03 Linear Colliders, Lepton Accelerators and New Acceleration Techniques

A09 Muon Accelerators and Neutrino Factories

Paper Title Page
WEPEC082 Computational Modeling of Muons passing through Gas Pressured RF Cavities 3070
 
  • A. Samolov, A.L. Godunov
    ODU, Norfolk, Virginia
 
 

Using high-pressure RF cavities for muon colliders would provide higher accelerating gradients, that is crucial for fast acceleration of short-living muons .This approach requires a good evaluation for mechanisms of muon - low-Z gas interaction, including such effects as multiple scattering and space charge effects. Most present simulation tools (GEANT4, G4MICE) for muon beams are based on single particle tracking, where collective effects are not taken into account. We use a modified molecular dynamic simulation technique to study effects of both multiple scattering and space charge screening by the gas on scattering, energy loss, and propagation of muons during both ionization cooling and acceleration.

 
WEPE042 Mice Status 3443
 
  • A. Alekou
    Imperial College of Science and Technology, Department of Physics, London
 
 

Muon ionization cooling provides the only practical solution to prepare high brilliance beams necessary for a neutrino factory or muon colliders. The muon ionization cooling experiment (MICE)* is under development at the Rutherford Appleton Laboratory (UK). It comprises a dedicated beam line to generate a range of input emittance and momentum, with time-of-flight and Cherenkov detectors to ensure a pure muon beam. A first measurement of emittance is performed in the upstream magnetic spectrometer with a scintillating fiber tracker. A cooling cell will then follow, alternating energy loss in liquid hydrogen and RF acceleration. A second spectrometer identical to the first one and a particle identification system provide a measurement of the outgoing emittance. In May 2010 it is expected that the beam and most detectors will be commissioned and the time of the first measurement of input beam emittance closely approaching. The plan of steps of measurements of emittance and cooling, that will follow in the rest of 2010 and later, will be reported.


This abstract is submitted by the chear of the MICE speaker bureau. A member of the collaboration will be soon identified to present the poster and added a co-author.

 
WEPE043 Study for a Racetrack FFAG based Muon Ring Cooler 3446
 
  • A. Sato
    Osaka University, Osaka
 
 

FFAG lattices with racetrack-shape has been studied to cool muon beams. The ring has straight sections with FFAG magnets, which makes enough space to install kicker magnets to inject and extract the muon beam. Wedge absorbers using superfluid helium and RF cavities are installed to the ring. This paper reports progress of the study.

 
WEPE046 G4beamline Simulation for the COMET Solenoid Channel 3449
 
  • A. Sato
    Osaka University, Osaka
 
 

The COMET is an experiment to search for the process of muon to electron conversion in a muonic atom, and is in its design phase to be carried out at J-PARC in near future. The experiment uses a long superconducting solenoid channels from a pion production target to a detector system. In order, to study the solenoid channel the g4beamline is used for the magnetic field calculation and beam tracking. This paper reports the status of the simulation studies.

 
WEPE047 Frictional Cooling for a Slow Muon Source 3452
 
  • Y. Bao
    IHEP Beijing, Beijing
  • A. Caldwell, G.X. Xia
    MPI-P, München
  • D. Greenwald
    MPI für Physics, Muenchen
 
 

Low energy muon beams are useful for a wide range of physics experiments. High quality muon beams are also required for muon colliders and neutrino factories. The frictional cooling method holds promise for delivering slow muon beams with narrow energy spreads. With this technology, we consider the production of a cold muon beam from a surface muon source, such as that at the Paul Scherrer Institute. A cooling scheme based on frictional cooling is outlined. Simulation results show that the efficiency of slow muon production can be raised to 1%, which is significantly higher than current schemes.

