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lattice

Paper Title Other Keywords Page
MO3RAC04 Super-B Project Overview simulation, sextupole, luminosity, emittance 38
 
  • M.E. Biagini, R. Boni, M. Boscolo, T. Demma, A. Drago, S. Guiducci, P. Raimondi, S. Tomassini, M. Zobov
    INFN/LNF, Frascati (Roma)
  • K.J. Bertsche, M.H. Donald, Y. Nosochkov, A. Novokhatski, J. Seeman, M.K. Sullivan, U. Wienands, W. Wittmer, G. Yocky
    SLAC, Menlo Park, California
  • S. Bettoni, D. Quatraro
    CERN, Geneva
  • I. Koop, E.B. Levichev, S.A. Nikitin, P.A. Piminov, D.N. Shatilov
    BINP SB RAS, Novosibirsk
  • K. Ohmi
    KEK, Ibaraki
  • E. Paoloni
    University of Pisa and INFN, Pisa
 
 

The SuperB project aims at the construction of an asymmetric (4x7 GeV), very high luminosity, B-Factory on the Roma II (Italy) University campus. The luminosity goal of 1036 cm-2 s-1 can be reached with a new collision scheme with large Piwinski angle and the use of “crab” sextupoles. A crab-waist IR has been successfully tested at the DAPHNE Phi-Factory at LNF-Frascati (Italy) in 2008. The crab waist together with very low beta* will allow for operation with relatively low beam currents and reasonable bunch length, comparable to those of PEP-II and KEKB. In the High Energy Ring, two spin rotators permit bringing longitudinally polarized beams into collision at the IP. The lattice has been designed with a very low intrinsic emittance and is quite compact, less than 2 km long. The tight focusing requires a sophisticated Interaction Region with quadrupoles very close to the IP. A Conceptual Design Report was published in March 2007, and beam dynamics and collective effects R&D studies are in progress in order to publish a Technical Design Report by the end of 2010. A status of the design and simulations is presented in this paper.

 

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MO6PFP003 Specifications and R&D Program on Magnet Alignment Tolerances for NSLS-II alignment, quadrupole, closed-orbit, emittance 130
 
  • S.L. Kramer, A.K. Jain
    BNL, Upton, Long Island, New York
 
 

Funding: Work supported by U.S. DOE, Contract No.DE-AC02-98CH10886


The NSLS-II light source is a proposed 3 GeV storage ring, with the potential for ultra-low emittance*. Despite the reduced emittance goal for the bare lattice, the closed orbit amplification factors are on average >50 in both planes, for random quadrupole alignment errors. The high chromaticity will also require strong sextupoles and the low 3 GeV energy will require large dynamic and momentum aperture to insure adequate lifetime. This will require tight alignment tolerances (~30microns) on the multipole magnets during installation. By specifying tight alignment tolerances of the magnets on the support girders, the random alignment tolerances of the girders in the tunnel can be significantly relaxed. Using beam based alignment to find the golden orbit through the quadrupole centers, the closed orbit offsets in the multipole magnets will then be reduced to essentially the alignment errors of the magnets, restoring much of the DA and lifetime of the bare lattice. Our R&D program to achieve these tight alignment tolerances of the magnets on the girders using a vibrating wire technique**, will be discussed and initial results presented.


*Work presented on behalf of the NSLS-II Design Team, CDR(2006) and CD2(2007).
**A. Jain, et al, International Workshop on Accelerator Alignment, Tsukuba, Japan, Feb.11-15, 2008.

 
MO6PFP008 The Design and Construction of NSLS-II Magnets multipole, quadrupole, sextupole, dipole 145
 
  • J. Skaritka, J. Bengtsson, G. Danby, G. Ganetis, W. Guo, R.C. Gupta, J.W. Jackson, A.K. Jain, S.L. Kramer, S. Krinsky, Y. Li, W. Meng, B. Nash, S. Ozaki, M. Rehak, S. Sharma, C.J. Spataro, F.J. Willeke
    BNL, Upton, Long Island, New York
 
 

Funding: US DOE Office of Basic Energy Sciences


NSLS-II is a new state-of-the-art medium energy synchrotron light source designed to deliver world leading brightness and flux with top-off operation for constant output. Design and engineering of NSLS-II began in 2005 and the beginning of construction and operations are expected to start in 2009 and 2015, respectively. The energy of the machine is 3Gev and the circumference 792 m. The chosen lattice requires tight on magnetic field tolerances for the ring magnets. These magnets have been designed with 3D Opera software. The required multipole field quality and alignment preclude the use of multifunctional sextupoles, leading to discrete corrector magnets in the storage ring. The corrector magnets are multifunctional and will provide horizontal and vertical steering as well as skew quadrupole. This paper describes the dipoles, quadrupoles, sextupoles, and corrector magnets design and prototyping status of the NSLS-II.

 
MO6PFP016 Magnetic-Field Calculations for the Magnets of the High-Energy Storage Ring (HESR) at FAIR dipole, sextupole, quadrupole, multipole 166
 
  • H. Soltner, U. Bechstedt, R. Tölle
    FZJ, Jülich
  • J.G. De Villiers
    iThemba LABS, Somerset West
 
 

Funding: Work supported by BMBF and NRF, Project code SUA 06/003


Forschungszentrum Jülich has taken the leadership of a consortium responsible for the design, installation and commissioning of the High-Energy Storage Ring (HESR) for antiprotons as part of the FAIR project at GSI in Darmstadt, Germany. Since a normal-conducting design of the ring has now been favored over the previously envisioned superconducting option, new calculations have been performed in order to assess the magnetic field characteristics of the normal-conducting dipole, quadrupole, and sextupole magnets of the HESR. This paper presents the physical features of the magnets and the results of the 3D calculations with emphasis on the various multipole contributions at the ends of the magnets.

 
MO6PFP032 Magnet System for PLS-II Project quadrupole, sextupole, dipole, septum 208
 
  • D.E. Kim, H.S. Han, H.-G. Lee, K.-H. Park, H.S. Suh, Y.G. Young-Gyu
    PAL, Pohang, Kyungbuk
 
 

Funding: Supported by the MOEST of Korea and by POSCO


Pohang Accelerator Laboratory (PAL) is planning to upgrade the Pohang Light Source (PLS) which is a 3rd generation light source operating since 1995. The key features of the upgrade are, decrease of the beam emittance to 5.6 nm, increasing the beam energy to 3.0 GeV, additional shorter straight sections for more insertion devices. Because the PLSII should use practically same circumference preserving the shielding wall structure of the existing PLS, the lattice space is squeezed to the limit to secure the additional space for the insertion devices. This requirements forces heavy use of the combined function magnet. All dipoles are replaced to gradient magnet, and all sextupoles have horizontal corrector winding, vertical corrector winding, skew quadrupole windings. In this report, the design features and engineering efforts for the PLSII magnet systems are reported.

 
TU1RAI02 Non-Scaling FFAG Magnet Challenges quadrupole, injection, septum, extraction 619
 
  • N. Marks
    STFC/DL/ASTeC, Daresbury, Warrington, Cheshire
 
 

The latest initiatives to design and build non-scaling FFAGs have encountered novel technical challenges; the required DC combined function magnets (normal and superconducting) and fast pulsed magnets for injection and extraction present new problems. The talk will report on progress in meeting these challenges for the non-scaling machines, EMMA and PAMELA and will provide details of their current design status. With the main EMMA ring magnets now being delivered and the injection and extraction magnets being assembled in-house, practical engineering features of these systems will be presented.

 

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TU1GRI03 Muon Collider Progress collider, emittance, cavity, solenoid 652
 
  • R. B. Palmer
    BNL, Upton, Long Island, New York
 
 

In the past few years, there have been a number of advances in the design and supporting R&D for a machine to cool, accelerate and collide TeV muon beams. This talk will review progress and discuss how such a machine might evolve from programs to build high intensity proton sources and neutrino factories.

 

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TU1GRC04 FFAG Designs for the International Design Study for the Neutrino Factory cavity, dynamic-aperture, extraction, injection 657
 
  • J.S. Berg
    BNL, Upton, Long Island, New York
  • S. Machida
    STFC/RAL/ASTeC, Chilton, Didcot, Oxon
 
 

Funding: Work Supported by the United States Department of Energy, Contract No. DE-AC02-98CH10886.


The International Design Study for the Neutrino Factory (IDS-NF) aims to produce a design report for a neutrino factory. One component of that design is a linear non-scaling fixed-field alternating gradient accelerator (FFAG) that will accelerate to the final energy of 25~GeV. An FFAG is used to reduce the machine cost by maximizing the number of passes made through the RF cavities. We present some design options for this FFAG, individually optimized for cost. We study the addition of nonlinear magnets to the lattice to improve the performance of the lattice and consider the negative effects of doing so.

 

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TU2PBC02 Recent Improvements to CHEF, a Framework for Accelerator Computations linac, wakefield, emittance, space-charge 674
 
  • J.-F. Ostiguy, L. Michelotti
    Fermilab, Batavia
 
 

Funding: Work supported by US DOE under Contract No. DE-AC02-07CH11359


CHEF is body of software dedicated to accelerator beam dynamics and optics computations. It consists in a hierarchical set of libraries and a standalone application based on the latter. The code makes extensive use of templates and modern idioms such as smart pointers and generalized function objects. CHEF has been described in contributions at past conferences. In this paper, we document and discuss the implementation of recent improvements including:

  1. use of embedded SQL database technology to store, organize and retrieve lattice function data,
  2. a general approach to "knobs" based on generalized function objects,
  3. an improved architecture to support runtime plug-in propagation physics,
  4. a basic space-charge kick element,
  5. a facility to record particle loss on aperture boundaries and
  6. support for the MADX input format.

 

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TU2PBC03 Theory and Applications of Lattice with Negative Momentum Compaction Factor synchrotron, sextupole, quadrupole, dynamic-aperture 677
 
  • Y. Senichev
    FZJ, Jülich
 
 

A possible solution to avoid the transition energy crossing is the lattice with a negative momentum compaction factor. The developed lattice is based on the resonantly correlated curvature and gradient modulations in arcs with integer tunes in horizontal or both planes, and it called the “resonant” lattice*. This method was adopted for the TRIUMF and Moscow Kaon Factories. It was then applied in the SSC Low Energy Booster, the CERN Neutrino Factory, and in the Main Ring of the Japan Proton Accelerator Research Complex facility. For the superconducting option of High Energy Storage Ring lattice of the FAIR project, the same idea was also accepted, and at last it is one of the candidates for PS2 in CERN as well. Due to special features the idea of “resonant” lattice can be applied for the lattice with the stochastic cooling where the different arcs have the different mixing factors with conservation of the dynamic aperture for whole machine. The “resonant” lattice is appeared to be useful for electron machines where the minimum momentum-compaction factor and the minimum modulation of the dispersion function are both required simultaneously to have a small horizontal emittance.


*Yu. Senichev and A. Chechenin, Journal of Experimental and Theoretical Physics, 2007, v. {10}5, No. 6, p. 1141

 

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TU5RFP001 A Study of Lattice Structure and Insertion Devices at the Positron Ring of the TAC Project radiation, storage-ring, brilliance, positron 1081
 
  • K. Zengin, A.K. Çiftçi, R. Çiftçi
    Ankara University, Faculty of Sciences, Tandogan/Ankara
 
 

The Turkish Accelerator Complex (TAC) is a project for accelerator based fundamental and applied researches supported by Turkish State Planning Organization (DPT). The proposed complex is consisted of 1 GeV electron linac and 3.56 GeV positron ring for a charm factory and a few GeV proton linac. Apart from the particle factory, it is also planned to produce synchrotron radiation from positron ring. In this study the lattice structure design of the positron storage ring is made to produce the third generation synchrotron light. The parameters of complementary undulators and wigglers are determined. It is shown that the insertion devices with the proposed parameter sets produce maximal spectral brightness to cover 10 eV - 100 keV photon energy range.

 
TU5RFP007 NSLS-II Booster Acceptance Studies booster, injection, simulation, kicker 1099
 
  • R.P. Fliller, W. Guo, R. Heese, Y. Li, T.V. Shaftan
    BNL, Upton, Long Island, New York
 
 

The NSLS II is a state of the art 3 GeV synchrotron light source being developed at BNL. The injection system will consist of a 200 MeV linac and a 3GeV booster synchrotron. The injection system must supply 7.3nC every minute to satisfy the top off requirements. A large booster acceptance is neccessary to have a high booster injection efficiency and alleviate the requirements on linac gun. We also anticipate transverse stacking of bunches in the booster to increase the amount of charge that can be delivered. We present studies of the anticipated booster stay clear including lattice errors and the ramifications for injection efficiency and transverse stacking.

 
TU5RFP008 NSLS-II Lattice Optimization with Damping Wigglers sextupole, quadrupole, dynamic-aperture, damping 1102
 
  • W. Guo, S.L. Kramer, S. Krinsky, Y. Li, B. Nash, T. Tanabe
    BNL, Upton, Long Island, New York
 
 

Funding: NSLS-II, Brookhaven National Laboratory


NSLS-II, the third-generation light source which will be built at BNL is designed and optimized for 3 GeV energy, ultra-small emittance and high intensity of 500 mA. It will provide very bright synchrotron radiation over a large spectral range from IR to hard X-rays. Damping wigglers (DWs) are deployed to reduce the emittance of 2 nm by factors of 2-4, as well as for intense radiation sources for users. The linear and nonlinear effects induced by the DWs are integrated into the lattice design. In this paper, we discuss the linear and nonlinear optimization with DWs, and present a solution satisfying the injection and lifetime requirements. Our approach could be applied to the other light sources with strong insertion devices.

 
TU5RFP010 Flexibility in the Design of the NSLS-II Lattice emittance, quadrupole, sextupole, dipole 1108
 
  • S.L. Kramer, W. Guo
    BNL, Upton, Long Island, New York
 
 

Funding: Work supported by U.S. DOE, Contract No.DE-AC02-98CH10886


The NSLS-II light source is a proposed 3 GeV storage ring, with the potential for ultra-low emittance*. The lattice design uses a 30 cell DBA structure with a periodicity of 15, for alternating long and short straight sections. All cells are tuned achromatic to maximize the emittance reduction achieved as damping wigglers are added to the ring. Recent optimization of the lattice consisted of increasing the number of possible hard X-ray beam ports using three pole wigglers, reducing the number of magnets (quadrupoles and sextupoles) and shifting the magnets to allow easier extraction of the photon beams. The impact of the reduction of magnets on the lattice flexibility will be presented in terms of the tuning range possible for the lattice parameters: tune, emittance, and chromaticity, beta function matching to user insertion devices (IDs) and for compensating for ID induced distortions to these parameters. This flexibility is important for optimizing the lattice linear and nonlinear properties, the dynamic aperture, and its impact on beam lifetime, as well as matching the user source requirements and for value engineering of magnets and power supplies.


*Work presented on behalf of the NSLS-II Design Team, CDR(2006), CD2(2007) and CD3(2008).

 
TU5RFP013 Dynamic Response and Filtering Effects of a Light Source Accelerator Ring Structure site, ground-motion, simulation, storage-ring 1117
 
  • N. Simos, M. Fallier
    BNL, Upton, Long Island, New York
 
 

Vibration stability in third generation light sources such as the 3 GeV NSLS II under construction at BNL and which are aiming at high brightness and extremely small photon beam sizes is paramount. Movement of the magnetic elements of the accelerator lattice, and in particular when uncorrelated, will induce jitter in the beam and degrade the machine performance. The accelerator lattice response is coupled with the ring structure which in turn interacts with the site and the ground vibration field that characterizes it. Therefore, understanding this dynamic coupling between the accelerator ring structure and the site and the “filtering” effect of the interaction on both the amplitude and the spectral characteristics of the ground vibration is central towards establishing the response of the lattice. In this study, the site-ring dynamic interaction is evaluated based on the NSLS II design and site conditions using a state-of-the-art 3-D wave propagation and scattering analysis model. The study is augmented with an extensive array of measurements at the selected site as well as field studies at similar operating light source facilities.

 
TU5RFP015 Model for Addressing NSLS II Lattice Response to Random, Stationary Vibration site, ground-motion, photon, simulation 1123
 
  • N. Simos
    BNL, Upton, Long Island, New York
 
 

The extremely small photon beam dimensions of NSLS II impose challenging requirements on the e-beam orbital stability in the 6-D phase space. The electron beam orbit at the photon source locations must remain within a few hundred nanometer window for a wide frequency band. The beam orbit movement is coupled to the movement of the magnetic elements in the lattice which are itself coupled to the ring-building structure. While the vibration exciting the ring structure consists of deterministic and stochastic noise, it is the high frequency random, uncorrelated part that has the largest impact on the residual beam orbit movement as it is most difficult to control by fast orbit feedback. In this study, an analytical model is employed to quantify lattice displacement and beam orbit jitter for the expected conditions of NSLS II. The dynamic interaction of the ring supporting the lattice with the stationary ground vibration is addressed using a 3-D model of wave-structure interaction. Cross transfer functions linking ground vibration with the ring and magnetic lattice for various stochastic parameters are deduced leading to a multi-degree of freedom cross-spectral density of the lattice.

