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MOPEB008 Magnetic Field Measurement required for High Luminosity Accelerator dipole, luminosity, quadrupole, power-supply 292
 
  • K. Egawa, M. Masuzawa
    KEK, Ibaraki
 
 

The KEKB is a high luminosity accelerator which achieved the highest luminosity record of 2.1x1034. It requires the precise and stable beam control to keep its high luminosity continually. Slight change of the magnetic field may easily deteriorate the performance of the collisions of the very small and thin beams. The field measurement accuracy better than 10-4 has been already achieved. The resolution of the measurement has reached to a few 10-5. But it is known by the beam studies that the field change less than 10-4 may cause deterioration of the luminosity. The requirement on the stability of magnetic field will be stricter for future nano beam colliders. We have studied the effects of the following conditions on the magnetic field by using some KEKB magnets: changes of the magnetic field due to air or cooling water temperature, changes due to initialization conditions, field coupling between the adjacent magnets, effect of excitation of the adjacent magnet and behavior of the magnetic field under polarity change have been measured. These studies are not only useful for the existing KEKB but also important for future nano beam accelerators.

 
TUPEA030 Transmission of Reference RF Signals Through Optical Fiber at XFEL/SPring-8 klystron, laser, LLRF, resonance 1390
 
  • T. Ohshima, N. Hosoda, H. Maesaka, S. Matsubara, Y. Otake
    RIKEN/SPring-8, Hyogo
 
 

The pulse width of an X-ray laser at XFEL/SPring-8 is several tens femto-seconds, which requires reference rf signals to have the same time-stability. The reference signals with a low phase-noise oscillator are sent to instruments in 19" racks developed along an accelerator by an optical fiber system. The temperature drift of the fiber makes phase shifts of the reference signals. Therefore, the fiber is put in a thermal-insulated duct. By feeding temperature-controlled water (26.1 ± 0.1 deg. C) in a pipe attached to the duct, the fiber temperature was kept to be 26.2 ± 0.08 deg. C at the ambient temperature change of 29.1 ± 1.7 deg. C. From this temperature controllability, the phase shifts of the signals through a 400 m fiber of a thermal coefficient of 5 ps/km/K are 160 fs. Further reduction of the shifts is required and will be achieved by a fiber-length feedback control in a future plan. Vibration of the fiber also degrades the quality of the signals. The fiber is embedded on a vibration buffer material. A test to evaluate the effect of the vibration to the transmitted signal phase was carried out. The test result will be also shown in this paper.

 
TUPEB013 Strong-strong Simulation for Super B Factories simulation, luminosity, radiation, damping 1542
 
  • K. Ohmi
    KEK, Ibaraki
 
 

Super B factories are designed with very low emittance and very low beta function at the interaction point. The two beams collide with a large crossing angle, thus the overlap area of the beams is limited at a small part of their length. Simulation of the beam-beam effects is hard because of the longitudinal slice of the beam is the order of 100. We discuss two methods for the simulation. One is a simplified method, which is mixture of the particle in cell and Gaussian approximation. The other is fully strong-strong simulation using the particle in cell. The shifted Green function is used to calculate the beam-beam force for less overlap of the beam distribution. Luminosity and its degradation due to IP optics errors in Super B factories are discussed.

 
TUPEB015 Dynamic Aperture Limit caused by IR Nonlinearity in Extremely Low-beta B Factories dynamic-aperture, quadrupole, sextupole, interaction-region 1548
 
  • K. Ohmi, H. Koiso
    KEK, Ibaraki
 
 

Progress of Graphic Processor Unit (GPU) is marveled. The performance is 1TFlops per unit. Simulation of electron gun can be performed by particle-particle interactions, in which the calculation cost is NxN. Since the calculation of each interaction is very simple, GPU can demonstrate its ability. We show simulation results and discuss the possibilities to extend other simulations.

 
TUPEB017 Effects of Linear and Chromatic X-Y Couplings in the SuperKEKB coupling, luminosity, simulation, emittance 1551
 
  • D.M. Zhou, H. Koiso, A. Morita, K. Ohmi, Y. Ohnishi, Y. Seimiya
    KEK, Ibaraki
 
 

Using a weak-strong beam-beam code, in which the symplectic maps for the linear coupling and chromatic aberrations were implemented, the luminosity degradation caused by the linear and chromatic X-Y couplings at the interaction point (IP) were evaluated for the SuperKEKB project under design. The linear and chromatic X-Y couplings were estimated through modeling the machine errors using random seeds, based on a baseline design of the SuperKEKB rings. It was found that the linear and chromatic X-Y couplings can potentially degrade the luminosity performance.

