   H   I   J   K   L   M   N   O   P   Q   R   S   T   U   V   W   X   Y   Z  

Kirk, H.G.

Paper Title Page
WEPE065 The US Muon Accelerator Program 3491
 
  • A.D. Bross, S. Geer, V.D. Shiltsev
    Fermilab, Batavia
  • H.G. Kirk
    BNL, Upton, Long Island, New York
  • Y. Torun
    IIT, Chicago, Illinois
  • M.S. Zisman
    LBNL, Berkeley, California
 
 

An accelerator complex that can produce ultra-intense beams of muons presents many opportunities to explore new physics. A facility of this type is unique in that, in a relatively straightforward way, it can present a physics program that can be staged and thus move forward incrementally, addressing exciting new physics at each step. At the request of the US Department of Energy's Office of High Energy Physics, the Neutrino Factory and Muon Collider Collaboration and the Fermilab Muon Collider Task Force have recently submitted a proposal to create a Muon Accelerator Program that will have, as a primary goal, to deliver a Design Feasibility Study for an energy-frontier Muon Collider after a 7 year R&D program. This paper presents a description of a Muon Collider facility with a brief physics motivation, gives an overview of the proposal with respect to its organization and timeline and then discusses in some detail its major technical components.

 
WEPE078 The MERIT High-Power Target Experiment at the CERN PS 3527
 
  • K.T. McDonald
    PU, Princeton, New Jersey
  • J.R.J. Bennett
    STFC/RAL/ASTeC, Chilton, Didcot, Oxon
  • O. Caretta, P. Loveridge
    STFC/RAL, Chilton, Didcot, Oxon
  • A.J. Carroll, V.B. Graves, P.T. Spampinato
    ORNL, Oak Ridge, Tennessee
  • I. Efthymiopoulos, F. Haug, J. Lettry, M. Palm, H. Pereira
    CERN, Geneva
  • A. Fabich
    EBG MedAustron, Wr. Neustadt
  • H.G. Kirk, H. Park, T. Tsang
    BNL, Upton, Long Island, New York
  • N.V. Mokhov, S.I. Striganov
    Fermilab, Batavia
  • P.H. Titus
    PPPL, Princeton, New Jersey
 
 

We report on the analysis of data collected in the MERIT experiment at CERN during the Fall of 2007. These results validate the concept of a free mercury jet inside a high-field solenoid magnet as a target for a pulsed proton beam of 4-MW power, as needed for a future Muon Collider and/or Neutrino Factory.

 
WEPE101 A 4-MW Target Station for a Muon Collider or Neutrino Factory 3590
 
  • H.G. Kirk
    BNL, Upton, Long Island, New York
  • J.J. Back
    University of Warwick, Coventry
  • C.J. Densham, P. Loveridge
    STFC/RAL, Chilton, Didcot, Oxon
  • X.P. Ding
    UCLA, Los Angeles, California
  • V.B. Graves
    ORNL, Oak Ridge, Tennessee
  • F. Ladeinde, Y. Zhan
    SUNY SB, Stony Brook, New York
  • K.T. McDonald
    PU, Princeton, New Jersey
 
 

We outline a program of engineering design and simulation for a target station and pion production/capture system for a 4-MW proton beam at the front end of a Muon Collider or a Neutrino Factory. The target system consists of a free liquid-metal (nominally mercury) jet immersed in a high-field solenoid magnet capture system that also incorporates the proton beam dump. Topics to be studied include optimization of proton beam and jet target parameters, of the magnetic configuration for capture and subsequent transport of pions and muons, of the beam dump, of the radiation/thermal shielding of the capture magnets, and of the beam windows.

 
THPEC092 A Pion Production and Capture System for a 4MW Target Station 4272
 
  • X.P. Ding, D.B. Cline
    UCLA, Los Angeles, California
  • J.S. Berg, H.G. Kirk
    BNL, Upton, Long Island, New York
 
 

A study of a pion production and capture system for a 4MW target station for a neutrino factory or muon collider is presented. Using the MARS code, we simulate the pion production produced by the interaction of a free liquid mercury jet with an intense proton beam. We study the variation of meson production with the direction of the proton beam relative to the target. We also examine the influence on the meson production by the focusing of the proton beam. The energy deposition in the capture system is determined and the shielding required in order to avoid radiation damage is discussed.