 
TU5RFP019 Design and Optimization of the BEPCII Synchrotron Radiation Mode emittance, wiggler, dynamic-aperture, sextupole 1132
 
  • Q. Qin, L.M. Chen, Y. Jiao, D. Wang, J.Q. Wang, X.H. Wang, Y. Wei, X.M. Wen, J. Xing, G. Xu, C.H. Yu, C. Zhang, Y. Zhang
    IHEP Beijing, Beijing
 
 

Funding: Work supported by National Natural Science Foundation of China contract 10725525


The upgraded project of the Beijing Electron-Positron Collider (BEPCII) can be operated not only for high energy physics experiments as a charm factory, but for synchrotron radiation users as a first generation light source. The design of the synchrotron radiation (SR) mode of the BEPCII storage ring keeps all the original beam lines of the BEPC. The lattice based on the layout of the collider can meet all the requirements of the SR users, and the emittance is minimized. Optimization of the SR mode focuses on reducing the effects from wigglers around the ring. Some results from the operations of the SR mode are also given.

 
TU5RFP044 An Optic with Small Vertical Beta Function for the CAMD Light Source injection, quadrupole, wiggler, resonance 1189
 
  • V.P. Suller, P. Jines, D.J. Launey, T.A. Miller, Y. Wang
    LSU/CAMD, Baton Rouge, Louisiana
  • S. Wang
    CAEP/IFP, Mainyang, Sichuan
 
 

At the CAMD Light Source a new optic has been developed for the lattice having small vertical beta function in each of the 4 long straight sections. This optic will be necessary to operate the multipole wigglers with small vertical aperture which are planned to be installed in the near future. Results are presented of the tests which have been made with this optic, particularly in the critical area of injection, which is made low energy. The lattice functions have been characterized using LOCO software and the reduced vertical aperture confirmed with an adjustable scraper.

 
TU5RFP058 3D CAD Collaboration at European XFEL and ILC linac, positron, civil-engineering, survey 1214
 
  • L. Hagge, N. Bergel, A. Herz, J. Kreutzkamp, S. Sühl, N. Welle
    DESY, Hamburg
 
 

In most sub-systems of the European XFEL, more than one institute participates in the design & development activities. This is the case for e.g. the cold linac, cryogenics, bunch compressors, undulators and photon beam systems. To ensure interface compatibility and make sure components fit into their complex environments, the collaborating institutes have to create high-level 3D models of their sub-systems. These 3D models are centrally integrated into a master model, which enables identification and elimination of collisions and non-conformities prior to manufacturing. A "collaborative design process", which supports efficient, interactive and inter-disciplinary cooperation of different institutes, has been successfully developed and established at the European XFEL. It consists of design guidelines and processes definitions for information & data exchange, reviews, approvals and change management. The process is supported by the DESY Engineering Data Management System, DESY EDMS, and allows the combination of 3D models from multiple 3D CAD systems. Following the good experience at the European XFEL, the same process is now established at the Global Design Effort for the ILC.

 
TU5RFP079 ERL Staging linac, emittance, brightness, SRF 1272
 
  • K.C. Harkay, Y.-C. Chae
    ANL, Argonne
 
 

Funding: Work supported by U. S. Department of Energy, Office of Science, Office of Basic Energy Sciences, under Contract No. DE-AC02-06CH11357.


ERL staging is a novel concept that provides a practical path to upgrading an existing synchrotron light source while minimizing disruption to the users and managing the technical risk. In the very first stage, the accelerator operating parameters are comparable to CEBAF without recirculation. Therefore, initially, energy recovery is not required and the injector is more modest. Consequently, the technical risk is significantly reduced relative to the full ERL. Using the APS as an example, the first stage is based on a full-energy, 7-GeV superconducting radiofrequency (srf) linac and an electron source that is almost off-the-shelf. The linac would initially deliver a low average current beam (<200 uA), but with a geometric emittance that is much smaller than the storage ring, the x-ray brightness can exceed the APS. Furthermore, the spatial coherence fraction would be about 100 times higher and the pulse length up to 100 times smaller than the APS. Valuable srf operating experience is attained at an early stage while allowing critical energy recovery issues to be studied. Energy recovery is commissioned in stage 2. The optics design and performance at each stage will be presented.

 
TU6PFP024 Swift Heavy Ion Induced Modifications at Mo/Si System ion, electron, vacuum, target 1340
 
  • G. Agarwal, R. Dhunna, I.P. Jain, V.K. Kulshrestha
    UOR, Jaipur
  • D. Kabiraj
    IUAC, New Delhi
 
 

Swift Heavy Ion (SHI) induced modification at Metal/Si interfaces has emerged as an interesting field of research due to its large applications. In the present study we investigate SHI induced mixed molybdenum silicide film with ion fluences. The Molybdenum and Si thin thin films were deposited on Silicon substrates using e-beam evaporation at 10-8 torr vacuum. Thin films were irradiated with Au ions of energy 120 MeV to form molybdenum silicide. The samples were characterized by grazing incidence X-ray diffraction (GIXRD) technique for the identification of phase formation at the interface. Rutherford backscattering spectrometry (RBS) was used to investigate the elemental distribution in the films. The mixing rate calculations were made and the diffusivity values obtained leads to a transient melt phase formation at the interface according to thermal spike model.

 
TU6PFP030 6D Acceleration Studies in Proton Fixed Field Alternating Gradient Accelerator Lattices proton, cyclotron, neutron, injection 1354
 
  • S.C. Tygier
    Manchester University, Manchester
  • R.J. Barlow, H.L. Owen
    UMAN, Manchester
 
 

It has been proposed to use a proton Fixed Field Alternating Gradient (FFAG) accelerator to drive an Accelerator Driven Subcritical Reactor (ADSR) as they have the potential to provide high current beams to energies needed, 500 MeV to 1 GeV. This paper describes the results of 6D simulations of acceleration in possible lattice designs to explore longitudinal acceptance. This is needed to evaluate accelerator duty cycle and options for acceleration such as harmonic number jumping.

 
TU6PFP071 Exploration of Design Alternative for an 8 GeV Proton Linac at Fermilab linac, cavity, emittance, cryomodule 1454
 
  • X. Wu, C. Compton, M. Doleans, W. Hartung, R.C. York, Q. Zhao
    NSCL, East Lansing, Michigan
 
 

An 8 GeV proton linac is being considered for the Fermilab accelerator complex. A design calls for five superconducting cavity types: three types of half-wave and two types of multi-cell elliptical structures. The elliptical cavity types have a frequency of 1.3 GHz with a beta = 0.81 and a beta = 1 and provide acceleration from 420 MeV to 8 GeV. An alternative concept would be to use an additional 1.3 GHz elliptical cavity type starting at 150 MeV. The alternative design may reduce project cost and risk. It would increase the technology overlap between Project X and the International Linear Collider. Preliminary simulations show the alternative linac layout has adequate longitudinal acceptance. This paper will discuss the beam dynamics studies for the alternative linac layout in comparison with the baseline layout.

 
TU6PFP075 Progress in Antiproton Production at the Fermilab Tevatron Collider antiproton, target, kicker, collider 1463
 
  • R.J. Pasquinelli, B.E. Drendel, K. E. Gollwitzer, S.R. Johnson, V.A. Lebedev, A.F. Leveling, J.P. Morgan, V.P. Nagaslaev, D.W. Peterson, A.D. Sondgeroth, S.J. Werkema
    Fermilab, Batavia
 
 

Run II has been ongoing since 2001. Peak luminosities in the Tevatron have increased from approximately 10×1030 cm-2ses-1 to 300×1030 cm-2ses-1 – a factor of 30 improvement. A significant contributing factor in this remarkable progress is a greatly improved antiproton production capability. Since the beginning of Run II, the average antiproton accumulation rate has increased from 2×1010 p/hr to about 24×1010 p/hr. Peak antiproton stacking rates presently exceed 25×1010 p/hr. The antiproton stacking rate has nearly doubled in the last two years alone. A variety of improvements have contributed to the recent progress in antiproton production. The process of transferring antiprotons to the Recycler Ring for subsequent transfer to the collider has been significantly restructured and streamlined, allowing more time to be utilized for antiproton production. Improvements to the target station have greatly increased the antiproton yield from the production target. The performance of the Antiproton Source stochastic cooling systems has been enhanced by improvements to the cooling electronics, accelerator lattice optimization, and improved operating procedures.

 
TU6PFP078 Stochastic Cooling for the HESR at the FAIR Facility target, pick-up, kicker, antiproton 1472
 
  • H. Stockhorst, R. Maier, D. Prasuhn, R. Stassen
    FZJ, Jülich
  • T. Katayama
    CNS, Saitama
  • L. Thorndahl
    CERN, Geneva
 
 

The High Energy Storage Ring (HESR) of the future International Facility for Antiproton and Ion Research (FAIR) at the GSI in Darmstadt will be built as an anti-proton cooler ring in the momentum range from 1.5 to 15 GeV/c. An important and challenging feature of the new facility is the combination of phase space cooled beams with internal targets. In addition to electron cooling transverse and longitudinal stochastic cooling are envisaged to accomplish these goals. A detailed numerical analysis of the Fokker-Planck equation for longitudinal filter and time-of-flight cooling including an internal target and intrabeam scattering has been carried out to demonstrate the stochastic cooling capability. Model predictions have been compared to experimental cooling results with internal targets at the COSY facility. Experimental results at COSY to compensate the large mean energy loss induced by an internal Pellet target similar to that being used by the PANDA experiment at the HESR with a barrier bucket cavity (BB) will be presented. Experimental tests of stochastic filter cooling with internal target and BB operation as well as expected cooling properties for the HESR are discussed.

 
TU6PFP080 Nonscaling FFAG Variants for HEP and Medical Applications acceleration, proton, ion, controls 1478
 
  • C. Johnstone
    Fermilab, Batavia
  • M. Berz, K. Makino
    MSU, East Lansing, Michigan
  • S.R. Koscielniak
    TRIUMF, Vancouver
  • F.E. Mills
    PAC, Batavia, Illinois
  • P. Snopok
    UCR, Riverside, California
 
 

The quest for higher beam power and duty factor and precisely controlled beams at reasonable cost has generated world-wide interest in Fixed-field Alternating Gradient accelerators (FFAGs). A new concept in non-scaling FFAGs to stabilize the betatron tune is under development. The emphasis to date has been on electron and proton accelerators, yet many facilities utilize H- front ends. This concept naturally extends to H- FFAGs and under conditions of rapid acceleration, the FFAG functions essentially as a recirculating linac with a common-aperture arc. As such it may be suitable for replacement of aging H- linac sections. For a slow acceleration cycle, an H- FFAG machine can exploit H- techniques to control extraction and intensity, and represents an innovation in proton therapy accelerators. Prototype RF and magnet component design have been initiated. For ten-turn acceleration, the rf cavities in a 10-100 MeV FFAG cannot be re-phased on the revolution time scale, and local adjustment of the pathlength is the proposed approach. For slow acceleration, broad-band, low-frequency rf can be applied. The basic optics and components for such FFAGs are presented.

 
TU6RFP044 Options for an 11 GeV RF Beam Separator for the Jefferson Lab CEBAF Upgrade cavity, extraction, optics, linac 1644
 
  • J.R. Delayen, M. Spata, H. Wang
    JLAB, Newport News, Virginia
  • J.R. Delayen
    ODU, Norfolk, Virginia
 
 

Funding: Authored by Jefferson Science Associates, LLC under U.S. DOE Contract No. DE-AC05-06OR23177


The CEBAF accelerator at Jefferson Lab has had, since first demonstration in 1996, the ability to deliver a 5-pass electron beam to experimental halls (A, B, and C) simultaneously. This capability was provided by a set of three, room temperature 499 MHz rf separators in the 5th pass beamline. The separator was two-rod, TEM mode type resonator, which has a high shunt impedance. The maximum rf power to deflect the 6 GeV beams was about 3.4kW. The 12 GeV baseline design does not preserve the capability of separating the 5th pass, 11 GeV beam for the 3 existing halls. Several options for restoring this capability, including extension of the present room temperature system or a new superconducting design in combination with magnetic systems, are under investigation and are presented.

 
WE2PBC01 Local Chromaticity Measurement Using the Response Matrix Fit at the APS sextupole, quadrupole, betatron, focusing 1849
 
  • V. Sajaev
    ANL, Argonne
 
 

Funding: Work supported by the U.S. Department of Energy, Office of Science, Office of Basic Energy Sciences, under Contract No. DE-AC02-06CH11357.


The response matrix fit is routinely used at APS for linear optics correction. The high accuracy of the method enables us to measure the variation of betatron phase advance around the ring with rf frequency. This variation can be used to calculate local chromaticity. Such measurements were first performed at the APS at the moment when a sextupole was mistakenly connected with the wrong polarity. Local chromaticity calculations clearly pointed to the location of the sextupole error. Results and details of the measurements are reported and discussed.

 

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WE3PBI01 Head-Tail Modes for Strong Space Charge space-charge, damping, synchrotron, emittance 1889
 
  • A.V. Burov
    Fermilab, Batavia
 
 

Head-tail modes are described when the space charge tune shift significantly exceeds the synchrotron tune. Spatial shape of the modes, their frequencies, coherent growth rates and Landau damping rates are found.

 

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Slides

 
WE3PBC04 Nonlinear Dynamics Study of Storage Ring with Super-Periods sextupole, dynamic-aperture, storage-ring, emittance 1904
 
  • H. Hao, X.Q. Wang
    USTC/NSRL, Hefei, Anhui
  • Y.K. Wu
    FEL/Duke University, Durham, North Carolina
 
 

Funding: Work supported by US Air Force Office of Scientific Research medical FEL grant FA9550-04-01-0086 (YKWu), also supported by National Natural Science Foundation of China (No.10175062 and 10575100).


Many modern light source storage rings use a basic magnetic lattice structure consisting of a number of repetitive periodic lattice block, the super periods. The study of one super-period can reveal the dynamical proprieties of the storage ring. Unlike the traditional approach of studying the one-turn map of the storage ring, the work focuses on the study of a super-period lattice, which allows us to gain new insight into the storage ring dynamics using a simpler magnetic structure. In this paper, both analytical and numerical techniques, including Lie Algebra and Normal Form, and particle tracking and frequency analysis, are used to study the nonlinear dynamics of one super-period of a standard double-bend achromat (DBA) and triple-bend achromat (TBA) with two or more nonlinear elements (e.g. sextupoles). The relationship between the super-period dynamics and storage ring dynamics is explored in terms of the global lattice tuning and local lattice selection for straight sections.


H. Hao is currently working as a visiting scholar at Duke University Free Electron Laser Laboratory.

 

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Slides

 
WE3PBC05 Advanced Simulation and Optimization Tools for Dynamic Aperture of Non-Scaling FFAGs and Related Accelerators Including Modern User Interfaces simulation, dynamic-aperture, proton, cyclotron 1907
 
  • C. Johnstone, V. Kashikhin
    Fermilab, Batavia
  • M. Berz, K. Makino
    MSU, East Lansing, Michigan
  • P. Snopok
    St. Petersburg State University, St. Petersburg
 
 

Innovations in computer techniques in combination with increased sophistication in modeling are required to accurately understand, design and predict high-energy, and, in particular, the new generation of frontier accelerators for HEP and other applications. A recently identified problem lies in the simulation and optimization of FFAGs and related devices, for which currently available tools provide only approximate and inefficient simulation. For this purpose new tools are being developed within the advanced accelerator code COSY INFINITY to address complex, specific electromagnetic fields, including high-order fringe fields, out of plane fields, edge effects, and general field profiles; tools linked to modern global optimization techniques that can further accommodate the ultra-large emittances of proposed beams to allow efficient probing of very high dimensional parameter space. This new set of tools based on modern techniques and simulation approaches will be furnished with modern GUI-based user interfaces.