 
TUPEC063 Particle Tracking in Matter-dominated Beam Lines simulation, space-charge, collider, polarization 1871
 
  • T.J. Roberts, K.B. Beard
    Muons, Inc, Batavia
  • S. Ahmed, D. Huang, D.M. Kaplan, L.K. Spentzouris
    Illinois Institute of Technology, Chicago, Illinois
 
 

The G4beamline program* is a useful and steadily improving tool to quickly and easily model beam lines and experimental equipment without user programming. It has both graphical and command-line user interfaces. Unlike most accelerator physics codes, it easily handles a wide range of materials and fields, being particularly well suited for the study of muon and neutrino facilities. As it is based on the Geant4 toolkit**, G4beamline includes most of what is known about the interactions of particles with matter. We are continuing the development of G4beamline to facilitate its use by a larger set of beam line and accelerator developers. A major new feature is the calculation of space-charge effects. G4beamline is open source and freely available at: http://g4beamline.muonsinc.com


* http://g4beamline.muonsinc.com
** http://geant4.cern.ch

 
TUPD081 Wake Fields in the Super B Factory Interaction Region interaction-region, wakefield, impedance, HOM 2105
 
  • S.P. Weathersby, A. Novokhatski
    SLAC, Menlo Park, California
 
 

The geometry of storage ring collider interaction regions present an impedance to beam fields resulting in the generation of additional electromagnetic fields (higher order modes or wake fields) which affect the beam energy and trajectory. These affects are computed for the Super B interaction region by evaluating longitudinal loss factors and averaged transverse kicks for short range wake fields. Results indicate at least a factor of 2 lower wake field power generation in comparison with the interaction region geometry of the PEP-II B-factory collider. Wake field reduction is a consideration in the Super B design. Transverse kicks are consistent with an attractive potential from the crotch nearest the beam trajectory. The longitudinal loss factor scales as the -2.5 power of the bunch length. A factor of 60 loss factor reduction is possible with crotch geometry based on an intersecting tubes model.

 
WEPEA034 Development and Operational Status of PF-Ring and PF-AR injection, power-supply, linac, undulator 2561
 
  • T. Honda, T. Aoto, S. Asaoka, K. Ebihara, K. Furukawa, K. Haga, K. Harada, Y. Honda, T. Ieiri, N. Iida, M. Izawa, T. Kageyama, M. Kikuchi, Y. Kobayashi, K. Marutsuka, A. Mishina, T. Miyajima, H. Miyauchi, S. Nagahashi, T.T. Nakamura, T. Nogami, T. Obina, K. Oide, M. Ono, T. Ozaki, C.O. Pak, H. Sakai, H. Sakai, Y. Sakamoto, S. Sakanaka, H. Sasaki, Y. Sato, K. Satoh, M. Shimada, T. Shioya, M. Tadano, T. Tahara, T. Takahashi, R. Takai, S. Takasaki, Y. Tanimoto, M. Tobiyama, K. Tsuchiya, T. Uchiyama, A. Ueda, K. Umemori, M. Yamamoto, Ma. Yoshida, S.I. Yoshimoto
    KEK, Ibaraki
 
 

KEK manages two synchrotron radiation sources, Photon Factory storage ring (PF-ring) of 2.5 GeV and Photon Factory advanced ring (PF-AR) of 6.5 GeV. These rings share an injector linac with the two main rings of KEK B-factory, 8-GeV HER and 3.5-GeV LER. Recently, the linac has succeeded in a pulse by pulse multi-energy acceleration. A top-up operation of PF-ring has been realized as the simultaneous continuous injection to the 3 rings, PF-ring, HER and LER. Development of new injection scheme using a pulsed sextupole magnet continues aiming at practical use in the top-up operation. A rapid-polarization-switching device consisting of tandem two APPLE-II type undulators has been developed at PF-ring. The first undulator was installed in 2008, and the second one will be installed in 2010 summer. PF-AR, operated in a single-bunch mode at all times, has been suffered from sudden lifetime drop phenomena attributed to dust trapping for many years. Using the movable electrodes installed for experiment, we confirmed that the discharge created by the electrode was followed by the dust trapping, and succeeded in a visual observation of luminous dust streaking in front of CCD cameras.