 
WEPE050 Alternative Muon Front-end for the International Design Study (IDS) 3455
 
  • C.T. Rogers
    STFC/RAL/ASTeC, Chilton, Didcot, Oxon
  • A. Alekou
    Imperial College of Science and Technology, Department of Physics, London
  • M. Martini, G. Prior
    CERN, Geneva
  • D.V. Neuffer
    Fermilab, Batavia
  • D. Stratakis
    BNL, Upton, Long Island, New York
  • C. Y. Yoshikawa
    Muons, Inc, Batavia
  • M.S. Zisman
    LBNL, Berkeley, California
 
 

We discuss alternative designs of the muon capture front end of the Neutrino Factory International Design Study (IDS). In the front end, a proton bunch on a target creates secondary pions that drift into a capture channel, decaying into muons. A sequence of RF cavities forms the resulting muon beams into strings of bunches of differing energies, aligns the bunches to (nearly) equal central energies, and initiates ionization cooling. This design is affected by limitations on accelerating gradients within magnetic fields. The effects of gradient limitations are explored, and mitigation strategies are presented.

 
WEPE051 Muon Cooling Performance in Various Neutrino Factory Cooling Cell Configurations using G4MICE 3458
 
  • A. Alekou, J. Pasternak
    Imperial College of Science and Technology, Department of Physics, London
  • C.T. Rogers
    STFC/RAL/ASTeC, Chilton, Didcot, Oxon
 
 

The Neutrino Factory is a planned particle accelerator complex that will produce an intense, focused neutrino beam, using neutrinos from muon decay. Such high neutrino intensities can only be achieved by reducing the muon beam emittance using an ionization cooling system. The G4MICE software is used to study the performance of various cooling cell configurations. A comparison is drawn between the cooling in the FS2 cells, the baseline Neutrino Factory and doublet cells. The beam dynamics in each of cooling channels are presented. The lattices are compared with respect to the equilibrium emittance, muon transmission, acceptance and evolution of emittance along the channel. Conclusions for a possible optimisation of the future muon cooling channel of the Neutrino Factory are presented.

 
WEPE052 Optimization of the MICE Muon Beam Line 3461
 
  • M. Apollonio
    Imperial College of Science and Technology, Department of Physics, London
  • M.A. Rayner
    OXFORDphysics, Oxford, Oxon
 
 

In the Muon Ionization Cooling Experiment (MICE) at RAL muons are produced and transported in a dedicated beamline connecting the production point (target) to the diffuser, a mechanism inside the first spectrometer solenoid designed to inflate the initial normalized emittance up to 10 mm rad in a controlled fashion. In order to match the incoming muons to the downstream experiment, covering all the possible values of the emittance-momentum matrix, an optimisation procedure has been devised which is based upon a genetic algorithm coupled to the tracking code G4Beamline. Details of beamline tuning and initial measurements are discussed.

 
WEPE053 Muon Polarimeter in a Neutrino Factory Decay Ring 3464
 
  • M. Apollonio
    Imperial College of Science and Technology, Department of Physics, London
  • A.P. Blondel
    DPNC, Genève
  • D.J. Kelliher
    STFC/RAL/ASTeC, Chilton, Didcot, Oxon
 
 

Monitoring the muon beam properties in the final stage of the Neutrino Factory (the Decay Ring) is important for the understanding of the beam itself and a crucial piece of information for the downstream physics detectors. The main topics to be assessed are: knowledge of the muon beam energy, divergence of the muon beam and muon beam current. In the framework of the International Design Study for the Neutrino Factory (IDS-NF) a Race Track model Decay Ring based on G4beamline has been produced to understand how electrons from muon decays can be used to infer the energy properties of the beam via the spin depolarisation technique. The use of other codes, like Zgoubi, to generate a realistic beam including effects like spin polarisation, are considered. A general discussion on the remaining topics is presented.

 
WEPE054 The MICE Muon Beam: Status and Progress 3467
 
  • A.J. Dobbs, M. Apollonio, K.R. Long, J. Pasternak
    Imperial College of Science and Technology, Department of Physics, London
  • D.J. Adams
    STFC/RAL/ISIS, Chilton, Didcot, Oxon
 
 

The international Muon Ionisation Cooling Experiment (MICE) is designed to provide a proof of principal of the ionisation cooling technique proposed to reduce the muon beam phase space at a future Neutrino Factory or Muon Collider. The pion production target is a titanium cylinder that is dipped into the proton beam of the Rutherford Appleton Laboratory's ISIS 800 MeV synchrotron. Studies of the particle rate in the MICE muon beam are presented as a function of the beam loss induced in ISIS by the MICE target. The implications of the observed beam loss and particle rate on ISIS operation and MICE data taking is discussed.