 

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Slides

 
WE5PFP004 Titanium Nitride Coating as a Multipactor Suppressor on RF Coupler Ceramic Windows multipactoring, target, controls, vacuum 1991
 
  • W. Kaabi, H. Jenhani, A. Variola
    LAL, Orsay
  • G. Keppel, V. Palmieri
    INFN/LNL, Legnaro (PD)
 
 

LAL-Orsay is developing an important effort on R&D studies on RF power couplers. One of the most critical components of those devices is the ceramic RF window that allows the power flux to be injected in the coaxial line. The presence of a dielectric window on a high power RF line has a strong influence on the multipactor phenomena. To reduce this effect, the decrease the secondary emission yield (SEY)of the ceramic window is needed. Due to its low SEY coefficient, TiN coating is used for this goal. In this framework, a TiN sputtering bench has been developed in LAL. The reactive sputtering of TiN needs the optimisation of gas flow parameters and electrical one, to obtain stoechiometric deposit. XRD analysis was performed to control the film composition and stoechiometry. Measurements point out how the Nitrogen vacancy on the film can be controlled acting on the N2 flow. In addition, the coating thickness must be optimized so that the TiN coating effectively reduces the SEY coefficient but does not cause excessive heating, due to ohmic loss. For this purposes, multipactor level breakdown and resistance measurements were done for different deposit thickness.

 
WE5RFP003 Transverse Deflecting RF Structures in the Designed QBA Lattice of Taiwan Photon Source emittance, cavity, electron, sextupole 2264
 
  • H. Ghasem, G.-H. Luo
    NSRRC, Hsinchu
 
 

Quadruple Bend Achromat (QBA) low emittance lattice of 3GeV Taiwan Photon Source (TPS) allows us to consider three configurations for location of a pair of superconducting transverse RF deflecting cavities for generation ultra short X-ray pulses. The available arrangements for location of cavities in a super-period of TPS are investigated. We find that use of such deflecting cavities in the middle of two QBA lattices in a super-period of TPS provides better conditions for emittance of electron beam.

 
WE5RFP004 Study of Errors due to Utilization of the Transverse Deflectors in QBA Lattice of Taiwan Photon Source emittance, cavity, electron, simulation 2267
 
  • H. Ghasem, G.-H. Luo
    NSRRC, Hsinchu
 
 

Deflecting cavity generates a correlation between longitudinal position and vertical momentum of electrons in the synchrotron light sources for production short X-ray pulses. Use of such structures leads to growth in vertical amplitude and slope of stored electrons. Since errors are characteristic of real machine, any errors associated with the photon compression system must be considered and the tolerance of them must be evaluated. In this paper we present simulation of main errors due to deflecting structures, QBA lattice and injection system and find tolerances of them.

 
WE5RFP006 Progress Report of the TPS Lattice Design booster, sextupole, quadrupole, dipole 2273
 
  • C.-C. Kuo, H.-P. Chang, H.C. Chao, P.J. Chou, G.-H. Luo, H.-J. Tsai
    NSRRC, Hsinchu
 
 

A 3 GeV synchrotron light source is planned to be built at the existing site of NSRRC campus. The project is called the Taiwan Photon Source (TPS). It will provide x-ray photon beam with brilliance several orders higher than the one generated by the existing 1.5 GeV synchrotron. The design issues of accelerator lattice for the 3 GeV storage ring and booster injector will be presented. These issues cover the properties of linear and nonlinear beam dynamics, the optimization of dynamic aperture and momentum acceptance, collective beam instabilities and lifetime issues, the effects caused by various error sources and technical measures to suppress these error effects, etc.

 
WE5RFP009 Correction of Imperfections in the SLS Storage Ring sextupole, quadrupole, storage-ring, emittance 2282
 
  • A. Streun, M. Böge, J.T.M. Chrin, A. Lüdeke
    PSI, Villigen
 
 

Recently the energy acceptance and Touschek lifetime of the storage ring of the Swiss Light Source (SLS) could be successfully set to values in agreement with simulations for an ideal lattice. This was finally achieved through control of linear coupling and symmetrization of the sextupole pattern. 36 small corrector magnets were installed for this purpose as additional windings on the ring sextupoles: 30 skew quadrupoles (24 at zero and 6 at maximum dispersion) and 6 auxiliary sextupoles. Base for the success of these measures were previous corrections of dipolar and quadrupolar errors, which we will summarize briefly.

 
WE5RFP010 Low-Alpha Operation of the SLS Storage Ring synchrotron, injection, storage-ring, radiation 2285
 
  • A. Streun, M. Böge, N. Milas, F. Müller, V. Schlott, H. Sigg
    PSI, Villigen
  • G.A. Amatuni, D. Gishyan, K. Manukyan, A. Sargsyan
    CANDLE, Yerevan
 
 

Recently tentative top-up operation of the Swiss Light Source (SLS) storage ring at low momentum compaction factor has been started. We will present an analysis of the longitudinal dynamics and simulations of the injection process, and explain our method to ensure closed orbit stability. First experimental results will be shown and compared to the model predictions.

 
WE5RFP015 Concepts for the PEP-X Light Source emittance, brightness, storage-ring, cavity 2297
 
  • R.O. Hettel, K.L.F. Bane, K.J. Bertsche, Y. Cai, A. Chao, V.A. Dolgashev, J.D. Fox, X. Huang, Z. Huang, T. Mastorides, C.-K. Ng, Y. Nosochkov, A. Novokhatski, T. Rabedeau, C.H. Rivetta, J.A. Safranek, J. Seeman, J. Stohr, G.V. Stupakov, S.G. Tantawi, L. Wang, M.-H. Wang, U. Wienands, L. Xiao
    SLAC, Menlo Park, California
  • I. Lindau
    Stanford University, Stanford, California
  • C. Pellegrini
    UCLA, Los Angeles, California
 
 

Funding: This work was supported by the Director, Office of Science, Office of Basic Energy Sciences, of the U.S. Department of Energy under Contract No. DE-AC02-76SF00515.


SSRL and SLAC groups are developing a long-range plan to transfer its evolving scientific programs from the SPEAR3 light source to a much higher performing photon source that would be housed in the 2.2-km PEP-II tunnel. While various concepts for the PEP-X light source are under consideration, including ultimate storage ring and ERL configurations, the present baseline design is a very low-emittance storage ring. A hybrid lattice has DBA or QBA cells in two of the six arcs that provide a total ~30 straight sections for ID beam lines extending into two new experimental halls. The remaining arcs contain TME cells. Using ~100 m of damping wigglers the horizontal emittance at 4.5 GeV would be ~0.1 nm-rad with >1 A stored beam. PEP-X will produce photon beams having brightnesses near 1022 at 10 keV. Studies indicate that a ~100-m undulator could have FEL gain and brightness enhancement at soft x-ray wavelengths with the stored beam. Crab cavities or other beam manipulation systems could be used to reduce bunch length or otherwise enhance photon emission properties. The present status of the PEP-X lattice and beam line designs are presented and other implementation options are discussed.

 
WE5RFP024 HALS: Our Future Light Source at NSRL emittance, damping, wiggler, radiation 2321
 
  • L. Wang, Z. Bai, G. Feng, W. Li, L. Liu, C.-F. Wu, S.C. Zhang
    USTC/NSRL, Hefei, Anhui
 
 

Hefei Light Source is a second generation VUV light source, whose performance cannot meet the requirements of synchrotron radiation users at the present time. One year ago, the concept of the Hefei Advanced Light Source, whose main features are ultra low beam emittance and high brilliance in VUV and soft X-ray range, was brought forward. In the preliminary design study, a medium scale storage ring and multi bend achromat focusing structure were adopted to achieve beam emittance lower than 0.2 nm.rad. Linear and nonlinear parameter optimizations were performed to obtain large on-momentum and off-momentum dynamic aperture. The design status will be introduced briefly in the presentation.

 
WE5RFP043 Optics Design for a Soft X-Ray FEL at the SLAC A-Line linac, emittance, undulator, dipole 2364
 
  • H. Geng, Y.T. Ding, P. Emma, Z. Huang, Y. Nosochkov, M. Woodley
    SLAC, Menlo Park, California
 
 

Funding: This work is supported by the Department of Energy contract DE-AC02-76SF00515.


LCLS capabilities can be significantly extended with a second undulator aiming at the soft x-ray spectrum (1- 5 nm). To allow for simultaneous hard and soft x-ray operations, 14 GeV beams at the end of the LCLS accelerator can be intermittently switched into the SLAC A-line (the beam transport line to End Station A) where the second undulator may be located. In this paper, we discuss the A-line optics design for transporting the high-brightness LCLS beams using the existing tunnel. To preserve the high brightness of the LCLS beams, special attentions are paid to effects of incoherent and coherent synchrotron radiation. Start-to-end simulations using realistic LCLS beam distributions are carried out.

 
WE5RFP071 Overview of Quasi-Periodic Undulators undulator, radiation, photon, synchrotron 2426
 
  • S. Sasaki
    HSRC, Higashi-Hiroshima
 
 

After the first demonstration of original quasi-periodic undulator (QPU) at the NIJI-IV*, there have been many modifications for QPU structures. One of the first most productive improvements was introducing the quasi-periodicity by modifying the magnetic field in a periodic undulator instead of modifying the period length**. In addition to this practical improvement, a slight modification of creation theory of one-dimensional quasi-periodicity gave another advantage for building this type of device. As the result, many different types of QPUs for generating both linearly and elliptically polarized radiations have been installed in the synchrotron radiation (SR) facilities worldwide. Furthermore, some more SR facilities are considering to building such devices in order to improve their performance. In the presentation, we will discuss about limitations and possible improvements of performance of QPU on the basis of synchrotron radiation physics and mathematics of quasi-periodicity.


*Kawai, et al, Proc. EPAC96, p.2549.
**Diviacco, Walker, ELETTRA Technical Note ST/M-TN-97/11, 1997, Chavanne, et al, Proc. EPAC98, p.2213, Diviacco, et al, ibid., p.2216.

 
WE6PFP006 Overview of Magnetic Nonlinear Beam Dynamics in RHIC sextupole, dipole, resonance, dynamic-aperture 2489
 
  • Y. Luo, M. Bai, J. Beebe-Wang, J. Bengtsson, R. Calaga, W. Fischer, A.K. Jain, N. Malitsky, S. Peggs, F.C. Pilat, V. Ptitsyn, G. Robert-Demolaize, T. Satogata, S. Tepikian, D. Trbojevic
    BNL, Upton, Long Island, New York
  • R. Tomás
    CERN, Geneva
 
 

Funding: Work supported by Brookhaven Science Associates, LLC under Contract No. DE-AC02-98CH10886 with the U.S. Department of Energy.


In the article we review the nonlinear beam dynamics from nonlinear magnetic fields in the Relativistic Heavy Ion Collider. The nonlinear magnetic fields include the magnetic field errors in the interaction regions, chromatic sextupoles, and sextupole component from arc dipoles. Their effects on the beam dynamics and long-term dynamic apertures are evaluated. The online measurement and correction methods for the IR nonlinear errors, nonlinear chromaticity, and horizontal third order resonance are reviewed. The overall strategy for the nonlinear effect correction in the RHIC is discussed.

 
WE6PFP007 Dynamic Aperture Evaluation for the RHIC 2009 Polarized Proton Runs dynamic-aperture, emittance, sextupole, proton 2492
 
  • Y. Luo, M. Bai, J. Beebe-Wang, W. Fischer, C. Montag, G. Robert-Demolaize, T. Satogata, S. Tepikian, D. Trbojevic
    BNL, Upton, Long Island, New York
 
 

Funding: Work supported by Brookhaven Science Associates, LLC under Contract No. DE-AC02-98CH10886 with the U.S. Department of Energy.


In preparation for the RHIC polarized proton run 2009, simulations were carried out to evaluate the million turn dynamic apertures for different beta*s at the proposed beam energies of 100 GeV and 250 GeV. One goal of this study is to find out the best beta* for this run. We also evaluated the effects of the second order chromaticity correction. The second order chromaticties can be corrected with the MAD8 Harmon module or by correcting the horizontal and vertical half-integer resonance driving terms.

 
WE6PFP023 Status of the CLIC Beam Delivery System luminosity, collimation, laser, wakefield 2537
 
  • R. Tomás, B. Dalena, J. Resta-López, G. Rumolo, D. Schulte
    CERN, Geneva
  • D. Angal-Kalinin, F. Jackson
    STFC/DL/ASTeC, Daresbury, Warrington, Cheshire
  • B. Bolzon, L. Brunetti, N. Geffroy, A. Jeremie
    IN2P3-LAPP, Annecy-le-Vieux
  • K.P. Schuler
    DESY, Hamburg
  • A. Seryi
    SLAC, Menlo Park, California
 
 

The CLIC BDS is experiencing the careful revision from a large number of world wide experts. This was particularly enhanced by the successful CLIC'08 workshop held at CERN. Numerous new ideas, improvements and critical points are arising, establishing the path towards the Conceptual Design Report by 2010.

 
WE6PFP024 ATF2 Ultra-Low IP Betas Proposal emittance, octupole, linear-collider, simulation 2540
 
  • R. Tomás, H.-H. Braun, J.-P. Delahaye, A. Marin, D. Schulte, F. Zimmermann
    CERN, Geneva
  • D. Angal-Kalinin, J.K. Jones
    STFC/DL/ASTeC, Daresbury, Warrington, Cheshire
  • S. Bai, J. Gao, X.W. Zhu
    IHEP Beijing, Beijing
  • P. Bambade, M. Renier
    LAL, Orsay
  • Y. Honda, S. Kuroda, T. Okugi, T. Tauchi, N. Terunuma, J. Urakawa
    KEK, Ibaraki
  • A. Scarfe
    UMAN, Manchester
  • A. Seryi, G.R. White, M. Woodley
    SLAC, Menlo Park, California
 
 

The CLIC Final Focus System has considerably larger chromaticity than those of ILC and its scaled test machine ATF2. We propose to reduce the IP betas of ATF2 to reach a CLIC-like chromaticity. This would also allow to study the FFS tuning difficulty as function of the IP beam spot size. Both the ILC and CLIC projects will largely benefit from the ATF2 experience at these ultra-low IP betas.

 
WE6PFP037 3D Strong-Strong Simulations of Wire Compensation of Long-Range Beam-Beam Effects at LHC emittance, simulation, beam-beam-effects, luminosity 2576
 
  • J. Qiang
    LBNL, Berkeley, California
 
 

Funding: Work supported by the U.S. Department of Energy under Contract No. DE-AC02-05CH11231.


In this paper, we report on studying wire compensation of long-range beam-beam effects using a fully 3D strong-strong beam-beam model. The simulations include two head-on collisions with 0.3 mrad crossing angle and 64 long-range beam-beam collisions near IP 1 and IP5. We found that using conducting wires with appropriate current level will compensate the tail emittance growth due to long-range beam-beam effects. The random fluctuation of current level should be controlled below 0.1% level for a good compensation. Lowering the long-range beam-beam separations by 20% together with wire compensation will improve the luminosity by a few percentage. Further reducing the beam-beam separations causes significant beam blow-up and decrease of luminosity.

 
WE6PFP041 Petavac: 100 TeV Proton-Antiproton Collider in SSC Tunnel dipole, luminosity, collider, synchrotron 2585
 
  • P.M. McIntyre, A. Sattarov
    Texas A&M University, College Station, Texas
 
 

Funding: DOE grant DE-FG02-06ER41405.


A conceptual design is presented for a 100 TeV proton-antiproton collider consisting of a single storage ring based upon 16.5 T dipoles, installed in the 83 km circumference SSC tunnel, fed using a proportionately expanded antiproton source. Provisions have been designed to intercept synchrotron light on room-temperature photon stops and to suppress electron cloud effect using a continuous clearing electrode running throughout the collider. Beams would be separated using split dipoles so that 20 ns bunch spacing should be attainable. Synchrotron damping time of half-hour would help to stabilize against mechanisms for slow emittance growth. It is reasonable to project the potential for a luminosity of 1035/cm2/s.

 
WE6PFP044 Lattice Design for SuperKEKB quadrupole, dynamic-aperture, cavity 2591
 
  • H. Koiso, A. Morita, Y. Ohnishi, K. Oide
    KEK, Ibaraki
 
 

Lattice design for SuperKEKB is based on the present KEKB lattice. The unit-cell structure of KEKB has a wide range of flexibility, therefore main beam-optical parameters can be adjusted without changing the arcs. The interaction region (IR) and the other straight sections are changed to squeeze the vertical beta function to 3 mm at IP, keeping sufficient dynamic apertures. Recent progress such as a new design of IR with superconducting quadrupole magnets at 1.9 K, traveling focus scheme by using crab cavities, local chromaticity correction for the high energy ring, is presented.