 
WEPEB034 Superb Bunch-by-bunch Feedback R&D feedback, controls, emittance, luminosity 2761
 
  • A. Drago, M.M. Beretta
    INFN/LNF, Frascati (Roma)
  • K.J. Bertsche, A. Novokhatski
    SLAC, Menlo Park, California
  • M. Migliorati
    Rome University La Sapienza, Roma
 
 

The SuperB project has the goal to build in the Frascati or Tor Vergata area, an asymmetric e+/e- Super Flavor Factory to achieve a peak luminosity > 1036 cm-2 s-1. The SuperB design is based on collisions with extremely low vertical emittance beams. A source of emittance growth comes from the bunch by bunch feedback systems producing high power correction signals to damp the beams. To limit any undesirable effect, a large R&D program is in progress, partially funded by the INFN Fifth National Scientific Committee through the SFEED (SuperB feedback) project approved within the 2010 budget. One of the first steps of the R&D program consists in the upgrade and test of new 12-bit feedback systems in the vertical plane of the DAΦNE main rings. The systems are the direct evolution of the previous 8-bit system design by a KEK/SLAC/LNF collaboration, yielding a good compatibility with the powerful diagnostics and analysis programs developed in the past. Studies on their effects in the longitudinal plane are also in progress.

 
WEPEC007 Surface Investigation on Prototype Cavities for the European XFEL cavity, niobium, accelerating-gradient, electron 2902
 
  • X. Singer, S. Aderhold, A. Ermakov, W. Singer, K. Twarowski
    DESY, Hamburg
  • M. Hoss, F. Schoelz, B. Spaniol
    W.C. Heraeus GmbH, Materials Technology Dept., Hanau
 
 

Performance of XFEL prototype cavities fabricated at the industry and treated at DESY demonstrates big scattering from 15 to 41 MV/m. Most cavities satisfy the XFEL specification. Few cavities with low performance (15-17 MV/m) are limited by thermal break down without field emission. The T-map analysis detected the quench areas mainly close to the equator. Optical control by high resolution camera has been applied and allowed to monitor the defects in some cases with good correlation to T-map data. In order to understand the cause of reduced performance and get more detailed information of defects origin some samples have been extracted from two cavities and investigated by light microscope, 3D- microscope, SEM, EDX and Auger spectroscopy. Several surface flaws with sizes from few μm to hundreds of μm were detected by microscopy. The defects can be separated in two categories. The first category of defects indicates foreign elements (often increased content of carbon). Inclusions with increased content of carbon adhered on the surface and presumably have a hydrocarbon nature. Deviation from smooth surface profile characterizes the second type of defects (holes, bumps and pits).

 
WEPD027 Tuning of the Fast Local Bump System for Helicity Switching at the Photon Factory kicker, controls, photon, undulator 3150
 
  • K. Harada, Y. Kobayashi, T. Miyajima, S. Nagahashi, T. Obina, M. Shimada, R. Takai
    KEK, Ibaraki
  • S. Matsuba
    Hiroshima University, Graduate School of Science, Higashi-Hiroshima
 
 

The fast local bump system for the helicity switching of variably polarizing undulators has been developed at the Photon Factory ring. The system consists of two APPLE-II type variably polarizing undulators and five identical horizontal kicker magnets for local bump with four small corrector magnets to prevent the leakage of the bump. At present, one undulator and the local bump system with corrector magnets are installed. For beam test, the system was operated with frequency up to 50 Hz with feed forward correction. In this presentation, after brief description of the system configuration, the results of the test operation and fine tunings of the fast local bump system are shown.

 
WEPD028 Magnetic Field Adjustment of a Polarizing Undulator (U#16-2) at the Photon Factory polarization, undulator, photon, simulation 3153
 
  • K. Tsuchiya, T. Aoto
    KEK, Ibaraki
 
 

We have been developing a rapid-polarization-switching source at the B15-16 straight section in the PF 2.5GeV ring. The source consists of tandem two APPLE-II type elliptically polarizing undulators (EPU), namely U#16-1 and U#16-2, and a fast kicker system. These two undulators are designed to obtain the soft x-ray at the energy region from 200eV to 1keV with various polarization states. We have constructed U#16-1 and installed in the PF ring in March 2008. The operation of U#16-1 for the user experiments has been started successfully since April 2008. The construction of the second undulator U#16-2 is underway. U#16-2 will be installed in the PF ring at this summer. We report the result of the magnetic field adjustment of the U#16-2.

