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Tomas, R.     [Tomás, R.]

Paper Title Page
MO4RAC02 Status of LHC Crab Cavity Simulations and Beam Studies 85
 
  • R. Calaga, R. De Maria
    BNL, Upton, Long Island, New York
  • R.W. Assmann, J. Barranco, F. Caspers, E. Ciapala, T.P.R. Linnecar, E. Métral, Y. Sun, R. Tomás, J. Tuckmantel, Th. Weiler, F. Zimmermann
    CERN, Geneva
  • G. Burt
    Lancaster University, Lancaster
  • Y. Funakoshi, A. Morita, Y. Morita, K. Nakanishi, Y. Ohnishi
    KEK, Ibaraki
  • Z. Li, A. Seryi, L. Xiao
    SLAC, Menlo Park, California
  • P.A. McIntosh
    STFC/DL/ASTeC, Daresbury, Warrington, Cheshire
  • J. Qiang
    LBNL, Berkeley, California
  • N. Solyak, V.P. Yakovlev
    Fermilab, Batavia
 
 

Funding: This work was partially performed under the auspices of the US DOE and the European Community-Research Infrastructure, FP6 programme (CARE, contract number RII3-CT-2003-506395)}


The LHC crab cavity program is advancing rapidly towards a first prototype which is anticipated to be tested during the early stages of the LHC phase I upgrade and commissioning. Some aspects related to crab optics, collimation, aperture constraints, impedances, noise effects, beam transparency and machine protection critical for a safe and robust operation of LHC beams with crab cavities are addressed here.

 

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MO6PFP046 First Field Test of FiDeL the Magnetic Field Description for the LHC 241
 
  • L. Bottura, M.C.L. Buzio, N. Catalan-Lasheras, L. Deniau, M. DiCastro, S.D. Fartoukh, M. Giovannozzi, P. Hagen, J.-P. Koutchouk, M. Lamont, J. Miles, RV. Remondino, N.J. Sammut, S. Sanfilippo, F. Schmidt, D. Sernelius, R.J. Steinhagen, M. Strzelczyk, E. Todesco, R. Tomás, W. Venturini Delsolaro, L. Walckiers, J. Wenninger, R. Wolf, P. Xydi
    CERN, Geneva
 
 

The start-up of the LHC has provided the first field test for the concept, functionality and accuracy of FiDeL, the Field Description for the LHC. FiDeL is primarily a parametric model of the transfer function of the main field integrals generated by the series of magnets in the LHC powering circuits, from main optical elements to high-order harmonic correctors, both superconducting and normal-conducting magnets. In addition, the same framework is used to predict harmonic errors of both static and dynamic nature, and forecast appropriate corrections. In this paper we give a description of the level of detail achieved in the model and the rationale adopted for the LHC start-up. Beam-based measurements have been used for an assessment of the first-shot accuracy in the prediction of the current setting for the main arc magnets*.


*The work reported has been performed by the authors and the FiDeL Team

 
TU6PFP087 High Intensity Beams from the CERN PS Booster 1497
 
  • B. Mikulec, M. Chanel, A. Findlay, K. Hanke, D. Quatraro, G. Rumolo, J. Tan, R. Tomás
    CERN, Geneva
 
 

The CERN Proton Synchrotron Booster (PSB) has been running for more than 30 years. Originally designed to accelerate particles from 50 to 800 MeV, later upgraded to an energy of 1 GeV and finally 1.4 GeV, it is steadily being pushed to its operational limits. One challenge is the permanent demand for intensity increase, in particular for CNGS and ISOLDE, but also in view of LINAC4. As it is an accelerator working with very high space charge during the low energy part of its cycle, its operational conditions have to be precisely tuned. Amongst other things resonances must be avoided, stop band crossings optimized and the machine impedance minimized. Recently, an operational intensity record was achieved with >4.25·1013 protons accelerated. An orbit correction campaign performed during the 2007/2008 shutdown was a major contributing factor to achieving this intensity. As the PSB presently has very few orbit correctors available, the orbit correction has to be achieved by displacing and/or tilting some of the defocusing quadrupoles common to all 4 PSB rings. The contributing factors used to optimize performance will be reviewed.