 
WE6PFP049 Crab Waist Collision Scheme: Numerical Simulations versus Experimental Results luminosity, simulation, sextupole, collider 2604
 
  • P.A. Piminov, E.B. Levichev, D.N. Shatilov
    BINP SB RAS, Novosibirsk
  • C. Milardi, M. Zobov
    INFN/LNF, Frascati (Roma)
  • K. Ohmi
    KEK, Ibaraki
 
 

A novel scheme of crab waist collisions has been successfully tested at the electron-positron collider DAΦNE, Italian Phi-factory. In this paper we compare numerical simulations of the crab waist beam-beam interaction with obtained experimental results. For this purpose we perform weak-strong and quasi strong-strong beam-beam simulations using a realistic DAΦNE lattice model that has proven to reproduce reliably both linear and nonlinear collider optics.

 
WE6PFP053 A Proposed Fast Luminosity Feedback for the Super-B Accelerator luminosity, feedback, shielding, power-supply 2616
 
  • K.J. Bertsche, R.C. Field, A.S. Fisher, M.K. Sullivan
    SLAC, Menlo Park, California
  • A. Drago
    INFN/LNF, Frascati (Roma)
 
 

Funding: Work supported by the Department of Energy under contract number DE-AC03-76SF00515.


We present a possible design for a fast luminosity feedback for the Super-B Interaction Point (IP). The design is an extension of the fast luminosity feedback installed on the PEP-II accelerator. During the last two runs of PEP-II and BaBar (2007-2008), we had an improved luminosity feedback system that was able to maintain peak luminosity with faster correction speed than the previous system. The new system utilized fast dither coils on the High-Energy Beam (HEB) to independently dither the x position, the y position and the y angle at the IP, at roughly 100 Hz. The luminosity signal was then read out with three independent lock-in amplifiers. An overall correction was computed based on the lock-in signal strengths and beam corrections for position in x and y and in the y angle at the IP were simultaneously applied to the HEB. With the 100 times increase in luminosity for the SuperB design, we propose using a similar fast luminosity feedback that can operate at frequencies between DC and 1 kHz, high enough to be able to follow and nullify any vibrational beam motion from the final focusing magnets.

 
WE6PFP064 Achromatic Interaction Point Design collider, focusing, emittance, interaction-region 2649
 
  • Y.S. Derbenev, S.A. Bogacz, P. Chevtsov
    JLAB, Newport News, Virginia
  • A. Afanasev, C.M. Ankenbrandt, V. Ivanov, R.P. Johnson, G.M. Wang
    Muons, Inc, Batavia
 
 

Designers of high-luminosity energy-frontier muon colliders must provide strong beam focusing in the interaction regions. However, the construction of a strong, aberration-free beam focus is difficult and space consuming, and long straight sections generate an off-site radiation problem due to muon decay neutrinos that interact as they leave the surface of the earth. Without some way to mitigate the neutrino radiation problem, the maximum c.m. energy of a muon collider will be limited to about 3.5 TeV. A new concept for achromatic low beta design is being developed, in which the interaction region telescope and optical correction elements, are installed in the bending arcs. The concept, formulated analytically, combines space economy, a preventative approach to compensation for aberrations, and a reduction of neutrino flux concentration. An analytical theory for the aberration-free, low beta, spatially compact insertion is being developed.

 
WE6PFP098 Multipass Arc Lattice Design for Recirculating Linac Muon Accelerators optics, linac, focusing, controls 2736
 
  • G.M. Wang
    ODU, Norfolk, Virginia
  • S.A. Bogacz
    JLAB, Newport News, Virginia
  • R.P. Johnson, G.M. Wang
    Muons, Inc, Batavia
  • D. Trbojevic
    BNL, Upton, Long Island, New York
 
 

Funding: Supported in part by USDOE STTR Grant DE-FG02-08ER86351


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. One problem is that in the simplest schemes, a separate return arc is required for each passage of the muons through the linac. 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. With these sorts of arcs and a single linac, a Recirculating Linear Accelerator (RLA) will have greater cost effectiveness and reduced losses from muon decay. We will develop the optics and 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.

 
WE6PFP099 Muon Storage Rings for a Neutrino Factory factory, site, storage-ring, proton 2739
 
  • C.R. Prior
    STFC/RAL/ASTeC, Chilton, Didcot, Oxon
 
 

The goal of a Neutrino Factory is to generate intense beams of neutrinos from muon decay inorder to study CP violation in the Standard Model, the mass hierarchy, and the neutrino mixing angle θ13. Intense muon beams are created and accelerated in a system of particle accelerators to energies of 20-50 GeV. They are then allowed to decay in dedicated storage rings with long straight sections aligned on suitably chosen long-range detectors. A variety of geometries are possible, and their design and construction present demanding challenges for accelerator R & D, covering not only beam optics but touching on geological and engineering aspects of constructing almost vertical storage rings several hundred metres below the Earth's surface. The basic ideas are described in this paper and are demonstrated by three possible models developed in recent years.

 
WE6PFP104 CesrTA Low-Emittance Tuning – First Results coupling, emittance, quadrupole, betatron 2754
 
  • J.P. Shanks, M.G. Billing, S.S. Chapman, M.J. Forster, S.B. Peck, D. L. Rubin, D. Sagan, J.W. Sexton
    CLASSE, Ithaca, New York
 
 

Funding: Support provided by the US National Science Foundation and the US Department of Energy.


The Cornell Electron Storage Ring has been reconfigured as a test accelerator (CesrTA) for low emittance damping ring R&D for the International Linear Collider (ILC). We are developing low emittance tuning techniques with a goal of 1) achieving a vertical emittance approaching that of the ILC damping rings and 2) Gaining an understanding of the effectiveness of those techniques. We will use gain mapping to characterize beam position monitor (BPM) electrode gains, orbit response analysis to determine BPM button misalignments, betatron phase and coupling measurements to characterize optical errors, and orbit and dispersion measurements to locate sources of vertical dispersion. We are investigating a nondestructive dispersion measurement that depends on exciting a synchrotron oscillation and monitoring the phase and amplitude at each BPM. We have developed the analysis tools necessary to correct magnet and alignment errors. An x-ray beam size monitor is being deployed that will allow us to monitor vertical emittance in real time, allowing for empirical tuning of beam size. We will describe the measurement and correction techniques and show data demonstrating their efficacy.

 
WE6PFP105 Lattice Options for the CLIC Damping Rings emittance, wiggler, damping, quadrupole 2757
 
  • Y. Papaphilippou, F. Antoniou
    CERN, Geneva
  • E.B. Levichev, S.V. Sinyatkin, P. Vobly, K. Zolotarev
    BINP SB RAS, Novosibirsk
  • P. Raimondi
    INFN/LNF, Frascati (Roma)
 
 

Optics design optimisation studies have been undertaken for the CLIC damping ring lattice. Main parameters such as the ring energy and output longitudinal emittance were reconsidered in order to reduce the detrimental effect of collective instabilities. In this respect, the low emittance arc cell length was rationalized taking into account space and magnet design requirements. The straight section cell filled with super-conducting wigglers was modified to accommodate a robust absorption scheme. Several low emittance rings were considered and compared with respect to their dynamic aperture and the IBS-dominated output emittances.

 
WE6PFP107 Design Considerations for the CLIC Pre-Damping Rings emittance, wiggler, dipole, damping 2760
 
  • F. Antoniou
    National Technical University of Athens, Zografou
  • Y. Papaphilippou, F. Zimmermann
    CERN, Geneva
 
 

The CLIC pre-damping rings have to accommodate a large emittance beam, coming in particular from the positron target and reduce its size to low enough values for injection into the main damping rings. In particular, polarized positron stacking imposes stringent requirements with respect to longitudinal acceptance and damping times. Linear lattice design options based on low-emittance cells, multiple bend cells and the inclusion of damping wigglers are compared with respect to linear optics functions, tunability, chromatic properties and acceptance. The optics of special regions for the placement of injection, extraction and RF elements are also presented. Non-linear dynamics simulations are finally undertaken for evaluating and maximizing the rings dynamic aperture, especially for large momentum spreads.

 
WE6RFP019 Simulation Results for Crystal Collimation Experiment in SPS UA9 simulation, proton, scattering, octupole 2823
 
  • E. Laface, W. Scandale
    CERN, Geneva
  • G. Cavoto
    INFN-Roma, Roma
  • S. Peggs
    BNL, Upton, Long Island, New York
 
 

The UA9 experiment will take place in 2009 at the CERN-SPS and will evaluate the feasibility of silicon crystals as primary collimators for a storage ring. A crystal placed at 6 σ from the beam core will deviate protons towards two roman pots and a tungsten absorber (TAL). In this paper the authors show simulations of the expected beam dynamics and of the capture efficiency into the secondary collimator. The result of these simulations will guide us in interpreting the experimental data expected in UA9.

 
WE6RFP057 Wake Fields in Photonic Crystal Accelerator Structures and Application to RF Sources wakefield, cavity, HOM, higher-order-mode 2929
 
  • G.R. Werner, C.A. Bauer, J.R. Cary, T. Munsat
    CIPS, Boulder, Colorado
 
 

Funding: This work is supported by the U.S. Department of Energy grant DE-FG02-04ER41317.


The RF properties of photonic crystals (PhCs) can be exploited to avoid the parasitic higher order modes (HOMs) that degrade beam quality in accelerator cavities and reduce efficiency and power in RF generators. Computer simulations show that long-range wake fields are significantly reduced in accelerator structures based on dielectric PhC cavities, which can be designed to trap only those modes within a narrow frequency range. A 2D PhC structure can be used to create a 3D accelerator cavity by using metal end-plates to confine the fields in the third dimension; however, even when the 2D photonic structure allows only a single mode, the 3D structure may trap HOMs, such as guided modes in the dielectric rods, that increase wake fields. For a 3D cavity based on a triangular lattice of dielectric rods, the rod positions can be optimized (breaking the lattice symmetry) to reduce radiation leakage using a fixed number of rods; moreover, the optimized structure has reduced wake fields. Using computer simulation, wake fields in pillbox, PhC, and optimized photonic cavities are calculated; a design for a klystron using the optimized photonic cavity structure is presented.

 
WE6RFP092 Axial Channeling of Positively Charged High-Energy Proton Beams proton, scattering, alignment, simulation 3010
 
  • V. Guidi, S. Baricordi, P. Dalpiaz, M. Fiorini
    UNIFE, Ferrara
  • A.G. Afonin, Y.A. Chesnokov, V.A. Maisheev, I.A. Yazynin
    IHEP Protvino, Protvino, Moscow Region
  • G. Ambrosi, B. Bertucci, W.J. Burger, P. Zuccon
    INFN-PG, Perugia
  • D. Bolognini, S. Hasan, A. Mozzanica, M. Prest
    Università dell'Insubria & INFN Milano Bicocca, Como
  • G. Cavoto, R. Santacesaria, P. Valente
    INFN-Roma, Roma
  • G. Della Mea, R. Milan, A. Vomiero
    INFN/LNL, Legnaro (PD)
  • A.S. Denisov, Yu.A. Gavrikov, Yu.M. Ivanov, L.P. Lapina, L.G. Malyarenko, V. Skorobogatov, V.M. Suvorov, S.A. Vavilov
    PNPI, Gatchina, Leningrad District
  • A.D. Kovalenko, A.M. Taratin
    JINR, Dubna, Moscow Region
  • C. Luci
    Università di Roma I La Sapienza, Roma
  • A. Mazzolari
    INFN-Ferrara, Ferrara
  • W. Scandale
    CERN, Geneva
  • E. Vallazza
    INFN-Trieste, Trieste
 
 

The H8RD22 collaboration has accomplished an extensive study of axial channeling in the external lines of the CERN SPS. For 400 GeV protons, it was recorded deflection by about 90% of the particles by a short crystal, by far exceeding the performance of previous experiments. Axial channeling with 150 GeV negative hadrons was also firmly observed with deflection capability comparable to the case of positive particles. Near-axis effect such as multiple-volume reflections in a single crystal as a result of the superposition of volume reflections by a series of parallel planes sharing the same axis was investigated with 400 GeV protons. Confirmation of theoretical expectation was observed, in particular most of the particles were deflected by about 50 urad, four times the deflection angle imparted by a single volume reflection of most efficient planes. In this case the angular acceptance was sensitively broader than for the case of channeling. In summary, channeling in axial mode and multi-volume reflections were proven to be two mechanisms for manipulation steering of high-energy particle beams, which side most established techniques such as planar channeling and volume reflection.*


*Contribution on behalf of the H8RD22 collaboration.

 
WE6RFP094 Preliminary Study of the Arc for a Muon Collider with 1.5TeV CM Energy and Using 20T HTS Dipole Magnets collider, dipole, superconductivity, luminosity 3016
 
  • D.B. Cline, X.P. Ding
    UCLA, Los Angeles, California
  • R.C. Gupta
    BNL, Upton, Long Island, New York
  • R.J. Weggel
    Particle Beam Lasers, Inc., Northridge
 
 

We describe preliminary study of the design of a Muon Collider using 20T Dipole Magnets such a collider could be constructed at FNAL.

 
TH4GAC03 PAMELA Overview: Design Goals and Principles proton, ion, cavity, injection 3142
 
  • K.J. Peach, J.H. Cobb, S.L. Sheehy, H. Witte, T. Yokoi
    JAI, Oxford
  • M. Aslaninejad, M.J. Easton, J. Pasternak
    Imperial College of Science and Technology, Department of Physics, London
  • R.J. Barlow, H.L. Owen, S.C. Tygier
    UMAN, Manchester
  • C.D. Beard, P.A. McIntosh, S.L. Smith, S.I. Tzenov
    STFC/DL/ASTeC, Daresbury, Warrington, Cheshire
  • N. Bliss
    STFC/DL, Daresbury, Warrington, Cheshire
  • T.R. Edgecock, J.K. Pozimski, J. Rochford
    STFC/RAL, Chilton, Didcot, Oxon
  • R.J.L. Fenning, A. Khan
    Brunel University, Middlesex
  • M.A. Hill
    GIROB, Oxford
  • C. Johnstone
    Fermilab, Batavia
  • B. Jones, B. Vojnovic
    Gray Institute for Radiation Oncology and Biology, Oxford
  • D.J. Kelliher, S. Machida
    STFC/RAL/ASTeC, Chilton, Didcot, Oxon
  • R. Seviour
    Cockcroft Institute, Lancaster University, Lancaster
 
 

Funding: EPSRC EP/E032869/1


The PAMELA (Particle Accelerator for MEdicaL Applications) project is to design an accelerator for proton and light ion therapy using non-scaling Fixed Field Alternating Gradient (FFAG) accelerators, as part of the CONFORM project, which is also constructing the EMMA electron model of a non-scaling FFAG at Daresbury. This paper presents an overview of the PAMELA design, and a discussion of the design goals and the principles used to arrive at a preliminary specification of the accelerator.

 

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TH4PBC01 LNLS-2: A New High Performance Synchrotron Radiation Source for Brazil radiation, synchrotron, brightness, emittance 3166
 
  • P.F. Tavares, J.A. Brum, J.F. Citadini, R.H.A. Farias, J.G.R.S. Franco, L. Liu, S.R. Marques, X.R. Resende, M.C. Rocha, C. Rodrigues, R.M. Seraphim, G. Tosin
    LNLS, Campinas
 
 

We present an overview of a new synchrotron radiation source currently being designed at the Brazilian Synchrotron Light Laboratory (LNLS) in Campinas. The LNLS-1 light source, based on a 1.37 GeV storage ring, has been in routine operation since 1997. The LNLS-2 light source will consist of an injector system and a low emittance 2.5 GeV electron storage ring capable of delivering undulator radiation with average brightness in excess of 1020 photons/sec/0.1%/mm2/mrad2 in the few hundred eV to several tens of keV photon energy range. High flux radiation up to 100 keV will also be available with the use of superconduting wigglers. In this work, we present the basic design considerations and parameters for a proposed magnetic lattice for LNLS-2, with special attention to providing solutions for the realization of low emittance which are cost effective regarding both the construction investment as well as the operation of the facility. In particular, the possibility of the large scale use of permanent magnet technology for the storage ring lattice magnets is discussed.

 

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TH4PBC03 Major Upgrade Activity of the PLS in PAL: PLS-II linac, klystron, storage-ring, injection 3172
 
  • S.H. Nam
    PAL, Pohang, Kyungbuk
 
 

The Pohang Accelerator Laboratory (PAL) celebrated its 20th anniversary this year. After the completion of the Pohang Light Source (PLS) construction in 1994, the PLS started user service with two beamlines in 1995. The PLS energy was 2.0 GeV. The first major upgrade of the PLS had been done from 2000 to 2002, in which operation energy of the PLS was increased from 2.0 GeV to 2.5 GeV. The number of beamlines has been steadily increased since the start of user service. The number of beamlines currently in service is 28. Three beamlines are under construction. Number of users and performed experiments in 2007 were respectively 2553 and 837. Average impact factor of published papers is over 3.0, which is one of the best among Korean research institutes. Based on such success, the PAL is pursuing the second upgrade plan, called the PLS-II. The PLS will be upgraded its energy from 2.5 GeV to 3.0 GeV. With the upgrade, it will be possible to construct ten more insertion devices. The brightness of the PLS-II will be more than a order higher compared to the current PLS. In this presentation, details of the PLS-II project will be introduced.