 
WEPE055 The COherent Muon to Electron Transition (COMET) Experiment 3470
 
  • A. Kurup
    Imperial College of Science and Technology, Department of Physics, London
  • A. Kurup
    Fermilab, Batavia
 
 

The COherent Muon to Electron Transition (COMET) experiment aims to measure muon to electron conversion with an unprecedented sensitivity of less than 1 in 10 million billion. The COMET experiment was given stage 1 approval by the J-PARC Program Advisory Committee in July 2009 and work is currently underway towards preparing a technical design report for the whole experiment. The need for this sensitivity places several stringent requirements on the beamline, such as, a pulsed proton beam with an extinction level between pulses of 9 orders of magnitude; a 5T superconducting solenoid operating near a high radiation environment; precise momentum selection of a large emittance muon beam and momentum selection and collimation of a large emittance electron beam. This paper will present the current status of the various components of the COMET beamline.

 
WEPE056 Accelerator and Particle Physics Research for the Next Generation Muon to Electron Conversion Experiment - the PRISM Task Force 3473
 
  • J. Pasternak, L.J. Jenner, Y. Uchida
    Imperial College of Science and Technology, Department of Physics, London
  • R.J. Barlow
    UMAN, Manchester
  • K.M. Hock, B.D. Muratori
    Cockcroft Institute, Warrington, Cheshire
  • D.J. Kelliher, S. Machida, C.R. Prior
    STFC/RAL/ASTeC, Chilton, Didcot, Oxon
  • Y. Kuno, A. Sato
    Osaka University, Osaka
  • A. Kurup
    Fermilab, Batavia
  • J.-B. Lagrange, Y. Mori
    KURRI, Osaka
  • M. Lancaster
    UCL, London
  • S.A. Martin
    FZJ, Jülich
  • C. Ohmori
    KEK/JAEA, Ibaraki-Ken
  • J. Pasternak
    STFC/RAL, Chilton, Didcot, Oxon
  • S.L. Smith
    STFC/DL/ASTeC, Daresbury, Warrington, Cheshire
  • H. Witte, T. Yokoi
    JAI, Oxford
 
 

The next generation of lepton flavour violation experiments will use high intensity and high quality muon beams. Such beams can be produced by sending a short proton pulse to the pion production target, capturing pions and performing RF phase rotation on the resulting muon beam in an FFAG ring, which was proposed for the PRISM project. A PRISM task force was created to address the accelerator and detector issues that need to be solved in order to realise the PRISM experiment. The parameters of the initial proton beam required and the PRISM experiment are reviewed. Alternative designs of the PRISM FFAG ring are presented and compared with the reference design. The ring injection/extraction system, matching with the solenoid channel and progress on the ring's main hardware systems like RF and kicker magnet are discussed. The activity on the simulation of a high sensitivity experiment and the impact on physics reach is described. The progress and future directions of the study are presented in this paper.

 
WEPE057 Injection/Extraction System of the Muon FFAG for the Neutrino Factory 3476
 
  • J. Pasternak, M. Aslaninejad
    Imperial College of Science and Technology, Department of Physics, London
  • J.S. Berg
    BNL, Upton, Long Island, New York
  • D.J. Kelliher, S. Machida
    STFC/RAL/ASTeC, Chilton, Didcot, Oxon
  • J. Pasternak
    STFC/RAL, Chilton, Didcot, Oxon
  • H. Witte
    JAI, Oxford
 
 

Nonscaling FFAG is required for the muon acceleration in the Neutrino Factory, which baseline design is under investigation in the International Design Study (IDS-NF). In order to inject/extract the muon beam with a very large emittance, several strong kickers with a very large aperture are required distributed in many lattice cells. Once the sufficient orbit separation is obtained by the kickers, the final degree of separation from the lattice is made by the septum, which needs to be superconducting. The geometry of the symmetric solutions allowing to inject/extract both signs of muons is presented. The preliminary design of the kicker and septum magnets is given.