 
WEPE042 Mice Status solenoid, emittance, target, collider 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.

 
WEPE047 Frictional Cooling for a Slow Muon Source dipole, quadrupole, simulation, proton 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.

 
WEPE051 Muon Cooling Performance in Various Neutrino Factory Cooling Cell Configurations using G4MICE lattice, cavity, emittance, betatron 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.

 
WEPE053 Muon Polarimeter in a Neutrino Factory Decay Ring polarization, electron, dipole, monitoring 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.

 
WEPE060 Investigation of Beam Loading Effects for the Neutrino Factory Muon Accelerator beam-loading, cavity, linac, simulation 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 emittance, lattice, optics, solenoid 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.

 
WEPE065 The US Muon Accelerator Program collider, simulation, cavity, target 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.

 
WEPE074 A Possible Hybrid Cooling Channel for a Neutrino Factory cavity, vacuum, emittance, proton 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.

 
WEPE078 The MERIT High-Power Target Experiment at the CERN PS proton, target, solenoid, collider 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.

 
WEPE098 Optimising Pion Production Target Shapes for the Neutrino Factory target, proton, simulation 3581
 
  • S.J. Brooks
    STFC/RAL/ASTeC, Chilton, Didcot, Oxon
 
 

The neutrino factory requires a source of pions within a momentum window determined by the ‘muon front end' accelerator structure downstream. The technique of finding which parts of a large target block are net absorbers or emitters of particles may be adapted with this momentum window in mind. Therefore, analysis of a hadronic production simulation run using MARS15 can provide a candidate target shape in a single pass. However, changing the shape of the material also affects the absorption/emission balance, so this paper investigates iterative schemes to find a self-consistent optimal, or near-optimal, target geometry.

 
WEPE101 A 4-MW Target Station for a Muon Collider or Neutrino Factory target, proton, collider, solenoid 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 Brok, 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.

 
THXMH02 International Design Study of a Neutrino Factory cavity, target, proton, storage-ring 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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THYRA01 Beam-beam Interaction in Novel, Very High Luminosity Parameter Regimes luminosity, sextupole, simulation, collider 3639
 
  • M. Zobov
    INFN/LNF, Frascati (Roma)
 
 

To achieve luminosities significantly higher than in existing machines, future storage-ring based colliders will need to operate in novel parameter regimes combining ultra-low emittance, large Piwinski angle and high bunch charge; implementation of techniques such as a "crab waist" will add further challenges. Understanding the beam-beam interaction in these situations will be essential for the design of future very high luminosity colliders. Recent developments in modeling tools for studying beam-beam effects, capable of investigating the relevant regimes, will be discussed and examples, including tests with crab waist collisions in DAΦNE, will be presented.

 

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THPEA047 Dielectric Loaded RF Cavities for Muon Facilities cavity, vacuum, simulation, collider 3783
 
  • M. Popovic, A. Moretti
    Fermilab, Batavia
  • C.M. Ankenbrandt, M.A.C. Cummings, R.P. Johnson, M.L. Neubauer
    Muons, Inc, Batavia
 
 

Alternative RF cavity fabrication techniques for accelerator applications at low frequencies are needed to improve manufacturability, reliability and cost. RF cavities below 800 MHz are large, take a lot of transverse space, increase the cost of installation, are difficult to manufacture, require significant lead times, and are expensive. Novel RF cavities partially loaded with a ceramic for accelerator applications will allow smaller diameter cavities to be designed and built. The manufacturing techniques for partially loaded cavities will be explored. A new 200MHz cavity will be built for the Fermilab Proton Source to improve the longitudinal emittance and energy stability of the linac beam at injection to the Booster. A cavity designed for 400 MHz with a ceramic cylinder will be tested at low power at cryogenic temperatures to test the change in Qo due to the alumina ceramic. Techniques will be explored to determine if it is feasible to change the cavity frequency by replacing an annular ceramic insert without adversely effecting high power cavity performance.