This work was supported by the MEST (Ministry of Education, Science and Technology) and the POSCO (POhang iron and Steel making COmpany) in Korea.

 

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TH5PFP015 Recent Developments for the HEADTAIL Code: Updating and Benchmarks wakefield, impedance, space-charge, electron 3220
 
  • D. Quatraro, G. Rumolo, B. Salvant
    CERN, Geneva
 
 

The HEADTAIL code models the evolution of a single bunch interacting with a localized impedance source or an electron cloud, optionally including space charge. The newest version of HEADTAIL relies on a more detailed optical model of the machine taken from MAD-X and is more flexible in handling and distributing the interaction and observation points along the simulated machine. In addition, the option of the interaction with the wake field of specific accelerator components has been added, such that the user can choose to load dipolar and quadrupolar components of the wake from the impedance database Z-BASE. The case of a single LHC-type bunch interacting with the realistic distribution of the kicker wake fields inside the SPS has been successfully compared with a single integrated beta-weighted kick per turn. The current version of the code also contains a new module for the longitudinal dynamics to calculate the evolution of a bunch inside an accelerating bucket.

 
TH5PFP033 Touschek Lifetime Measurements at Small Horizontal Emittance in the ALS emittance, scattering, storage-ring, synchrotron 3269
 
  • C. Steier, L. Yang
    LBNL, Berkeley, California
 
 

Funding: This work was supported by the Director, Office of Science, U. S. Department of Energy under Contract No. DE-AC02-05CH11231.


The Touschek lifetime in low energy or small emittance lepton storage rings strongly depends on the particle density in bunches. In the usual parameter range, this dominates other effects and the lifetime gets shorter with higher the bunch density, i.e. with smaller beam emittance. However, once one gets to extremely small horizontal emittances, this is no longer the case. Since the Touschek scattering process is an energy transfer from the transverse plane to the longitudinal one, the Touschek lifetime actually increases, once the transverse temperature (i.e. emittance) gets small enough. In the usual Touschek lifetime formulas, this is accounted for with a complicated multiparameter function (form factor). This paper presents to our knowledge the first direct measurements of the Touschek lifetime in this region of reversed dependence on horizontal emittance, as well as comparison with theory. The measurements were carried out at the ALS at reduced beam energy and ultrasmall horizontal emittance.

 
TH5PFP038 Intrabeam Scattering Effect Calculated for a Non-Gaussian Distributed Linac Beam linac, emittance, scattering, electron 3281
 
  • A. Xiao, M. Borland
    ANL, Argonne
 
 

Funding: Work supported by the U.S. Department of Energy, Office of Science, Office of Basic Energy Sciences, under Contract No. DE-AC02-06CH11357.


A high-brightness electron beam used for linac-based fourth-generation light sources such as X-ray free-electron lasers (FELs) and energy recovery linacs (ERLs) is often non-Gaussian distributed especially in the longitudinal direction. In order to study the intra-beam scattering effect (IBS) in such a beam, we added a slice analysis method to elegant. This paper explains this method and an application result to a possible ERL upgrade of the Advanced Photon Source.

 
TH5PFP040 Optical Matching of EMMA Cell Parameters Using Field Map Sets simulation, closed-orbit, resonance, acceleration 3287
 
  • Y. Giboudot
    Brunel University, Middlesex
  • F. Méot
    CEA, Gif-sur-Yvette
 
 

The Non Scaling FFAG EMMA lattice allows a important displacement of the magnets in the radial direction. From this peculiarity, interesting studies of beam dynamics can be performed comparing simulated and experimental results. Being able to study a specific resonance, choosing a certain set of parameters for the lattice is really challenging. Simulations have been done integrating particle trajectories with Zgoubi through Magnetic Field Map created with OPERA. From a chosen tune evolution, one can find the corresponding magnets' configuration required by interpolating between a various sets of Field Map. Relative position and strength of the magnets are degrees of freedom. However, summing field maps requires a special care since the real magnetic field created by two magnets is not obviously linearly dependent on each single magnet. For this reason, frequently used hard edge and fringe field models may not be accurate enough. This linearity of the magnetic field has been studied directly through OPERA finite element method solutions and further on with Zgoubi tracking results.

 
TH5PFP041 Particle Tracking Studies Using Dynamical Map Created from Finite Element Solution of the EMMA Cell quadrupole, closed-orbit, vacuum, simulation 3290
 
  • Y. Giboudot, A. Khan
    Brunel University, Middlesex
  • T.R. Edgecock
    STFC/RAL, Chilton, Didcot, Oxon
  • A. Wolski
    The University of Liverpool, Liverpool
 
 

The unconventional size and the possibility of transverse displacement of the magnets in the EMMA non-scaling FFAG motivates a careful study of particle behavior within the EMMA ring. The magnetic field map of the doublet cell is computed using a Finite Element Method solver; particle motion through the field can then be found by numerical integration, using (for example) OPERA, or ZGOUBI. However, by obtaining an analytical description of the magnetic field (by fitting a Fourier-Bessel series to the numerical data) and using a differential algebra code, such as COSY, to integrate the equations of motion, it is possible to produce a dynamical map in Taylor form. This has the advantage that, after once computing the dynamical map, multi-turn tracking is far more efficient than repeatedly performing numerical integrations. Also, the dynamical map is smaller (in terms of computer memory) than the full magnetic field map; this allows different configurations of the lattice, in terms of magnet positions, to be represented very easily using a set of dynamical maps, with interpolation between the coefficients in different maps*.


*yoel.giboudot@stfc.ac.uk

 
TH5PFP048 Collimating Touschek Particles in an Energy Recovery Linear Accelerator simulation, scattering, linac, shielding 3309
 
  • M. P. Ehrlichman, G.H. Hoffstaetter
    CLASSE, Ithaca, New York
 
 

Funding: This work was supported by the National Science Foundation.


The theories of beam loss and emittance growth by Touschek and intra-beam scattering formulated for beams in storage rings have recently been extended to linacs. In most linacs, these effects are not relevant, but they become important in Energy Recovery Linacs (ERLs) not only because of their large current, but also because the deceleration of the spent beam increases the relative energy deviation and transverse oscillation amplitude of the scattered particles. In this paper, we describe a methodology for designing a collimator scheme to control where scattered particles are lost. The methodology is based on Touschek particle generation and tracking simulations implemented in {\tt BMAD}, Cornell's beam dynamics code. The simulations give the locations where scattering occurs and the locations where the scattered particles are lost. The simulations are used to determine the trajectory of the scattered particles, which are analyzed to determine optimal locations for collimators.

 
TH5PFP049 Acceleration of Symplectic Integrator with Graphical Processing Units dynamic-aperture, multipole, target, resonance 3312
 
  • J. Rowland, I.P.S. Martin
    Diamond, Oxfordshire
 
 

The study of nonlinear effects in storage rings requires massively parallel particle tracking over a range of initial conditions. Stream processing architectures trade cache size for greatly increased floating point throughput in the case of regular memory access patterns. The symplectic integrator of Tracy-II* has been implemented in CUDA** on the nVidia stream processor and used to calculate dynamic apertures and frequency maps for the Diamond low-alpha lattice. To facilitate integration with existing workflows the the lattice description of Accelerator Toolbox*** is re-used. The new code is demonstrated to achieve a two orders of magnitude increase in tracking speed over a single CPU core and benchmarks of the performance and accuracy against other codes are presented.


*J. Bengtsson, Tracy-2 User's Manual, Feb 1997.
**NVIDIA, NVIDIA_CUDA_Programming_Guide_1.1.pdf
***A. Terebilo - ACCELERATOR MODELING WITH MATLAB ACCELERATOR TOOLBOX, PAC 2001

 
TH5PFP071 Multiobjective Light Source Lattice Optimization brightness, emittance, quadrupole, synchrotron 3365
 
  • L. Yang, D. Robin, F. Sannibale, C. Steier, W. Wan
    LBNL, Berkeley, California
 
 

Funding: Work supported by the Director, Office of Science, U. S. Department of Energy under Contract No. DE-AC02-05CH11231.


Multiobjective optimization has been used in many fields including accelerator related projects. Here we use it as a powerful tool for lattice design and optimization, which includes betatron functions, brightness.

 
TH5PFP072 Simulating an Acceleration Schedule for NDCX-II acceleration, simulation, solenoid, ion 3368
 
  • W. M. Sharp, A. Friedman, D.P. Grote
    LLNL, Livermore, California
  • E. Henestroza, M. Leitner, W.L. Waldron
    LBNL, Berkeley, California
 
 

Funding: Work performed under the auspices of US Department of Energy by LLNL under Contract DE- AC52-07NA27344 and by LBNL under Contract DE-AC03-76SF00098.


The Virtual National Laboratory for Heavy-Ion Fusion is developing a physics design for NDCX-II, an experiment to study warm dense matter heated by ions near the Bragg-peak energy. Present plans call for using about thirty induction cells to accelerate 30 nC of Li+ ions to more than 3 MeV, followed by neutralized drift-compression. To heat targets to useful temperatures, the beam must be compressed to a sub-millimeter radius and a duration of about 1 ns. An interactive 1-D particle-in-cell simulation with an electrostatic field solver, acceleation-gap fringe fields, and a library of realizable analytic waveforms has been used for developing NDCX-II acceleration schedules. Multidimensional source-to-final-focus simulations with the particle-in-cell code Warp have validated this 1-D model and have been used both to design transverse focusing and to compensate for injection non-uniformities and 3-D effects. Results from this work are presented, and ongoing work to replace the analytic waveforms with output from circuit models is discussed.

 
TH5PFP088 HOM Sensitivity in the PEP-II HER Vacuum Chamber HOM, vacuum, synchrotron, synchrotron-radiation 3413
 
  • S.P. Weathersby, A. Novokhatski, M.K. Sullivan
    SLAC, Menlo Park, California
 
 

Funding: Work supported by Department of Energy Contract DE-AC02-76SF00515


Synchrotron radiation is the main source of vacuum chamber heating in the PEP-II storage ring collider. This heating is reduced substantially as lattice energy is lowered. Energy scans over Υ energy states were performed by varying the high energy ring (HER) lattice energy at constant gap voltage and frequency. We observed unexpected temperature rise at particular locations when HER lattice energy was lowered from 8.6 GeV (Υ(3S)) to 8.0 GeV (Υ(2S)) while most other temperatures decreased. Bunch length measurements reveal a shorter bunch at the lower energy. The shortened bunch overheated a beam position monitoring electrode causing a vacuum breach. We explain the unexpected heating as a consequence of increased higher order mode (HOM) power generated by a shortened bunch. In this case, temperature rise helps to identify HOM sources and HOM sensitive vacuum chamber elements. Reduction of gap voltage helps to reduce this unexpected heating.

 
TH5RFP037 On the Continuous Measurement of the LHC Beta-Function - Prototype Studies at the SPS betatron, optics, quadrupole, monitoring 3528
 
  • R.J. Steinhagen, A. Boccardi, E. Calvo Giraldo, M. Gasior, J.L. Gonzalez, O.R. Jones
    CERN, Geneva
 
 

Until now, the continuous monitoring of the LHC lattice has been considered as impractical due to tight constraints on the maximum allowed beam excitations and acquisition time usually required for betatron function measurements. As an further exploitation of the Base-Band-Tune (BBQ) detection principle, already widely used for tune diagnostic, a real-time beta-beat measurement prototype has been successfully tested at the CERN SPS based on the continuous measurement of the cell-to-cell betatron phase advance. Tests show that the phase resolutions is better than a degree corresponding to a peak-to-peak beta-beat resolution of about one percent. Due to the system's high sensitivity it required only micro-metre range excitation, making it compatible with nominal LHC operation. This contribution discusses results, measurement systematics and possible additional exploitation that may be used to improve the nominal LHC performance.

 
TH6PFP002 Beam Dynamics Simulations for CLIC Drive Beam Accelerator linac, quadrupole, simulation, wakefield 3690
 
  • A. Aksoy, O. Yavas
    Ankara University, Faculty of Engineering, Tandogan, Ankara
  • D. Schulte
    CERN, Geneva
 
 

Funding: Turkish Atomic Energy Authority


CLIC study aims at a center-of-mass energy for electron-positron collisions of 3TeV using room temperature accelerating structures at high frequency (12GHz) which are likely to achieve 100 MV/m gradient. Due to conventional high frequency RF sources do not provide sufficient RF power for 100MV/m gradient, CLIC relies upon a two-beam-acceleration concept: The 12GHz RF power is generated by a high current electron beam (Drive Beam) running parallel to the main beam with deceleration in special Power Extraction Structures (PETS) and the generated RF power is transferred to the main beam. In order to obtain very high RF power at 12GHz frequency, injected beam into PETS should have 2.37GeV energy, 101A pulse current and pulse length around 240ns. Drive beam accelerator (DBA) accelerates the beam up to 2.37GeV in almost fully-loaded structures and the pulse after DBA contains more than 70000 bunches, has a length around 140μs and 4.2A pulse current. After some modifications in delay loop and in combiner rings the beam has 101A pulse current and 240ns pulse length. In this study simulations of some transverse beam parameters for different options for the lattice of the DBA are presented.

 
TH6PFP003 A Lattice Study for the Synchrotron Radiation Facility of the Turkish Accelerator Complex (TAC) with 3.56 GeV emittance, storage-ring, synchrotron, quadrupole 3693
 
  • K. Zengin
    Ankara University, Faculty of Sciences, Tandogan/Ankara
 
 

The Turkish Accelerator Complex (TAC) is a project for accelerator based fundamental and applied researches supported by Turkish State Planning Organization (DPT). The proposed complex is consisted of 1 GeV electron linac and 3.56 GeV positron ring for a charm factory and a few GeV proton linac. Apart from the particle factory, it is also planned to produce synchrotron radiation from positron ring. In this study the lattice structure design of the positron storage ring is made to produce the third generation synchroton light. It has been studied with different lattice structures (DBA, TBA, DDBA etc.) for TAC. It has been compared lattice structures and tried to find the best structure for lowest emittance.

 
TH6PFP004 Search for Nonlinear Beam Dynamics Causes of Lifetime Reduction at the APS Storage Ring sextupole, simulation, optics, power-supply 3696
 
  • L. Emery, M. Borland, V. Sajaev, A. Xiao
    ANL, Argonne
 
 

Funding: This work was supported by U.S. Department of Energy, Office of Science, Office of Basic Energy Sciences, under Contract No. DE-AC02-06CHlI357.


During an operating period in which a sextupole unknowingly connected with the wrong polarity resulted in reduced beam lifetime, a list of machine physics experiments and simulations were developed to identify possible gradient errors of one or more sextupole magnets. We tried tune dependence on orbit, response matrix measurements at different momenta, sector-wise chromaticity measurements, empirical search with sextupole harmonics, and guidance from tracking simulations. The practicality of each will be discussed.

 
TH6PFP007 Simulation of Linear Lattice Correction and Coupling Correction of an Energy-Recovery Linac Designed for an APS Upgrade quadrupole, simulation, sextupole, optics 3705
 
  • V. Sajaev
    ANL, Argonne
 
 

Funding: Work supported by the U.S. Department of Energy, Office of Science, Office of Basic Energy Sciences, under Contract No. DE-AC02-06CH11357.


An energy recovery linac (ERL) is one of the candidates for an upgrade of the Advanced Photon Source (APS). In addition to the APS ring and full-energy linac, our design also includes a large turn-around arc that could accommodate new x-ray beamlines as well. In total, the beam trajectory length would be close to 3 km. The ERL lattice has strong focusing to limit emittance growth, and it includes strong sextupoles to keep beam energy spread under control and minimize beam losses. As in storage rings, trajectory errors in sextupoles will result in lattice perturbations that would affect delivered x-ray beam properties. In storage rings, the response matrix fit method is widely used to measure and correct linear lattice errors. Here, we explore the application of the method to the linear lattice correction and coupling correction of an ERL.

 
TH6PFP009 Low Alpha Configuration for Generating Short Bunches storage-ring, synchrotron, single-bunch, quadrupole 3711
 
  • Y.E. Tan, D.R.T. Appadoo, M.J. Boland, R.T. Dowd
    ASCo, Clayton, Victoria
 
 

Generating short bunches for time resolved studies or the generation of THz radiation has been done at many other light sources and is of increasing interest in the user community. Light sources not designed with ps bunchs can usually tune the lattice to reduce ps bunchs without much difficulty, sometimes referred to as a Low Alpha mode. At the Australian light source a low alpha configuration has been investigated. The results looking into the 'shaping' of the momentum compaction factor, beam stability and current limitations will be presented.