 
WE6PFP019 First Beam-Based Aperture Measurements in the Arcs of the CERN Large Hadron Collider 2525
 
  • S. Redaelli, I.V. Agapov, B. Dehning, M. Giovannozzi, F. Roncarolo, R. Tomás
    CERN, Geneva
  • R. Calaga
    BNL, Upton, Long Island, New York
 
 

Various LHC injection tests were performed in August and early September 2008 in preparation for the circulating beam operation. These tests provided the first opportunity to measure with beam the available mechanical aperture in two LHC sectors (2-3 and 7-8). The aperture was probed by exciting free oscillations and local orbit bumps of the injected beam trajectories. Intensities of a few 109 protons were used to remain safely below the quench limit of superconducting magnets in case of beam losses. In this paper the methods used to measure the mechanical aperture, the available on-line tools, and beam measurements for both sectors are presented. Detailed comparisons with the expected results from the as-built aperture models are also presented. It is shown that the measurements results are in good agreement with the LHC design aperture.

 
WE6PFP020 Study with One Global Crab Cavity at IR4 for LHC 2528
 
  • Y. Sun, R.W. Assmann, J. Barranco, R. Tomás, Th. Weiler, F. Zimmermann
    CERN, Geneva
  • R. Calaga
    BNL, Upton, Long Island, New York
  • A. Morita
    KEK, Ibaraki
 
 

Funding: This work was supported by the European Community-Research Infrastructure Activity under the FP6 "Structuring the European Research Area" programme (CARE, contract number RII3-CT-2003-506395).


Modern colliders bring into collision a large number of bunches per pulse or per turn to achieve a high luminosity. The long-range beam-beam effects arising from parasitic encounters at such colliders are mitigated by introducing a crossing angle. Under these conditions, crab cavities (CC) can be used to restore effective head-on collisions and thereby to increase the geometric luminosity. In this paper, we discuss the beam dynamics issues of a single global crab cavity (GCC) for both nominal LHC optics and one upgrade LHC optics.

 
WE6PFP021 First Beta-Beating Measurement in the LHC 2531
 
  • R. Tomás, M. Aiba, S.D. Fartoukh, F. Franchi, M. Giovannozzi, V. Kain, M. Lamont, G. Vanbavinckhove, J. Wenninger, F. Zimmermann
    CERN, Geneva
  • R. Calaga
    BNL, Upton, Long Island, New York
  • A. Morita
    KEK, Ibaraki
 
 

In 2008 beam successfully circulated in the LHC. Thanks to an excellent functioning of the BPM system and the related software, injection oscillations were recorded for the first 90 turns at all BPMs. The analysis of these data gives the unique opportunity of evaluating the periodic optics and inferring possible error sources.

 
WE6PFP022 Beta-Beating Corrections in the SPS as a Testbed for the LHC 2534
 
  • R. Tomás, M. Aiba, G. Vanbavinckhove, J. Wenninger
    CERN, Geneva
  • R. Calaga
    BNL, Upton, Long Island, New York
  • A. Morita
    KEK, Ibaraki
 
 

For several years optics measurement and correction algorithms have been developed for the LHC. During 2008 these algorithms have been directly tested in the SPS and RHIC. The experimental results proving the readiness of the applications are presented.

 
WE6PFP023 Status of the CLIC Beam Delivery System 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 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.

 
WE6PFP026 Linear & Nonl. Optics Checks during LHC Injection Tests 2546
 
  • F. Zimmermann, S.D. Fartoukh, M. Giovannozzi, V. Kain, M. Lamont, Y. Sun, R. Tomás
    CERN, Geneva
  • R. Calaga
    BNL, Upton, Long Island, New York
 
 

In early LHC commissioning, linear and "higher-order" polarity checks were performed for one octant per beam, by launching suitable free betatron oscillations and then inverting a magnet-circuit polarity or strength. Circuits tested included trim quadrupoles, skew quadrupoles, lattice sextupoles, sextupole spool-pieces, Landau octupoles, and skew sextupoles. A nonzero momentum offset was introduced to enhance the measurement quality. The low-intensity single-pass measurements proved sufficiently sensitive to verify the polarity and the amplitude of (almost) all circuits under investigation, as well as the alignment of individual trim quadrupoles. A systematic polarity inversion detected by this measurement helped to pin down the origin of observed dispersion errors. Later, the periodic "ring dispersion" was reconstructed from the full first-turn trajectory of an injected off-momentum beam, by removing, at each location, the large incoming dispersion mismatch, forward-propagated via the optics model. Various combinations of inverted trim quadrupoles were considered in this model until reaching a good agreement of reconstructed dispersion and prediction.

 
WE6PFP006 Overview of Magnetic Nonlinear Beam Dynamics in RHIC 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.

 
TH5PFP016 Tune Shift due to Crossing Collision and Crab Collision 3223
 
  • Y. Sun, R. Tomás, F. Zimmermann
    CERN, Geneva
 
 

Funding: This work was supported by the European Community-Research Infrastructure Activity under the FP6 "Structuring the European Research Area" programme (CARE, contract number RII3-CT-2003-506395).