 
WEPE060 Investigation of Beam Loading Effects for the Neutrino Factory Muon Accelerator 3479
 
  • J.K. Pozimski, M. Aslaninejad, C. Bontoiu
    Imperial College of Science and Technology, Department of Physics, London
  • J.S. Berg
    BNL, Upton, Long Island, New York
  • S.A. Bogacz
    JLAB, Newport News, Virginia
  • S. Machida
    STFC/RAL/ASTeC, Chilton, Didcot, Oxon
 
 

The IDS study showed that a Neutrino Factory seems to be the most promising candidate for the next phase of high precision neutrino oscillation experiments. A part of the increased precision is due to the fact that in a Neutrino Factory the decay of muons produces a neutrino beam with narrow energy distribution and divergence. The effect of beam loading on the energy distribution of the muon beam in the Neutrino Factory has been investigated numerically. The simulations have been performed using the baseline accelerator design including cavities for different number of bunch trains and bunch train timing. A detailed analysis of the beam energy distribution expected is given together with a discussion of the energy spread produced by the gutter acceleration in the FFAG and the implications for the neutrino oscillation experiments will be presented.

 
WEPE061 Measurements of Muon Beam Properties in MICE 3482
 
  • M.A. Rayner, J.H. Cobb
    OXFORDphysics, Oxford, Oxon
 
 

The Muon Ionization Cooling Experiment is one lattice section of a cooling channel suitable for conditioning the muon beam at the front end of a Neutrino Factory or Muon Collider. Scintillating fibre spectrometers and 50 ps resolution timing detectors provide the unprecedented opportunity to measure the initial and final six-dimensional phase space vectors of individual muons. The capability of MICE to study the evolution of muon beams through a solenoidal lattice will be described.

 
WEPE062 MICE Target Operation and Monitoring 3485
 
  • P. Hodgson, C.N. Booth, P.J. Smith
    Sheffield University, Sheffield
 
 

The MICE experiment requires a beam of low energy muons to demonstrate muon cooling. A target mechanism has been developed that inserts a small titanium target into the circulating ISIS beam during the last 2ms before extraction. The target mechanism has been in operation in the ISIS beam during 2009 and a large set of useful data has been obtained describing the target's operational parameters. This has allowed the commissioning of the initial section of the MICE beam line and instrumentation, and the close monitoring of target performance. This work describes these target parameters and presents some of the results from operational shifts.

 
WEPE063 MICE Target Hardware 3488
 
  • P. Hodgson, C.N. Booth, P.J. Smith
    Sheffield University, Sheffield
  • J.S. Tarrant
    STFC/RAL, Chilton, Didcot, Oxon
 
 

The MICE experiment uses a beam of low energy muons to test the feasibility of ionisation cooling. This beam is derived parasitically from the ISIS accelerator at the Rutherford Appleton Laboratory. A target mechanism has been developed and deployed that rapidly inserts a small titanium target into the circulating proton beam immediately prior to extraction without undue disturbance of the primary ISIS beam. The first target drive was installed in ISIS during 2008 and operated successfully for over 100,000 pulses. A second upgraded design was installed in 2009 and is currently in operation. The technical specification for this upgraded design is given and the motivation for many of the improvements is discussed. In addition possible future improvements to the current design are discussed.

 
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.

 
WEPE066 Beam Test of a High Pressure Cavity for a Muon Collider 3494
 
  • M. Chung, A. Jansson, A. Moretti, A.V. Tollestrup, K. Yonehara
    Fermilab, Batavia
  • A. Kurup
    Imperial College of Science and Technology, Department of Physics, London
 
 

To demonstrate the feasibility of a high pressure RF cavity for use in the cooling channel of a muon collider, an experimental setup that utilizes 400-MeV Fermilab linac proton beam has been developed. In this paper, we describe the beam diagnostics and the collimator system for the experiment, and report the initial results of the beam commissioning. The transient response of the cavity to the beam is measured by the electric and magnetic pickup probes, and the beam-gas interaction is monitored by the optical diagnostic system composed of a spectrometer and two PMTs.