 
TH6PFP013 An Injection/Extraction Scenario for EMMA injection, septum, kicker, extraction 3723
 
  • J.S. Berg
    BNL, Upton, Long Island, New York
 
 

Funding: Work Supported by the United States Department of Energy, Contract No. DE-AC02-98CH10886.


EMMA is an experiment to study beam dynamics in a linear non-scaling fixed-field alternating gradient accelerator (FFAG). It accelerates an electron beam from 10 to 20 MeV kinetic energy. To optimally perform these studies, one must be able to inject the beam at any energy within the machine's energy range. Furthermore, because we wish to study the behavior of large-emittance beams in such a machine, the injection systems must be able to inject the beam anywhere within a transverse phase space ellipse with a normalized acceptance of 3 mm, and the extraction systems must be able to extract from that same ellipse. I describe a computation of kicker and septum fields to achieve all of these requirements, and discuss how this interacts with the hardware constraints.

 
TH6PFP016 Numerical Based Linear Model for Dipole Magnets dipole, optics, focusing, quadrupole 3732
 
  • Y. Li, S. Krinsky, M. Rehak
    BNL, Upton, Long Island, New York
 
 

Funding: Work supported by U.S. DOE, Contract No.DE-AC02-98CH10886


In this paper, we discuss an algorithm for constructing a numerical linear optics model for dipole magnets from a 3D field map. The difference between the numerical model and K. Brown’s analytic approach is investigated and clarified. It was found that the optics distortion due to the dipoles’ fringe focusing must be properly taken into account to accurately determine the chromaticities. In NSLS-II, there are normal dipoles with 35-mm gap and dipoles for infrared sources with 90-mm gap. This linear model of the dipole magnets is applied to the NSLS-II lattice design to match optics parameters between the DBA cells having dipoles with different gaps.

 
TH6PFP017 Simulations on the AGS Horizontal Tune Jump Mechanism resonance, emittance, polarization, simulation 3735
 
  • F. Lin, H. Huang, A.U. Luccio, T. Roser
    BNL, Upton, Long Island, New York
 
 

Funding: Work supported by Brookhaven Science Associates, LLC under Contract No. DE-AC02-98CH10886 with the U.S. Department of Energy.


A new horizontal tune jump mechanism has been proposed to overcome the horizontal intrinsic resonances and preserve the polarization of the proton beam in the AGS during the energy ramp. An adiabatic change of the AGS lattice is needed to avoid the emittance growth in both horizontal and vertical motion, as the emittance growth can deteriorate the polarization of the proton beam. Two critical questions are necessary to be answered: how fast can the lattice be changed and how much emittance growth can be tolerated from both optics and polarization points of view? Preliminary simulations, using a realistic AGS lattice and acceleration rate, have been carried out to give a first glance of this mechanism. Several different conditions are presented in this paper.

 
TH6PFP022 An FFAG Transport Line for the PAMELA Project emittance, closed-orbit, resonance, focusing 3741
 
  • R.J.L. Fenning, A. Khan
    Brunel University, Middlesex
  • T.R. Edgecock
    STFC/RAL, Chilton, Didcot, Oxon
  • D.J. Kelliher, S. Machida
    STFC/RAL/ASTeC, Chilton, Didcot, Oxon
  • K.J. Peach, T. Yokoi
    JAI, Oxford
 
 

The PAMELA project to design an accelerator for hadron therapy using non-scaling Fixed Field Alternating Gradient (NS-FFAG) magnets requires a transport line and gantry to take the beam to the patient. The NS-FFAG principle offers the possibility of a gantry much smaller, lighter and cheaper than conventional designs, with the added ability to accept a wide range of fast changing energies. This paper will build on previous work to investigate a transport line which could be used for the PAMELA project. The design is presented along with a study and optimisation of its acceptance.

 
TH6PFP027 ALBA Booster Settings for an Optimized Performance dipole, sextupole, quadrupole, dynamic-aperture 3756
 
  • G. Benedetti, D. Einfeld, J. Marcos, M. Muñoz, M. Pont
    CELLS-ALBA Synchrotron, Cerdanyola del Vallès
 
 

The ALBA booster is a 100 MeV-3 GeV ramping synchrotron, with large circumference of 249.6 m and low emittance of 9nm*rad, cycling at 3 Hz. The lattice consists of a 4-fold symmetric modified FODO lattice with defocusing gradient dipoles. Magnetic measurements on all magnets have been performed: the studies and lattice settings to recover the design optics preserving good machine performances, such as the lattice flexibility, the low beta functions and large dynamic aperture at high chromaticities, are presented.

 
TH6PFP032 A Low Momentum Compaction Lattice for the Diamond Storage Ring storage-ring, electron, synchrotron, emittance 3769
 
  • I.P.S. Martin, J. Rowland, B. Singh, C.A. Thomas
    Diamond, Oxfordshire
  • R. Bartolini, I.P.S. Martin
    JAI, Oxford
 
 

With the aim of generating short pulse radiation, a low momentum compaction lattice has recently been commissioned for the Diamond storage ring. By introducing both positive and negative dispersion in the bending magnets it has been possible to operate the storage ring in a quasi-isochronous state, resulting in a natural electron bunch length of less than 1 pico-second. A description of the techniques used to develop the lattice is given, along with first results obtained during recent machine trials. Operation with both positive and negative momentum compaction factor is also described

 
TH6PFP036 Lattice Issues of the CERN PSB with H- Charge Exchange Injection Hardware injection, quadrupole, linac, betatron 3781
 
  • C. Carli, M. Aiba, M. Chanel, B. Goddard, M. Martini, W.J.M. Weterings
    CERN, Geneva
 
 

The motivation for the construction of CERN Linac4 is to improve the performance of the PSB by raising the injection energy and implementing a new H- charge exchange multiturn injection scheme. Strategies to design the H- charge exchange injection hardware and, in particular, to mitigate perturbations of the lattice will be reported and the proposed geometry described.

 
TH6PFP047 CLIC Main Beam Dynamics in the Ring to Main Linac Transport linac, wakefield, emittance, simulation 3814
 
  • F. Stulle, L. Rinolfi, D. Schulte
    CERN, Geneva
  • A. Ferrari
    Uppsala University, Uppsala
  • A. Latina
    Fermilab, Batavia
 
 

Prior to acceleration in the main linac, the particle beams created in the centrally located injector have to be transported to the outer ends of the CLIC site. This transport should not only preserve the beam quality but also shape, characterize and tune the phase space distribution to match the requirements at the entrance of the main linac. Hence, the performance of the transport downstream of the damping rings up to the main linac, the so called RTML, is crucial for the overall performance of CLIC. The RTML consists of a variety of components like bunch compressors, accelerating cavities, spin rotators, collimators, diagnostics sections, feedback and feedforward systems, each serving a distinct function. We discuss the different parts of the RTML and the beam dynamics challenges connected to them. Their status is outlined and results of beam dynamics simulations are presented.

 
TH6PFP051 Muon Collider Lattice with Local Interaction Region Chromaticity Correction dipole, sextupole, collider, quadrupole 3820
 
  • Y. Alexahin, E. Gianfelice-Wendt
    Fermilab, Batavia
 
 

Funding: Fermi Research Alliance, LLC under Contract No. DE-AC02-07CH11359 with the United States Department of Energy.


Muon collider is a promising candidate for the next energy frontier machine. In order to obtain peak luminosity of the order of 1035/cm2/s in the TeV energy range the beta function at the interaction point should be smaller than 1cm. To obtain correspondingly small bunch length with a reasonable RF voltage (within 1GV) the momentum compaction factor should be smaller than 10-4 in the momentum range ~1%. The lattice design must also provide sufficient dynamic aperture for ~20 microns normalized beam emittance and minimum possible circumference. Together these requirements present a challenge which has never been met before. We offer a solution to this problem which has the following distinctive features: i) chromatic compensation achieved with sextupoles and dispersion generating dipoles placed near the IR quadrupoles (not in a special section), ii) low value of momentum compaction factor obtained by balancing positive contribution from the arcs with negative contribution from the suppressors of the generated in the IR dispersion. Theoretical aspects and various options will be discussed.

 
TH6PFP052 A Simple Transition-Free Lattice of an 8 GeV Proton Synchrotron sextupole, synchrotron, proton, dipole 3823
 
  • W. Chou
    Fermilab, Batavia
 
 

Funding: Work supported by the Fermi Research Alliance, LLC under contract No. DE-AC02-07CH11359 with the U.S. Dept. of Energy.


A transition-free lattice is a basic requirement of a high-intensity medium-energy (several GeV) proton synchrotron in order to eliminate beam losses during transition crossing. An 8 GeV synchrotron is proposed as a principal component in an alternative hybrid design of Project-X. This machine would be housed in the Fermilab antiproton source enclosure replacing the present Debuncher. A simple doublet lattice with high transition gamma has been designed. It uses just one type of dipoles and one type of quadrupoles (QF and QD are of the same length). It has no transition crossing. It has a triangular shape with three zero dispersion straight sections, which can be used for injection, extraction, RF and collimators. The beta-functions and dispersion are low. This lattice has plenty of free space for correctors and diagnostic devices, as well as good optical properties including large dynamic aperture, weak dependence of lattice functions on amplitude and momentum deviation.


*W. Chou, “An Alternative Approach to Project X,” this conference.

 
TH6PFP053 Linear and Nonlinear Beam Optics Studies in the SIS18 sextupole, simulation, optics, closed-orbit 3826
 
  • A.S. Parfenova, G. Franchetti
    GSI, Darmstadt
 
 

The GSI heavy ion synchrotron SIS18 will be used as a booster for the SIS100 synchrotron of the new FAIR facility. The linear corrections and measurements are a necessary step before the nonlinear field errors can be applied. A tune response to a change in a sextupole magnet strength for a certain Closed Orbit (CO) deformation is used to verify beta-functions of the SIS18 model at the location of the ring's sextupoles for chromaticity correction. The progress in development of Nonlinear Tune Response Matrix (NTRM) technique to diagnose nonlinear field components is presented.

 
TH6PFP060 Touschek Background and Lifetime Studies for the SuperB Factory simulation, background, coupling, emittance 3844
 
  • M. Boscolo, M.E. Biagini, P. Raimondi
    INFN/LNF, Frascati (Roma)
  • E. Paoloni
    University of Pisa and INFN, Pisa
  • M.K. Sullivan
    SLAC, Menlo Park, California
 
 

The novel crab waist collision scheme under test at the DAΦNE Frascati phi-factory finds its natural application to the SuperB project, the asymmetric e+e- flavour factory at very high luminosity with low beam currents and reduced background possibly located at Tor Vergata University. The SuperB accelerator design requires a careful choice of beam parameters to reach a good trade-off between different effects. We present here simulation results for the Touschek backgrounds and lifetime obtained for the latest machine design. Distributions of the Touschek particle losses at the at the interaction region have been tracked into the detectors for further investigations. A set of collimators is foreseen to stop Touschek particles. Their position along the rings has also been studied, together with their shape optimization.

 
TH6PFP062 Direct Methods of Optimization of Storage Ring Dynamic and Momentum Aperture sextupole, dynamic-aperture, emittance, synchrotron 3850
 
  • M. Borland, L. Emery, V. Sajaev, A. Xiao
    ANL, Argonne
 
 

Funding: Work supported by the U.S. Department of Energy, Office of Science, Office of Basic Energy Sciences, under Contract No. DE-AC02-06CH11357.


Optimization of dynamic and momentum aperture is one of the most challenging problems in storage ring design. For storage-ring-based x-ray sources, large dynamic aperture is sought primarily to obtain high injection efficiency, which is important in efficient operation but also in protecting components from radiation damage. X-ray sources require large momentum aperture in order to achieve workable Touschek lifetimes with low emittance beams. The most widely applied method of optimizing these apertures is to minimize the driving terms of various resonances. This approach is highly successful, but since it is based on perturbation theory, it is not guaranteed to give the best result. In addition, the user must somewhat arbitrarily assign weights to the various terms. We have developed several more direct methods of optimizing dynamic and momentum aperture. These have been successfully applied to operational and design problems related to the Advanced Photon Source and possible upgrades.

 
TH6PFP064 Touschek Lifetime Calculations for NSLS-II scattering, multipole, closed-orbit, damping 3853
 
  • B. Nash, S.L. Kramer
    BNL, Upton, Long Island, New York
 
 

The Touschek effect limits the lifetime for NSLS-II. The basic mechanism is Coulomb scattering resulting in a longitudinal momentum outside the momentum aperture. The momentum aperture results from a combination of the initial betatron oscillations after the scatter and the non-linear properties determining the resultant stability. We find that higher order multipole errors may reduce the momentum aperture, particularly for scattered particles with energy loss. The resultant drop in Touschek lifetime is minimized, however, due to less scattering in the dispersive regions. We describe these mechanisms, and present calculations for NSLS-II using a realistic lattice model including damping wigglers and engineering tolerances.

 
TH6PFP065 Impact of Higher-Order Multipole Errors in the NSLS-II Quadrupoles and Sextupoles on Dynamic and Momentum Aperture multipole, dynamic-aperture, quadrupole, sextupole 3856
 
  • B. Nash, W. Guo
    BNL, Upton, Long Island, New York
 
 

Successful operation of NSLS-II requires sufficient dynamic aperture for injection, as well as momentum aperture for Touschek lifetime. We explore the dependence of momentum and dynamic aperture on higher-order multipole field errors in the quadrupoles and sextupoles. We add random and systematic multipole errors to the quadrupoles and sextupoles and compute the effect on dynamic aperture. We find that the strongest effect is at negative momentum, due to larger closed orbit excursions. Adding all the errors based on the NSLS-II specifications, we find adequate dynamic and momentum aperture.

 
TH6PFP070 Effect of the Measured Magnetic Multipoles in the ALBA Lattice multipole, sextupole, dynamic-aperture, quadrupole 3868
 
  • M. Muñoz, D. Einfeld, Z. Martí
    CELLS-ALBA Synchrotron, Cerdanyola del Vallès
 
 

The Spanish synchrotron light source ALBA is in the process of installation, with the large majority of components already manufactured and delivered. Among them, the magnets of the storage ring. As part of the acceptance process of the magnets, a campaign to measure the quality of them (magnetic length, effective bending and focusing, high order multipolar components) has been performed in-house and in the manufacturer. The results of this measures have been applied to the model of the storage ring, analyzing the effects in the performance (lifetime, dynamic aperture, orbit, etc). The results of the study confirm the quality of the magnet's design and manufacturing as well as the performance of the lattice.

 
TH6PFP078 Stability Boundary of Ion Beams in the FAIR Storage Rings sextupole, storage-ring, quadrupole, antiproton 3886
 
  • A. Dolinskyy, C. Dimopoulou, O.E. Gorda, S.A. Litvinov, F. Nolden, C. Peschke, M. Steck
    GSI, Darmstadt
 
 

The FAIR Storage Rings (CR, RESR and NESR) are designed for efficient cooling, accumulation, deceleration and performing nuclear physics experiments with antiproton and rare isotopes beams. Tracking studies for all these rings have been performed to estimate the dynamic aperture and other properties of beam stability depending on the low and high field multipole components, fringe fields and field interference. The multipole limits have to be determined in order to provide a reasonable estimate of the stability boundary and needed correction of the low field multipoles. We report on quantitative studies of the effects of multipoles on the dynamic aperture of the rings, and show that the systematic multipole components in the present magnet designs are unlikely to impose a severe limitation.

 
TH6PFP084 Experimental Frequency Map Analysis Using Multiple BPMs damping, closed-orbit, storage-ring, simulation 3898
 
  • C. Steier, L. Yang
    LBNL, Berkeley, California
 
 

Funding: This work was supported by the Director, Office of Science, U. S. Department of Energy under Contract No. DE-AC02-05CH11231.


Frequency map analysis is being widely used, nowadays, both in simulations to design or improve accelerator lattices, as well as in experiments to study the transverse nonlinear dynamics in accelerators. A significant challenge to the use of frequency map analysis in experiments is the usually very fast decoherence of transverse oscillations, caused by the large nonlinearities of state-of-the-art lattices. Due to the decoherence, the center of mass oscillations of bunches often disappear in less than 100 turns. A potential way to get around this limitation is the use of multiple BPMs distributed (symetrically) around the storage ring. The presentation will describe the challenges multi-BPM frequency map analysis poses as well as initial results using the ALS.