 
THPEA049 Normal Conducting RF Cavity for MICE cavity, emittance, vacuum, coupling 3786
 
  • D. Li, A.J. DeMello, S.P. Virostek, M.S. Zisman
    LBNL, Berkeley, California
 
 

Normal conducting RF cavities must be used for the cooling section of international Muon Ionization Cooling Experiment (MICE) which is currently under construction at Rutherford Appleton Laboratory (RAL) in UK. Eight 201-MHz cavities are needed for the MICE cooling section; fabrication of the first five cavities is nearly complete. This paper reports the cavity fabrication status that includes the cavity design, fabrication techniques and preliminary low power RF measurements of the first five cavities.

 
THPEC089 Overview of Solid Target Studies for a Neutrino Factory target, laser, proton, simulation 4263
 
  • T.R. Edgecock
    STFC/RAL, Chilton, Didcot, Oxon
  • J.J. Back
    University of Warwick, Coventry
  • J.R.J. Bennett
    STFC/RAL/ISIS, Chilton, Didcot, Oxon
  • C.N. Booth, G.P. Skoro
    Sheffield University, Sheffield
  • S.J. Brooks
    STFC/RAL/ASTeC, Chilton, Didcot, Oxon
 
 

The UK programme of high power target developments for a Neutrino Factory is centred on the study of high-Z materials (tungsten, tantalum). A description of lifetime shock tests on candidate materials is given as part of the research into a solid target solution. A fast high current pulse is applied to a thin wire of the sample material and the lifetime measured from the number of pulses before failure. These measurements are made at temperatures up to ~2000 K. The stress on the wire is calculated using the LS-DYNA code and compared to the stress expected in the real Neutrino Factory target. It has been found that tantalum is too weak to sustain prolonged stress at these temperatures but a tungsten wire has reached over 26 million pulses (equivalent to more than ten years of operation at the Neutrino Factory). An account is given of the optimisation of secondary pion production from the target and the issues related to mounting the target in the muon capture solenoid and target station are discussed.

 
THPEC091 Tungsten Behavior at High Temperature and High Stress target, laser, simulation, site 4269
 
  • G.P. Skoro, C.N. Booth
    Sheffield University, Sheffield
  • J.J. Back
    University of Warwick, Coventry
  • J.R.J. Bennett, S.A. Gray, A.J. McFarland
    STFC/RAL/ISIS, Chilton, Didcot, Oxon
  • T.R. Edgecock
    STFC/RAL, Chilton, Didcot, Oxon
 
 

Recently reported results on the tungsten lifetime/fatigue tests under conditions expected in the Neutrino Factory target have strengthened the case of solid target option for a Neutrino Factory. This paper gives description of the detailed measurements of the tungsten properties at high temperature and high stress. We have performed extensive set of measurements of the surface displacement and velocity of the tungsten wires that were stressed by passing a fast, high current pulse through a thin sample. Radial and longitudinal oscillations of the wire were measured by a Laser Doppler Vibrometer. The wire was operated at temperatures of 300-2500 K by adjusting the pulse repetition rate. In doing so we have tried to simulate the conditions (high stress and temperature) expected at the Neutrino Factory. Most important result of this study is an experimental confirmation that strength of tungsten remains high at high temperature and high stress. The experimental results have been found to agree very well with LS-DYNA modelling results.

 
THPEC092 A Pion Production and Capture System for a 4MW Target Station proton, target, shielding, simulation 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.

 
THPD059 The Status of Turkish Accelerator Center Project FEL, electron, linac, synchrotron 4419
 
  • S. Ozkorucuklu
    SDU, Isparta
  • A. Aksoy, B. Ketenoğlu, O. Yavas
    Ankara University, Faculty of Engineering, Tandogan, Ankara
  • P. Arikan
    Gazi University, Faculty of Arts and Sciences, Teknikokullar, Ankara
  • O. Cakir, A.K. Çiftçi, R. Çiftçi, K. Zengin
    Ankara University, Faculty of Sciences, Tandogan/Ankara
  • H. Duran Yildiz
    Dumlupinar University, Faculty of Science and Arts, Kutahya
 
 

The status and road map of Turkish Accelerator Center (TAC) project is explained. TAC project is in third phase after feasibility and conceptual design phases with support of State Planning Organisation (SPO) of Turkey that the main aim of this phase is to complete of technical design report of TAC and to establish the first (test) facility. The first facility is planned as superconducting electron linac based IR FEL and bremsstrahlung facility. Third phase will be completed in 2013. It is planned that TAC will include a linac on ring type electron positron collider as a super charm factory, third and fourth generation light sources (SR and SASE FEL) and a proton facility. TAC collaboration is an inter-university collaboration of ten Turkish Universities under the coordination of Ankara University and TAC is a national project with international collaboration. In this study, the status of the project and the road map is explained with some results from design and construction studies.