The use of crab cavities in the LHC may not only raise the luminosity, but it could also complicate the beam dynamics, e.g. crab cavities might not only cancel synchro-betatron resonances excited by the crossing angle but they could also excite new ones. In this paper, we use weak-strong beam-beam model to study the incoherent linear tune shift of the weak beam, for the crossing collision case and crab collision case with a finite crossing angle. The tune shift is also compared among the head-on collision, crossing collision and crab collision cases, both analytically and numerically.

 
TH6PFP046 Dynamic Effects in the New CLIC Main Linac 3811
 
  • D. Schulte, R. Tomás
    CERN, Geneva
 
 

In the compact linear collider (CLIC) the tolerances on dynamic imperfections are tight in the main linac. In particular the limited beam delivery system bandwidth requires very good RF phase and amplitude stability. Transverse motion of the beam line components is also of concern. The resulting tolerances are detailed in the paper.

 
TH6PFP074 Solenoid and Synchrotron Radiation Effects in CLIC 3874
 
  • B. Dalena, D. Schulte, R. Tomás
    CERN, Geneva
  • D. Angal-Kalinin
    STFC/DL/ASTeC, Daresbury, Warrington, Cheshire
 
 

The emission of Synchrotron Radiation in the CLIC BDS is one of the major limitations of the machine performance. An extensive revision of this phenomenon is presented with special emphasis on the IP solenoid.

 
TH6PFP075 Linear and Non-Linear Optics Measurements at SOLEIL 3877
 
  • R. Tomás, M. Aiba, G. Vanbavinckhove
    CERN, Geneva
  • A. Nadji, L.S. Nadolski, M.-A. Tordeux
    SOLEIL, Gif-sur-Yvette
 
 

The successful correction of non-linear resonances in DIAMOND using the BPM turn-by-turn data has motivated testing this approach in SOLEIL in collaboration with CERN. We report on the first experiences towards the correction of non-linear resonances in SOLEIL.

 
FR1RAI01 CLIC Overview 4195
 
  • R. Tomás
    CERN, Geneva
 
 

The CLIC study is exploring the scheme for an electron-positron collider with a centre-of-mass energy of 3 TeV in order to make the multi-TeV range accessible for physics. The current goal of the project is to demonstrate the feasibility of the technology by the year 2010. Recently, important progress has has been made concerning the high-gradient accelerating structure tests and the experiments with beam in the CLIC test facility, CTF3. On the organizational side, the CLIC international collaborations have significantly gained momentum considerably boosting the CLIC study.

 

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FR5PFP021 Plans and Progress towards Tuning the ATF2 Final Focus System to Obtain a 35nm IP Waist 4353
 
  • G.R. White
    SLAC, Menlo Park, California
  • J.K. Jones
    STFC/DL/ASTeC, Daresbury, Warrington, Cheshire
  • K. Kubo, S. Kuroda
    KEK, Ibaraki
  • Y. Renier
    LAL, Orsay
  • A. Scarfe
    UMAN, Manchester
  • R. Tomás
    CERN, Geneva
 
 

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


Using a new extraction line currently being commissioned, the ATF2 experiment plans to test a novel compact final focus optics design using a local chromaticity correction scheme, such as could be used in future linear colliders*. Using a 1.3 GeV beam of ~30nm normalised vertical emittance extracted from the ATF damping ring, the primary goal is to achieve a vertical IP waist of 35nm. We discuss our planned strategy, implementation details and early experimental results for tuning the ATF2 beam to meet the primary goal. These optics require uniquely tight tolerances on some magnet strengths and positions, we discuss efforts to re-match the optics to meet these requirements using high-precision measurements of key magnet elements. We simulated in detail the tuning procedure using several algorithms and different code implementations for comparison from initial orbit establishment to final IP spot-size tuning. Through a Monte Carlo study of 100's of simulation seeds we find we can achieve a spot-size within 10% of the design optics value in at least 90% of cases. We also ran a simulation to study the long-term performance with the use of beam-based feedbacks.


*"ATF2 Proposal", ATF2 Collaboration (Boris Ivanovich Grishanov et al.)., KEK-REPORT-2005-2, Aug 23, 2005.

 
FR5RFP034 Transverse Impedance Localization Using Dependent Optics 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.