 
WEPE067 Beam-induced Electron Loading Effects in High Pressure Cavities for a Muon Collider 3497
 
  • M. Chung, A. Jansson, A.V. Tollestrup, K. Yonehara
    Fermilab, Batavia
  • Z. Insepov
    ANL, Argonne
 
 

Ionization cooling is a critical building block for the realization of a muon collider. To suppress breakdown in the presence of the external magnetic field, an idea of using an RF cavity filled with high pressure hydrogen gas is being considered for the cooling channel design. In the high pressure RF cavity, ionization energy loss and longitudinal momentum recovery can be achieved simultaneously. One possible problem expected in the high pressure RF cavity is, however, the dissipation of significant RF power through the electrons accumulated inside the cavity. The electrons are generated from the beam-induced ionization of the high pressure gas. To characterize this detrimental loading effect, we develop a simplified model that relates the electron density evolution and the observed pickup voltage signal in the cavity, with consideration of several key molecular processes such as the formation of the polyatomic molecules and ions, excitation, recombination and electron attachment. This model is expected to be compared with the actual beam test of the cavity in the MuCool Test Area (MTA) of Fermilab.

 
WEPE068 Muon Capture in the Front End of the IDS Neutrino Factory 3500
 
  • D.V. Neuffer
    Fermilab, Batavia
  • M. Martini, G. Prior
    CERN, Geneva
  • C.T. Rogers
    STFC/RAL/ASTeC, Chilton, Didcot, Oxon
  • C. Y. Yoshikawa
    Muons, Inc, Batavia
 
 

We discuss the design of the muon capture front end of a neutrino factory and present studies of variations of its components. In the front end, a proton bunch on a target creates secondary pions that drift into a capture transport channel, decaying into muons. A sequence of rf cavities forms the resulting muon beams into strings of bunches of differing energies, aligns the bunches to (nearly) equal central energies, and initiates ionization cooling. The cooling section uses absorber material (reducing the 3-D muon momenta) alternating with rf cavities (restoring longitudinal momentum) within strong focusing magnetic fields. The design is affected by limitations on accelerating gradients within magnetic fields. The effects of gradient limitations are explored, and mitigation strategies are presented. Variations of the ionization cooling and acceleration scenarios and extensions toward use in a muon collider are discussed.

 
WEPE069 Study of Electron Swarm in High Pressure Hydrogen Gas Filled RF Cavities 3503
 
  • K. Yonehara, M. Chung, A. Jansson, A. Moretti, M. Popovic, A.V. Tollestrup
    Fermilab, Batavia
  • M. Alsharo'a, R.P. Johnson, M. Notani
    Muons, Inc, Batavia
  • D. Huang
    IIT, Chicago, Illinois
  • Z. Insepov
    ANL, Argonne
  • T. Oka, H. Wang
    University of Chicago, Chicago, Illinois
  • D. Rose
    Voss Scientific, Albuquerque, New Mexico
 
 

A high pressurizing hydrogen gas filled RF cavity has a great potential to apply for muon colliders. It generates high electric field gradients in strong magnetic fields with various conditions. As the remaining demonstration, it must work under high radiation conditions. A high intensity muon beam will generate a beam-induced electron swarm via the ionization process in the cavity. A large amount of RF power will be consumed into the swarm. We show the recent non-beam test and discuss the electron swarm dynamics which plays a key role to develop a high pressure RF cavity.

 
WEPE071 Integrated Low Beta Region Muon Collider Detector Design 3506
 
  • M.A.C. Cummings
    Muons, Inc, Batavia
  • D. Hedin
    Northern Illinois University, DeKalb, Illinois
 
 

Muon Colliders produce high rates of unwanted particles near the beams in the detector regions. Previous designs have used massive shielding to reduce these backgrounds, at a cost of creating dead regions in the detectors. To optimize the physics from the experiments, new ways to instrument these regions are needed. Since the last study of a muon collider detector in the 1990s, new types of detectors, such as solid state photon sensors that are fine-grained, insensitive to magnetic fields, radiation-resistant, fast, and inexpensive have become available. These can be highly segmented to operate in the regions near the beams. We re-evaluate the detector design, based on new sensor technologies. Simulations that incorporate conditions in recent muon collider interaction region designs are used to revise muon collider detector parameters based on particle type and occupancy. Shielding schemes are studied for optimization. Novel schemes for the overall muon collider design, including "split-detectors", are considered.