 
THPD074 Using Project X as a Proton Driver for Muon Colliders and Neutrino Factories proton, collider, linac, target 4452
 
  • G. Flanagan, R.J. Abrams, C.M. Ankenbrandt, M.A.C. Cummings, R.P. Johnson
    Muons, Inc, Batavia
  • M. Popovic
    Fermilab, Batavia
 
 

The designs of accelerator systems that will be needed to transform Fermilab's Project X into a high-power proton driver for a muon collider and/or a neutrino factory are discussed. These applications require several megawatts of beam power delivered in tens or hundreds of short multi-GeV bunches per second, respectively. Project X may require a linac extension to higher energy for this purpose. Other major subsystems that are likely to be needed include storage rings to accumulate and shorten the proton bunches and an external beam combiner to deliver multiple bunches simultaneously to the pion production target.

 
THPD093 New Approaches to Muon Acceleration with Zero-chromatic FFAGS acceleration, cavity, emittance, lattice 4506
 
  • T. Planche, Y. Ishi, Y. Kuriyama, J.-B. Lagrange, Y. Mori, K. Okabe, T. Uesugi, E. Yamakawa
    KURRI, Osaka
 
 

The acceleration of intense muon beams up to 25 GeV is the challenge of the international design work for a future neutrino factory. The present baseline scenario for muon acceleration is based on linacs, recirculating linear accelerators (RLAs) and non-scaling fixed field alternating gradient (FFAG) rings. However RLAs are one of the most cost driving part. Two new approaches to use zero-chromatic FFAG instead of RLA have been proposed. Detailed lattices parameters and 6D tracking results are presented.

 
THPE033 Beam Dynamics Studies for the First Muon Linac of the Neutrino Factory linac, solenoid, cavity, acceleration 4590
 
  • C. Bontoiu, M. Aslaninejad, J.K. Pozimski
    Imperial College of Science and Technology, Department of Physics, London
  • S.A. Bogacz
    JLAB, Newport News, Virginia
 
 

Within the Neutrino Factory Project the muon acceleration process involves a complex chain of accelerators including a (single-pass) linac, two recirculating linacs and an FFAG. The linac consists of RF cavities and iron shielded solenoids for transverse focusing and has been previously designed relying on idealized field models. However, to predict accurately the transport and acceleration of a high emittance 30 cm wide beam with 10 % energy spread requires detailed knowledge of fringe field distributions. This article presents results of the front-to-end tracking of the muon beam through numerically simulated realistic field distributions for the shielded solenoids and the RF fields. Real and phase space evolution of the beam has been studied along the linac and the results will be presented and discussed.

 
THPE075 Application of Frequency Map Analysis to Beam-Beam Effects Study in Crab Waist Collision Scheme resonance, betatron, luminosity, simulation 4692
 
  • E.A. Simonov, E.B. Levichev, D.N. Shatilov
    BINP SB RAS, Novosibirsk
 
 

We applied Frequency Map Analysis (FMA) - a method that is widely used to explore dynamics of Hamiltonian systems - to beam-beam effects study. The method turned out to be rather informative and illustrative in case of a novel Crab Waist collision approach, when "crab" focusing of colliding beams results in significant suppression of betatron coupling resonances. Application of FMA provides visible information about all the working resonances, their widths and locations in the planes of betatron tunes and betatron amplitudes, so the process of resonances suppression due to the beams crabbing is clearly seen.

 
FRXBMH01 Next Generation B-factories luminosity, emittance, electron, solenoid 4764
 
  • M. Masuzawa
    KEK, Ibaraki
 
 

The KEKB and PEP-II B factories have achieved world record luminosities while doubling or tripling their original design luminosities. The demand now from the physics community is for Super B Factories with orders of magnitude higher luminosities than those achieved by the present generation of machines. This talk will discuss the next-generation B factories, which aim to push back the luminosity frontier in the search for physics beyond the Standard Model.

 

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