 
TH6PFP086 Single Particle Dynamics in the University of Maryland Electron Ring electron, simulation, space-charge, injection 3904
 
  • E.W. Nissen, B. Erdelyi
    Northern Illinois University, DeKalb, Illinois
  • S. Bernal, D.F. Sutter
    UMD, College Park, Maryland
 
 

We undertake a study of the single particle dynamics in a model of the University of Maryland Electron Ring. This accelerator uses a low energy electron beam to study the effects of space charge on beam dynamics. However, due to this low energy, other effects that are seldom taken into account in high energy accelerators become important to the single particle dynamics of the beam. The simulation is performed using COSY Infinity, which has the effects of the earth’s magnetic field added to it. When the simulated trajectories are compared to measured beam positions there is good agreement through the ninth section of the ring, at which point the difference between predicted and observed diverges. A method of calculating map elements corresponding to the measured data will be used to determine where issues with the ring that could cause these problems might be found.

 
TH6PFP088 Integrable Accelerator Lattices with Periodic and Exponential Invariants SRF, betatron, resonance, damping 3910
 
  • V.V. Danilov
    ORNL, Oak Ridge, Tennessee
 
 

Funding: SNS is managed by UT-Battelle, LLC, for the U. S. Department of Energy under Contract No. DE-AC05-00OR22725.


The paper presents a new variety of one-dimensional nonlinear integrable accelerator lattices with periodic and exponential invariants in coordinates and momenta. Extension to two-dimensional transverse motion, based on a recently published approach*, is discussed.


*V. Danilov, “Practical Solutions for Nonlinear Accelerator Lattice with Stable Nearly Regular Motion”, Phys. Rev. ST AB 11, 114001 (2008)

 
TH6PFP090 Adiabatic Formation and Properties of a Quasi-Equilibrium Beam Distribution Mathced to a Periodic Focusing Lattice focusing, quadrupole, simulation, vacuum 3916
 
  • M. Dorf, R.C. Davidson, H. Qin, E. Startsev
    PPPL, Princeton, New Jersey
 
 

Funding: Research supported by the U.S. Department of Energy.


This paper reports on recent advances in the development of a numerical scheme for describing the quiescent loading of a quasi-equilibrium beam distribution matched to a periodic focusing lattice*. The scheme allows for matched-beam distribution formation by means of the adiabatic turn-on of the oscillating focusing field, and it is examined here for the cases of alternating-gradient quadrupole and periodic solenoidal lattices. Furthermore, various distributions are considered for the initial beam equilibrium. The self-similar evolution of the matched-beam density profile is observed for arbitrary choice of initial distribution function and lattice type. The numerical simulations are performed using the WARP particle-in-cell code.


* M.Dorf et al., Phys. Rev. ST Accel. Beams, submitted for publication(2009).

 
TH6PFP091 Non-Commutative Courant-Snyder Theory for Coupled Transverse Dynamics of Charged Particles in Electromagnetic Focusing Lattices transverse-dynamics, quadrupole, focusing, coupling 3919
 
  • H. Qin, R.C. Davidson
    PPPL, Princeton, New Jersey
 
 

Funding: Supported by the U.S. Department of Energy.


Courant-Snyder (CS) theory is generalized to the case of coupled transverse dynamics with two degree of freedom. The generalized theory has the same structure as the original CS theory for one degree of freedom. The four basic components of the original CS theory, i.e., the envelope equation, phase advance, transfer matrix, and the CS invariant, all have their counterparts, with remarkably similar formal expressions, in the generalized theory presented here. The unique feature of the generalized CS theory is the non-commutative nature of the theory. In the generalized theory, the envelope function is generalized into an envelope matrix, and the envelope equation becomes a matrix envelope equation with matrix operations that are not commutative. The generalized theory gives a new parameterization of the 4D symplectic transfer matrix that has the same structure as the parameterization of the 2D symplectic transfer matrix in the original CS theory.

 
TH6PFP092 Super-B LER Dynamic Aperture Study and Optimization sextupole, dynamic-aperture, quadrupole, octupole 3922
 
  • P.A. Piminov, A.V. Bogomyagkov, E.B. Levichev
    BINP SB RAS, Novosibirsk
  • M.E. Biagini, P. Raimondi, M. Zobov
    INFN/LNF, Frascati (Roma)
 
 

A project of the SuperB Factory in Italy with the crab-waist collision scheme and extremely large luminosity addresses new challenges to the nonlinear beam dynamics study. Among these challenges are: low emittance lattice requiring strong sextupoles for chromatic correction, sub-mm vertical betatron function at the IP, crab sextupoles placed at both sides from the IP, etc. In this report we describe the results of the DA limiting sources analysis and optimization of the arrangement of the IR and Crab sextupoles and octupoles for the Low Energy Ring (LER).

 
TH6PFP095 Linear and Non-Linear Model Optimisation for SOLEIL Storage Ring coupling, quadrupole, sextupole, simulation 3931
 
  • M.-A. Tordeux, P. Brunelle, A. Loulergue, A. Nadji, L.S. Nadolski
    SOLEIL, Gif-sur-Yvette
 
 

SOLEIL, the French 2.75 GeV third generation synchrotron light source, was commissioned 3 years ago. Thanks to beam-based measurements, the theoretical model of the storage ring lattice model has been improved. First, the quadrupole lengths in the hard edge model were finely tuned to get good agreement with the experimental measurements of betatron tunes for different optics. Second, the non-linear model was modified to better fit with beam-based on-momentum frequency map measurements. A thick sextupole model has been introduced in addition to the non-linear effect of the fringe field in quadrupoles. Simulated and measured tune shifts with transverse amplitudes are then compared. Finally a coupled machine model has been built thanks to crosstalk closed orbit acquisitions. A comparison with another model which is based on turn by turn beam position monitor data is presented. As a validation check, the coupling effect of the 10 m long HU640 undulator is evaluated through these coupled models.

 
TH6REP065 Commissioning of the Bunch-to-Bunch Feedback System at the Advanced Photon Source pick-up, feedback, emittance, betatron 4102
 
  • C. Yao, N.P. Di Monte, W.E. Norum, V. Sajaev, H. Shang
    ANL, Argonne
 
 

Funding: Work supported by U.S. Department of Energy, Office of Science, Office of Basic Energy Sciences, under Contract No. DE-AC02-06CH11357.


The Advanced Photon Source storage ring has several bunch fill patterns for user operation. In some fill patterns the single-bunch beam charge is as high as 16 mA. We installed a bunch-to-bunch feedback system that aims to overcome high-charge beam instability and reduce the required chromatic correction. Due to the drive strength limitation, we decided to first commission the feedback system in the vertical plane. We present our preliminary results, some of the issues that we have experienced and resolved, and our plan to expand the system to the horizontal plane.

 
FR5PFP001 PAMELA: Lattice Design and Performance alignment, proton, betatron, acceleration 4302
 
  • S.L. Sheehy, K.J. Peach, H. Witte, T. Yokoi
    JAI, Oxford
  • D.J. Kelliher, S. Machida
    STFC/RAL/ASTeC, Chilton, Didcot, Oxon
 
 

PAMELA (Particle Accelerator for MEdicaL Applications) is a design for a non-scaling Fixed Field Alternating Gradient accelerator facility for Charged Particle Therapy, using protons and light ions such as carbon to treat certain types of cancer. A lattice has been designed which constrains the variation of betatron tunes through acceleration and thus avoids integer resonance crossing and beam blow-up. This paper outlines the design and performance of this proposed PAMELA lattice.

 
FR5PFP003 Harmonic Number Jump Acceleration in Scaling FFAG Ring cavity, acceleration, emittance, insertion 4308
 
  • Y. Mori
    KEK, Ibaraki
  • T. Planche
    KURRI, Osaka
 
 

Harmonic number jump (HNJ) acceleration in scaling FFAG accelerator, especially for muon acceleration in neutrino factory, has been studied. Criterions for HNJ acceleration were clarified and beam tracking simulations have been carried out.

 
FR5PFP007 Analytic Solution of the Envelope Equations for an Undepressed Matched Beam in a Quadrupole Doublet Channel focusing, space-charge, quadrupole, beam-transport 4320
 
  • O.A. Anderson
    LBNL, Berkeley, California
  • L.L. LoDestro
    LLNL, Livermore, California
 
 

Funding: Supported in part by the U.S. Department of Energy under Contract No. DE-AC02-05CH11231.


In 1958, Courant and Snyder analyzed the problem of alternating-gradient beam transport and treated a model without focusing gaps or space charge.* We extend their work to include the effect of gaps (still neglecting space charge) and obtain exact solutions for the matched envelopes.** We assume a periodic lattice of quadrupole doublets. The focus sections have piecewise-constant field strength and equal lengths, but the zero-field drift sections have arbitrary length ratio. We obtain and show the exact envelope results as functions of z for various field strengths, occupancies (eta), and gap-length ratios. We show the peak envelope excursion as a function of field strength or phase advance (σ) for various cases. There is a broad σ range over which the minimum peak varies less than ± 1%. For eta = 1, this range is 64 to 98 degrees; for eta = 0.5, it is 62 to 96 degrees. In the lowest stable band, the optimum field strength rises by 37.6% when eta is reduced from 1.0 to 0.5 and rises by 76.0% if also one gap has zero length. In the second stable band, the higher field strength accentuates the remarkable compression effect predicted for the FD (gapless) model.**


*E.D. Courant and H.S. Snyder, Ann. Phys. 3, 1 (1958).
**The present work extends a recent envelope analysis carried out without gaps (O.A. Anderson and L.L. LoDestro, submitted to Phys. Rev. ST-AB).

 
FR5PFP008 A Statistical Study of Beam Centroid Oscillations in a Solenoid Transport Channel solenoid, dipole, alignment, focusing 4323
 
  • S.M. Lund, J.E. Coleman, S.M. Lidia, P.A. Seidl, C.J. Wootton
    LBNL, Berkeley, California
 
 

Funding: This research was performed under the auspices of the U.S. DOE at the Lawrence Livermore and Lawrence Berkeley National Laboratories under Contracts No. DE-AC52-07NA27344 and No. DE-AC02-05CH11231.


A recent theory in Ref. * analyzes small-amplitude oscillations of the transverse beam centroid (center of mass) in solenoidal transport channels. This theory employs a transformation to a rotating Larmor frame to simply express the centroid response to mechanical misalignments (transverse center displacements and tilts about the of the longitudinal axis of symmetry) of the solenoid and initial centroid errors. The centroid evolution is expressed in terms of a superposition of the centroid evolving in the ideal aligned system plus an expansion in terms of "alignment functions" that are functions of only the ideal lattice with corresponding amplitudes set by the solenoid misalignment parameters. This formulation is applied to analyze statistical properties of beam centroid oscillations induced by solenoid misalignments. Results are compared to experiments at the NDCX experiment at the LBNL. It is found that contributions to oscillation amplitudes from tilts are significantly larger than contributions from offsets for expected parameters. Use of the formulation to optimally steer the centroid back on-axis with limited diagnostic measurements is also discussed.


* S.M. Lund, C.J. Wootton, and E.P. Lee, "Transverse centroid oscillations in solenoidally focused beam transport lattices," accepted for publication, Nuc. Inst. Meth. A.

 
FR5PFP010 Using Novel Injection Schemes for Enhanced Storage Ring Performance injection, brightness, insertion, insertion-device 4326
 
  • D. Robin, C. Steier, L. Yang
    LBNL, Berkeley, California
 
 

Funding: Supported by DOE BES contract DE-AC03-76SF00098.


Recently there has been a proposal to use pulsed high order multipole elements for injection. One of the advantages of this proposed injection scheme would be that it would be less disruptive to the stored beam and thus advantageous for Top-off operation. In addition to Top-off, such novel injectors might open the door to operating storage rings in more desirable lattice settings. In this paper we will explore some of the possibilities for taking advantage of high order multipole pulsed kick injection.

 
FR5PFP013 An Update of the USR Lattice: Towards a True Multi-User Experimental Facility extraction, quadrupole, storage-ring, antiproton 4335
 
  • A.I. Papash
    MPI-K, Heidelberg
  • C.P. Welsch
    Cockcroft Institute, Warrington, Cheshire
 
 

Funding: Work supported by the Helmholtz Association of National Research Centers (HGF) under contract number VH-NG-328 and GSI Helmholtzzentrum für Schwerionenforschung GmbH


In the future Facility for Low-energy Antiproton and Ion Research (FLAIR) at GSI, the Ultra-low energy electrostatic Storage Ring (USR) will provide cooled beams of antiprotons and possibly also highly charged ions down to energies of 20 keV/q. A large variety of the envisaged experiments demands a very flexible ring lattice to provide a beam with variable cross section, shape and time structure, ranging from ultra-short pulses to coasting beams. The preliminary design of the USR worked out in 2005 was not optimized in this respect and had to be reconsidered. In this contribution we present the final layout of the USR with a focus on its “split-achromat” geometry, the combined fast/slow extraction, and show the different modes of operation required for electron cooling, internal experiments, or beam extraction. We finally give a summary of the machine parameters and the layout of the optical elements.

 
FR5PFP019 Generalized Kapchinskij-Vladimirskij Solution for Wobbling and Tumbling Beams in a Solenoidal Focusing Lattice with Transverse Deflecting Plates target, focusing, space-charge, quadrupole 4347
 
  • H. Qin, R.C. Davidson
    PPPL, Princeton, New Jersey
 
 

Funding: Supported by the U.S. Department of Energy.


For applications of high-intensity beams in heavy ion inertial confinement fusion and high energy density physics, solenoidal focusing lattice and transverse wobblers can be used to achieve uniform illumination of the target and for suppressing deleterious instabilities. A generalized self-consistent Kapchinskij-Vladimirskij solution of the nonlinear Vlasov-Maxwell equations is derived for high-intensity beams in a solenoidal focusing lattice with transverse wobblers. The cross-section of the beam is an ellipse with dynamical centroid, titling angle, and transverse dimensions that are determined from 5 envelope-like equations.

 
FR5PFP025 Extending the Energy Range of 50Hz Proton FFAGs closed-orbit, proton, cavity, acceleration 4357
 
  • S.J. Brooks
    STFC/RAL/ASTeC, Chilton, Didcot, Oxon
 
 

Using an FFAG for rapid-cycling proton acceleration has the advantage that the acceleration cycle is no longer subject to constraints from the main magnet power supply used in an RCS. The RF can be used to its maximum potential to increase the energy range in a short 50Hz cycle as proposed for multi-MW proton driver projects. The challenge becomes an optical one of maintaining a stable lattice across a wide range of beam momenta without magnet sizes or the ring circumference making the machine prohibitively expensive for its purpose. Investigations of stable energy ranges for proton FFAG lattices in the few GeV regime (relativistic but not ultra-relativistic) are presented here.

 
FR5PFP029 Storage Ring Beam Dynamics Modeling with Limited Instrumentation quadrupole, betatron, storage-ring, emittance 4369
 
  • C. Kwankasem, S. Chunjarean
    SLRI, Nakhon Ratchasima
 
 

For the SIAM Photon Source, we propose to establish a storage ring model based on quadrupole fitting of the measured betatron functions. By fitting of quadrupole field strength parameters to measured values of the betatron function, a series of problems at the SIAM Photon Source could be determined. For example, the problem of turn-to turn electrical coil shorts was detected and solved by replacing the new quadrupole coils. Subsequently, we could identify a quadrupole calibration error due to conflicting information on the number of turns per coil. Other causes regarding the beam dynamics model such as high field saturation effects, power supply calibration error, and proximity to nearby magnets have been taken into account to establish accurate quadrupole calibration factors. The establishment of an accurate model is essential for beam dynamics predictions, closed orbit correction, response matrix determination for LOCO, low emittance operation, and optics correction for high filed insertion devices.

 
FR5PFP034 Optical Stochastic Cooling in a Low Energy Electron Storage Ring for a Compact X-Ray Source electron, storage-ring, insertion, emittance 4378
 
  • P.-CH. Yu, W.-H. Huang, X. Shen, C.-X. Tang
    TUB, Beijing
 
 

Funding: This work is supported by National Natural Science Foundation of China (Project 10735050) and National Basic Research Program of China (973 Program) (Grant No. 2007CB815102).


The feasibility study of optical stochastic cooling (OSC) utilizing a compact storage ring is presented in this paper. We present the general layout of the scheme, as well as the lattice design of the storage ring. The results of beam dynamics simulation are likewise presented.