 
WEPE072 Incorporating RF into a Muon Helical Cooling Channel 3509
 
  • S.A. Kahn, G. Flanagan, R.P. Johnson, M.L. Neubauer
    Muons, Inc, Batavia
  • V.S. Kashikhin, M.L. Lopes, K. Yonehara, M. Yu, A.V. Zlobin
    Fermilab, Batavia
 
 

A helical cooling channel (HCC) consisting of a pressurized gas absorber imbedded in a magnetic channel that provides solenoidal, helical dipole and helical quadrupole fields has shown considerable promise in providing six-dimensional cooling for muon beams. The energy lost by muons traversing the gas absorber needs to be replaced by inserting RF cavities into the HCC lattice. Replacing the substantial muon energy losses using RF cavities with reasonable gradients will require a significant fraction of the channel length be devoted to RF. However to provide the maximum phase space cooling and minimum muon losses, the HCC should have a short period and length. In this paper we examine an approach where each HCC cell has an RF cavity imbedded in the aperture with the magnetic coils are split allowing for half of the cell length to be available for the RF coupler and other services.

 
WEPE073 Quasi-isochronous Muon Collection Channels 3512
 
  • C. Y. Yoshikawa, C.M. Ankenbrandt
    Muons, Inc, Batavia
  • D.V. Neuffer
    Fermilab, Batavia
 
 

Intense muon beams have many potential applications, including neutrino factories and muon colliders. However, muons are produced as tertiary beams, resulting in diffuse phase space distributions. To make useful beams, the muons must be rapidly cooled before they decay. An idea conceived recently for the collection and cooling of muon beams, namely, the use of a Quasi-Isochronous Helical Channel (QIHC) to facilitate capture of muons into RF buckets, has been developed further. The resulting distribution could be cooled quickly and coalesced into a single bunch to optimize the luminosity of a muon collider. After a brief elaboration of the QIHC concept, some recent developments are described.

 
WEPE074 A Possible Hybrid Cooling Channel for a Neutrino Factory 3515
 
  • M.S. Zisman
    LBNL, Berkeley, California
  • J.C. Gallardo
    BNL, Upton, Long Island, New York
 
 

A Neutrino Factory requires an intense and highly cooled (in transverse phase space) muon beam. We discuss a hybrid approach for a linear 4D cooling channel consisting of high-pressure gas-filled RF cavities –potentially allowing high gradients without breakdowns– and discrete LiH absorbers to provide the necessary energy loss that results in the needed muon beam cooling. We report simulations of the channel performance and its comparison with the vacuum case; we also discuss the various technical and safety issues associated with cavities filled with high-pressure hydrogen gas. Even with additional windows that might be needed for safety reasons, the channel performance is comparable to that of the original, all-vacuum Feasibility Study 2a channel on which our design is based. If tests demonstrate that the gas-filled RF cavities can operate properly with an intense beam of ionizing particles passing through them, our approach would be an attractive way of avoiding possible breakdown problems with a vacuum RF channel.

 
WEPE075 Large-Acceptance Linac for Accelerating Low-Energy Muons 3518
 
  • S.S. Kurennoy, A.J. Jason, H.M. Miyadera
    LANL, Los Alamos, New Mexico
 
 

We propose a high-gradient linear accelerator for accelerating low-energy muons and pions in a strong solenoidal magnetic field. The acceleration starts immediately after collection of pions from a target by solenoidal magnets and brings muons to a kinetic energy of about 200 MeV over a distance of the order of 10 m. At this energy, both an ionization cooling of the muon beam and its further acceleration in a superconducting linac become feasible. The project presents unique challenges ' a very large energy spread in a highly divergent beam, as well as pion and muon decays ' requiring large longitudinal and transverse acceptances. One potential solution incorporates a normal-conducting linac consisting of independently fed 0-mode RF cavities with wide apertures closed by thin metal windows or grids. The guiding magnetic field is provided by external superconducting solenoids. The cavity choice, overall linac design considerations, and simulation results of muon acceleration are presented. While the primary applications of such a linac are for homeland defense and industry, it can provide muon fluxes high enough to be of interest for physics experiments.

 
WEPE076 Simulation of Large Acceptance Muon Linac 3521
 
  • H.M. Miyadera, A.J. Jason, S.S. Kurennoy
    LANL, Los Alamos, New Mexico
 
 

Many groups are working on muon accelerators for future neutrino factory and muon colliders. One of the applications of muon accelerator is muon radiography which is a promising method to investigate large objects taking advantage of the long penetration lengths of muons. We propose a compact muon accelerator that has a large energy and a phase acceptance to capture relatively low energy pion/muon of 10 - 100 MeV and accelerates them to 200 MeV without any beam cooling. Like an RFQ, mixed buncher/acceleration mode provides phase bunching during the acceleration. Our current design uses 805 MHz zero-mode normal-conducting cavities with 35 MV/m peak field*. The normal conducting cavities are surrounded by superconducting coils that produce 5 T focusing field. We ran Monte Carlo simulations to optimize linac parameters such as frequency and acceleration gradient. Muon energy loss and scattering effects at the cavity windows are studied, too. The simulation showed that about 10 % of the pion/muon injected into the linac can be accelerated to 200 MeV. Further acceleration is possible with superconducting linac.


* S. Kurennoy et al., IPAC 2010.

 
WEPE077 Permanent Magnet Quadrupole Final Focus System for the Muon Collider 3524
 
  • F.H. O'Shea, J.B. Rosenzweig
    UCLA, Los Angeles, California
  • G. Andonian
    RadiaBeam, Marina del Rey
 
 

One of the challenges of the proposed muon collider is the beam size at the interaction region. The current target for the beta function (beta-star) is 10mm for the 1.5TeV scenario with a beam emittance of 25mm-mrad. In this paper, we describe the design and development of a final focusing scheme that attempts to reach these parameters. The final focus scheme is based on the use of permanent magnet quadrupoles (PMQ) in a triplet configuration. Initial simulations show that the PMQs reach gradients as high as ~990T/m using Praseodymium based magnets in a Halbach style arrangement. Possible methods for tuning the PMQs at the interaction region, via temperature control and high-resolution movers, are also described.

 
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.

 
WEPE079 Particle Production in the MICE Beamline 3530
 
  • L. Coney
    UCR, Riverside, California
  • A.J. Dobbs
    Imperial College of Science and Technology, Department of Physics, London
  • Y. Karadzhov
    Sofia University St. Kliment Ohridski, Faculty of Physics, Sofia
 
 

The Muon Ionization Cooling Experiment (MICE) is being built at the Rutherford Appleton Laboratory (RAL) to test ionization cooling of a muon beam. Successful demonstration of cooling is a necessary step along the path toward creating future high intensity muon beams in either a Neutrino Factory or Muon Collider. Production of particles in the MICE beamline begins with a titanium target dipping into the ISIS proton beam. The resulting pions are captured, momentum-selected, and fed into a 5T superconducting decay solenoid which contains the pions and their decay muons. Another dipole then selects the final particles for propagation through the rest of the MICE beamline. Within the last year, the MICE target has been redesigned, rebuilt, and has begun operating in ISIS. The decay solenoid has also become operational, dramatically increasing the number of particles in the MICE beamline. In parallel, particle identification detectors have also been installed and commissioned. In this paper, the commissioning of the improved MICE beamline and target will be discussed, including the use of Time-of-Flight detectors to understand the content of the MICE beam between 200 and 444 MeV/c.

 
WEPE080 Six-Dimensional Cooling Lattice Studies for the Muon Collider 3533
 
  • P. Snopok, G.G. Hanson
    UCR, Riverside, California
 
 

A significant reduction in the six-dimensional emittance of the initial beam is required in any proposed Muon Collider scheme. Two lattices based on the original RFOFO ring design representing different stages of cooling are considered. One is the so-called open cavity lattice addressing the problem of the 201.25 MHz RF cavities running in a magnetic field, the other one is the 805 MHz RF lattice that is used for smaller emittances. The details of the acceptance analysis and tracking studies of both channels are presented and compared to the independent ICOOL implementation.