 
FR5PFP038 Possible Emittance Growth due to Nonuniform Particle Distribution in Beams with Thermal Equilibrium Condition emittance, space-charge, simulation, plasma 4390
 
  • T. Kikuchi
    Nagaoka University of Technology, Nagaoka, Niigata
  • K. Horioka
    TIT, Yokohama
 
 

Possible emittance growth due to a nonuniform particle distribution can be analyzed with a thermal equilibrium state in various space-charge potential beams. The possible emittance growth is given by a function of a space-charge tune depression and a nonlinear field energy factor. The nonlinear field energy factor, which is determined by nonuniformity of a charge distribution, is estimated in the thermal equilibrium distribution on a cross-section in a beam. The nonlinear field energy factor changes with space-charge potential for the thermal equilibrium distribution. It is expected that the possible emittance growth will be decreased effectively to consider in the thermal equilibrium condition.

 
FR5PFP042 Approximate Matched Solution for an Intense Charged Particle Beam Propagating through a Periodic Focusing Quadrupole Lattice focusing, quadrupole, transverse-dynamics, plasma 4402
 
  • E. Startsev, R.C. Davidson, M. Dorf
    PPPL, Princeton, New Jersey
 
 

Funding: Research supported by the U. S. Department of Energy.


The transverse dynamics of an intense charged particle beam propagating through a periodic quadrupole focusing lattice is described by the nonlinear Vlasov-Maxwell system of equations where the propagating distance plays the role of time. To find matched-beam quasi-equilibrium distribution functions one need to determine a dynamical invariant for the beam particle moving in the combined external and self-fields. The standard approach for sufficiently small phase advance is to use the smooth focusing approximation, where particle dynamics is determined iteratively using the small parameter (vacuum phase advance)/(360 degrees) < 1 accurate to cubic order. In this paper, we present a perturbative Hamiltonian transformation method which is used to transform away the fast particle oscillations and obtain the average Hamiltonian accurate to 5th order in the expansion parameter. This average Hamiltonian, expressed in the original phase-space variables, is an approximate invariant of the original system, and can be used to determine self-consistent beam equilibria that are matched to the focusing channel.

 
FR5PFP061 Matching and Injection of Beams with Space Charge into the University of Maryland Electron Ring (UMER) injection, solenoid, quadrupole, emittance 4449
 
  • R.A. Kishek, B.L. Beaudoin, S. Bernal, M. Cornacchia, I. Haber, P.G. O'Shea, M. Reiser, D.F. Sutter, J.C.T. Thangaraj, C. Wu
    UMD, College Park, Maryland
  • D. Stratakis
    BNL, Upton, Long Island, New York
 
 

Funding: This work is funded by the US Dept. of Energy Offices of High Energy Physics and High Energy Density Physics, and by the US Dept. of Defense Office of Naval Research and Joint Technology Office


Beam matching is critical for avoiding envelope mismatch oscillations that can lead to emittance growth and halo formation, especially if the beam has significant space charge. The University of Maryland Electron Ring (UMER) is a research storage ring that is designed for scaled studies that are applicable to many larger machines. Using 10 keV electron beams at relatively high current (0.6 – 100 mA), space charge forces are relatively strong. Matching of the UMER beam is rendered difficult by the space charge, the crowdedness of the lattice, and especially the unique injection scheme where an offset oversized quadrupole is shared between the ring and the injector. In this paper we discuss several schemes for optimizing the matching at injection, both analytical and beam-based, which we test using particle-in-cell simulations with the code, WARP. Comparison to UMER experimental data is provided where available.

 
FR5PFP066 A User-Friendly Code to Model Radiation of High Brightness Beams radiation, simulation, diagnostics, brightness 4464
 
  • G. Andonian, M. Ruelas
    RadiaBeam, Marina del Rey
  • S. Reiche
    UCLA, Los Angeles, California
 
 

The accelerator community has many codes that model beams and emitted radiation. Many of these codes are specialized and often, as in start-to-end simulations, multiple codes are employed in subsequent fashion. One of the most important goals of simulations is to accurately model beam parameters and compare results to those obtained from real laboratory diagnostics. This paper describes the development of a user-friendly code that models the coherent radiation of high brightness beams, with a heavy emphasis on simulation of observables via laboratory diagnostics.

 
FR5PFP072 Command Line Interface to Tracy Library insertion, multipole, insertion-device, wiggler 4476
 
  • B. Nash
    SLAC, Menlo Park, California
 
 

We describe a set of tools that interface to the Tracy particle tracking library. The state of the machine including misalignments, multipole errors and corrector settings is captured in a 'flat' file, or 'machine' file. There are three types of tools designed around this flat file: 1) flat file creation tools. 2) flat file manipulation tools. 3) tracking tools. We describe the status of these tools, and give some examples of how they have been used in the design process for NSLS-II.

 
FR5RFP003 Optimization of a Truncated Photonic Crystal Cavity for Particle Acceleration cavity, higher-order-mode, simulation, acceleration 4541
 
  • C.A. Bauer, J.R. Cary, G.R. Werner
    CIPS, Boulder, Colorado
 
 

Funding: This work is supported by the U.S. Department of Energy grant DE-FG02-04ER41317.


Through computer simulation, a 2D photonic crystal (PhC) cavity formed from a truncated triangular lattice of dielectric rods is optimized to confine a single accelerating mode efficiently. Photonic crystals have the ability to reflect radiation within only certain frequency ranges, called bandgaps; the bandgaps are determined by the geometry and material of the PhC and so are tunable. For truncated PhCs, reflection is incomplete. Therefore, the confinement of bandgap frequencies to a cavity within a truncated PhC is weakened by the severity of the truncation. For a cavity made of 18 dielectric rods in a truncated triangular lattice arrangement, the desired accelerating cavity mode is weakly confined. Adjusting the positions and sizes of the dielectric rods away from the best lattice configuration within an optimization procedure gives unintuitive structures, ultimately increasing the confinement of the accelerating mode by a factor of 100. Confinement of higher-order modes is also dramatically reduced by the optimization. Similar increases in confinement of the fundamental accelerating mode are found for a 24-rod structure.

 
FR5RFP023 Design of Photonic Bandgap Fiber Accelerating Structure accelerating-gradient, damping, wakefield, background 4582
 
  • H.Z. Zhang, S. Dong, C.-F. Wu
    USTC/NSRL, Hefei, Anhui
  • Z.P. Li
    USTC, Hefei, Anhui
 
 

Photonic crystals have been suggested for use as laser driven particle accelerator structures with higher accelerating gradients and effective damping of unwanted higher order modes. Here we selected Photonic band gap (PBG) fibers with hollow core defects to design such an accelerating structure. To achieve this design, Out-plane-wave mode in photonic crystal fiber was selected for longitudinal electric field. The out-plane-wave plane wave expansion method was deduced for confinement and the dispersive curve versus variation of kz and speed of line for synchronization. Then super cell approximation was also introduced for calculating the defected photonic crystal structure. After the design of appropriate geometry and the dimensions of photonic crystal fiber accelerating structure, the field distribution was simulated with RSOFT Bandsolve software for this structure.

 
FR5RFP034 Transverse Impedance Localization Using Dependent Optics impedance, optics, quadrupole, kicker 4604
 
  • R. Calaga
    BNL, Upton, Long Island, New York
  • G. Arduini, E. Métral, G. Papotti, D. Quatraro, G. Rumolo, B. Salvant, R. Tomás
    CERN, Geneva
 
 

Funding: This work has been partially performed under the auspices of US department of energy


Measurements of transverse impedance in the SPS to track the evolution over the last few years show discrepancies compared to the analytical estimates of the major contributors. Recent measurements to localize the major sources of the transverse impedance using intensity dependent optics are presented. Some simulations using HEADTAIL to understand the limitations of the reconstruction and related numerical aspects are also discussed.

 
FR5RFP078 Update on Electron-Cloud Simulations Using the Package WARP-POSINST electron, simulation, emittance, dipole 4719
 
  • J.-L. Vay, C.M. Celata, M.A. Furman, M. Venturini
    LBNL, Berkeley, California
  • D.P. Grote
    LLNL, Livermore, California
  • K.G. Sonnad
    FZK, Karlsruhe
 
 

Funding: Supported by the US-DOE under Contract DE-AC02-05CH11231, the US-LHC LARP, and the US-DOE SciDAC program ComPASS. Used resources of NERSC, supported by the US-DOE under Contract DE-AC02-05CH11231.


At PAC05, we presented the package WARP-POSINST for the modeling of the effect of electron clouds on high-energy beams. We present here the latest developments in the package. Three new modes of operations were implemented: 1) “build-up mode” where, similarly to Posinst (LBNL) or Ecloud (CERN), the build-up of electron clouds is modeled in one region of an accelerator driven by a legislated bunch train; 2) “quasi-static mode” where, similarly to Headtail (CERN) or Quickpic (USC/UCLA), the “frozen beam” approximation is used to split the modeling of the beam and the electrons into two components evolving on their respective time scales; and 3) “Lorentz boosted mode” where the simulation is performed into a moving frame where the space and time scales related to the beam and electron dynamics fall in the same range. The implementation of modes (1) and (2) was primary motivated by the need for benchmarking with other codes, while the implementation of mode (3) fulfills the drive toward fully self-consistent simulations of e-cloud effect on the beam including the build-up phase. We also present benchmarking with other codes and selected results from its application to e-cloud effects.

 
FR5REP001 High Availability On-Line Relational Databases for Accelerator Control and Operation controls, coupling, EPICS, storage-ring 4770
 
  • D. Dohan, G. Carcassi, L.R. Dalesio
    BNL, Upton, Long Island, New York
 
 

Funding: Work performed under auspices of the U.S. Department of Energy under Contract No. DE-AC02-98CH10886 with Brookhaven Science Associates, LLC.


The role of relational database (RDB) technology plays in accelelerator control and operation continues to grow in such areas as electronic log books, machine parameter definitions, and facility infrastructure management. RDBs are increasingly relied upon to provide the official 'master' copy of these data. The services provided by the RDB have traditionally not been 'mission critical'. The availability of modern RDB management systems is now equivalent to that of standard computer file-systems, and thus RDBs can be relied on to supply (pseudo-)realtime response to operator and machine physicist requests. This paper describes recent developments in the IRMIS RDB (1) project. Generic lattice support has been added, serving as the driver for model-based machine control. Abstract physics name service, with introspection has been added. Specific emphasis has been placed both on providing fast response time to accelerator operators and modeling code requests, as well as high (24/7) availability of the RDB service.

 
FR5REP003 RHIC Injector Complex Online Model Status and Plans booster, optics, proton, controls 4776
 
  • V. Schoefer, L. A. Ahrens, K.A. Brown, J. Morris, S. Nemesure
    BNL, Upton, Long Island, New York
 
 

Funding: Work supported by Brookhaven Science Associates, LLC under Contract No. DE-AC02-98CH10886 with the U.S. Department of Energy.


An online modeling system is being developed for the RHIC injector complex, which consists of the Booster, the AGS and the transfer lines connecting the Booster to the AGS and the AGS to RHIC. Historically the injectors have been operated using static values from design specifications or offline model runs, but tighter beam optics constraints required by polarized proton running (e.g. accelerating with near-integer tunes) have necessitated a more dynamic system. An online model server for the AGS has been implemented using MAD-X as the model engine, with plans to extend the system to the Booster and the injector transfer lines and to add the option of calculating optics using the Polymorphic Tracking Code (PTC) as the model engine.

 
FR5REP023 Interfacing of Third-Party Accelerator Code with the Lucretia Flight Simulator controls, extraction, simulation, monitoring 4814
 
  • S. Molloy, M.T.F. Pivi, G.R. White
    SLAC, Menlo Park, California
  • Y. Renier
    LAL, Orsay
 
 

The Flight Simulator is a tool used for international collaboration in the writing and deployment of online beam dynamics algorithms. Written as an add-on to the Lucretia tracking software, it allows simulation of a beamline in a control system environment identical to that in the control room. This allows the testing and development of monitoring and correction tools by an international collaboration by making the control system transparent to the user. The native beamline representation are those adopted by Lucretia, so, in order to allow third party software, to interface with this system, it was necessary to develop functionality to convert the lattice to a universal representation. Accelerator Markup Language (AML), and its associated Universal Accelerator Parser (UAP), were used for this purpose. This paper describes the use of the UAP to convert the internal beamline representation to AML, and the testing of this conversion routine using the lattice description of the ATF2 final focus experiment at KEK, Japan. Also described are the inclusion of PLACET and SAD based algorithms using appropriate converters, and tests of these on the ATF2 extraction line.

 
FR5REP044 Layout of an Electrostatic Storage Ring at KACST storage-ring, ion, quadrupole, injection 4866
 
  • M.O.A. El Ghazaly
    KUK, Abha
  • M.H. Al-Malki, M.O.A. El Ghazaly
    KACST, Riyadh
  • A.I. Papash
    MPI-K, Heidelberg
  • C.P. Welsch
    Cockcroft Institute, Warrington, Cheshire
 
 

A state-of-the-art fixed energy electrostatic storage ring that will allow for precision experiments with most different kinds of ions in the energy range of up to 30 keV will be constructed and operated at the National Center for Mathematic and Physics (NCMP) at the King Abdulaziz City for Science and Technology (KACST). The ring is planed to be the central machine of a unique and highly flexible experimental platform. The lattice design therefore has to cover the different experimental techniques that the ring will be equipped with, such as e.g. electron-ion crossed-beams and ion-laser/ion-ion/ion-neutral merged-beams techniques. This paper presents the technical and particle optical design of this novel machine, explains the particular challenges in its layout, and reports on the general project status.

 
FR5REP094 Tracking Periodic Parameters in the Measured Magnetic Field Maps of a Spiral FFAG closed-orbit, dipole, extraction, injection 4999
 
  • F. Méot
    CEA, Gif-sur-Yvette
  • F. Forest, M.J. Leray
    Sigmaphi, Vannes
  • J. Pasternak
    Imperial College of Science and Technology, Department of Physics, London
 
 

Funding: Agence Nationale de la Recherche, France, contract NT05-1_41853


A prototype of a spiral lattice FFAG magnet has been constructed in the frame of the RACCAM project*. THis magnet is subject to extensive field measurements and 3-dimensional field map measurements. The properties and qualities of the magnet are assessed directly from ray-tracing, using stepwise integration, for deriving lattice parameters as tunes, chromaticities, dynamic paertures, etc. Reporting on this is the subject of the poster.


*http://lpsc.in2p3.fr/service_accelerateurs/raccam.htm

 
FR5REP110 Magnetic Measurements of the RACCAM Prototype FFAG Dipole alignment, dipole, instrumentation, simulation 5032
 
  • M.J. Leray, P. Bocher, B. Diougoant, F. Forest, J.L. Lancelot
    Sigmaphi, Vannes
  • F. Méot
    CEA, Gif-sur-Yvette
  • J. Pasternak
    LPSC, Grenoble
 
 

The paper presents the magnetic measurements of the RACCAM prototype FFAG dipole, manufactured by SIGMAPHI for the Raccam ANR Medical FFAG project. This magnet prototyping work, started early 2006, is being performed in collaboration between the IN2P3/LPSC Laboratory team and SIGMAPHI. This paper describes the magnetic measurement results and comparison with Tosca simulation.

 
FR5REP112 Analysis of Orbits in Combined Function Magnets focusing, TRIUMF, closed-orbit, betatron 5038
 
  • S.R. Koscielniak
    TRIUMF, Vancouver
 
 

Fixed-Field Alternating-Gradient (FFAG) accelerators span a large range of momenta and have markedly different reference orbits for each momemtum. In the non-scaling (NS) versions proposed for rapid acceleration, the orbits are geometrically dissimilar. In particular, none of the orbits within bending magnets are arcs of circles and this complicates tune calculation. One approach to NS-FFAG design is to employ alternating combined-function magnets. Second generation NS-FFAGs designs attempt to mitigate the variation of betatron tunes; and careful calculation of orbits and tunes is essential. Starting from an analytic magnetic potential for the combined-function magnet, we elucidate expressions for orbit calculation which are second order in the cyclotron motion and arbitrary order in the momentum (no expansion is used).

 
FR5REP114 FFAGs and Cyclotrons with Reverse Bends cyclotron, focusing, resonance, TRIUMF 5044
 
  • M.K. Craddock
    UBC & TRIUMF, Vancouver, British Columbia
  • Y.-N. Rao
    TRIUMF, Vancouver
 
 

This paper describes tracking studies of FFAGs and radial-sector cyclotrons with reverse bends using the cyclotron equilibrium orbit code CYCLOPS. The results for FFAGs confirm those obtained with lumped-element codes, and suggest that cyclotron codes will prove to be important tools for evaluating the measured fields of FFAG magnets. The results for radial-sector cyclotrons show that the use of negative valley fields would allow axial focusing to be maintained, and hence allow intense cw beams to be accelerated, to energies of the order of 10 GeV.