 
WEPE081 Wedge Absorber Design for the Muon Ionisation Cooling Experiment 3536
 
  • P. Snopok, L. Coney
    UCR, Riverside, California
  • A. Jansson
    Fermilab, Batavia
  • C.T. Rogers
    STFC/RAL/ASTeC, Chilton, Didcot, Oxon
 
 

In the Muon Ionization Cooling Experiment (MICE), muons are cooled by ionization cooling. Muons are passed through material, reducing the total momentum of the beam. This results in a decrease in transverse emittance and a slight increase in longitudinal emittance, but overall reduction of 6D beam emittance. In emittance exchange, a dispersive beam is passed through wedge-shaped absorbers. Muons with higher energy pass through more material, resulting in a reduction in longitudinal and transverse emittance. Emittance exchange is a vital technology for a Muon Collider and may be of use for a Neutrino Factory. Two ways to demonstrate emittance exchange in the straight solenoidal lattice of MICE are discussed. One is to let a muon beam pass through a wedge shaped absorber; the input beam distribution must be carefully selected to accommodate chromatic aberrations in the solenoid lattice. Another approach is to use the input beam for MICE without beam selection. In this case no polynomial weighting is involved; however, a more sophisticated shape of the absorber is required to reduce longitudinal emittance.

 
WEPE084 Muon Acceleration with RLA and Non-scaling FFAG Arcs 3539
 
  • V.S. Morozov
    ODU, Norfolk, Virginia
  • S.A. Bogacz
    JLAB, Newport News, Virginia
  • D. Trbojevic
    BNL, Upton, Long Island, New York
 
 

Recirculating linear accelerators (RLA) are the most likely means to achieve the rapid acceleration of short-lived muons to multi-GeV energies required for Neutrino Factories and TeV energies required for Muon Colliders. In the work described here, a novel arc optics based on a Non Scaling Fixed Field Alternating Gradient (NS-FFAG) lattice is developed, which would provide sufficient momentum acceptance to allow multiple passes (two or more consecutive energies) to be transported in one string of magnets. We present a combination of the non-scaling NS-FFAG RLA placed in a straight section. Orbit offsets of different energy muons are kept small in the NS-FFAG arcs during multiple passes. The NS-FFAG, made of densely packed FODO cells, allows momentum acceptance of dp/p=±60%. This solution would reduce overall cost and simplify the operation. Difference in a muon path length for corresponding energies is corrected with a chicane. We will also discuss technical requirements to allow the maximum number of passes by using an adjustable path length to accurately control the returned beam phase to synchronize with the RF.

 
THXMH02 International Design Study of a Neutrino Factory 3597
 
  • J.S. Berg
    BNL, Upton, Long Island, New York
 
 

By providing an extremely intense source of neutrinos from the decays of muons in a storage ring, a Neutrino Factory will provide the opportunity for precision measurements and searches for new physics amongst neutrino interactions. An active international collaboration is addressing the many technical challenges that must be met before the design for a Neutrino Factory can be finalized. An overview of the accelerator complex and the current international R&D program will be presented, and the key technical issues will be discussed.

 

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THOAMH01 Recirculating Linear Accelerators for Future Muon Facilities 3602
 
  • S.A. Bogacz
    JLAB, Newport News, Virginia
  • K.B. Beard, R.P. Johnson
    Muons, Inc, Batavia
 
 

Neutrino Factories and Muon Colliders require rapid acceleration of short-lived muons to multi-GeV and TeV energies. A Recirculating Linear Accelerator (RLA) that uses superconducting RF structures can provide exceptionally fast and economical acceleration to the extent that the focusing range of the RLA quadrupoles allows each muon to pass several times through each high-gradient cavity. A new concept of rapidly changing the strength of the RLA focusing quadrupoles as the muons gain energy is being developed to increase the number of passes that each muon will make in the RF cavities, leading to greater cost effectiveness. We discuss the optics and technical requirements for RLA designs, using RF cavities capable of simultaneous acceleration of both μ+ and μ- species, with pulsed Linac quadrupoles and arc magnets to allow the maximum number of passes. The design will include the optics for the multi-pass linac and droplet-shaped return arcs.

 

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