 
FR1RAI03 ATF2 Commissioning 4205
 
  • A. Seryi, J.W. Amann, P. Bellomo, B. Lam, D.J. McCormick, J. Nelson, J.M. Paterson, M.T.F. Pivi, T.O. Raubenheimer, C.M. Spencer, M.-H. Wang, G.R. White, W. Wittmer, M. Woodley, Y.T. Yan, F. Zhou
    SLAC, Menlo Park, California
  • D. Angal-Kalinin, J.K. Jones
    STFC/DL/ASTeC, Daresbury, Warrington, Cheshire
  • R. Apsimon, B. Constance, C. Perry, J. Resta-López, C. Swinson
    JAI, Oxford
  • S. Araki, A.S. Aryshev, H. Hayano, Y. Honda, K. Kubo, T. Kume, S. Kuroda, M. Masuzawa, T. Naito, T. Okugi, R. Sugahara, T. Tauchi, N. Terunuma, J. Urakawa, K. Yokoya
    KEK, Ibaraki
  • S. Bai, J. Gao
    IHEP Beijing, Beijing
  • P. Bambade, Y. Renier, C. Rimbault
    LAL, Orsay
  • G.A. Blair, S.T. Boogert, V. Karataev, S. Molloy
    Royal Holloway, University of London, Surrey
  • B. Bolzon, N. Geffroy, A. Jeremie
    IN2P3-LAPP, Annecy-le-Vieux
  • P. Burrows
    OXFORDphysics, Oxford, Oxon
  • G.B. Christian
    ATOMKI, Debrecen
  • J.-P. Delahaye, D. Schulte, R. Tomás, F. Zimmermann
    CERN, Geneva
  • E. Elsen
    DESY, Hamburg
  • E. Gianfelice-Wendt, M.C. Ross, M. Wendt
    Fermilab, Batavia
  • A. Heo, E.-S. Kim, H.-S. Kim
    Kyungpook National University, Daegu
  • J.Y. Huang, W.H. Hwang, S.H. Kim, Y.J. Park
    PAL, Pohang, Kyungbuk
  • Y. Iwashita, T. Sugimoto
    Kyoto ICR, Uji, Kyoto
  • Y. Kamiya
    ICEPP, Tokyo
  • S. Komamiya, M. Oroku, T.S. Suehara, T. Yamanaka
    University of Tokyo, Tokyo
  • A. Lyapin
    UCL, London
  • B. Parker
    BNL, Upton, Long Island, New York
  • T. Sanuki
    Tohoku University, Graduate School of Science, Sendai
  • A. Scarfe
    UMAN, Manchester
  • T. Takahashi
    Hiroshima University, Graduate School of Science, Higashi-Hiroshima
  • A. Wolski
    Cockcroft Institute, Warrington, Cheshire
 
 

ATF2 is a final-focus test beam line that attempts to focus the low-emittance beam from the ATF damping ring to a beam size of about 37 nm, and at the same time to demonstrate nm beam stability, using numerous advanced beam diagnostics and feedback tools. The construction is well advanced and beam commissioning of ATF2 has started in the second half of 2008. ATF2 is constructed and commissioned by ATF international collaborations with strong US, Asian and European participation.

 

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FR1PBC05 The Large Hadron-Electron Collider (LHeC) at the LHC 4233
 
  • F. Zimmermann, F. Bordry, H.-H. Braun, O.S. Brüning, H. Burkhardt, A.L. Eide, R. Garoby, B.J. Holzer, J.M. Jowett, T.P.R. Linnecar, K.H. Meß, J.A. Osborne, L. Rinolfi, D. Schulte, R. Tomás, J. Tuckmantel, A. Vivoli, A. de Roeck
    CERN, Geneva
  • H. Aksakal
    N.U, Nigde
  • S. Chattopadhyay, J.B. Dainton
    Cockcroft Institute, Warrington, Cheshire
  • A.K. Çiftçi
    Ankara University, Faculty of Sciences, Tandogan/Ankara
  • M. Klein
    The University of Liverpool, Liverpool
  • T. Omori, J. Urakawa
    KEK, Ibaraki
  • S. Sultansoy
    TOBB ETU, Ankara
  • F.J. Willeke
    BNL, Upton, Long Island, New York
 
 

Sub-atomic physics at the energy frontier probes the structure of the fundamental quanta of the Universe. The Large Hadron Collider (LHC) at CERN opens for the first time the “terascale” (TeV energy scale) to experimental scrutiny, exposing the physics of the Universe at the sub-attometric (~10-19 m, 10-10 as) scale. The LHC will also take the science of nuclear matter to hitherto unparalleled energy densities (low-x physics). The hadron beams, protons or ions, in the LHC underpin this horizon, and also offer new experimental possibilities at this energy scale. A Large Hadron electron Collider, LHeC, in which an electron (positron) beam of energy (70 to 140 GeV) is in collision with one of the LHC hadron beams, makes possible terascale lepton-hadron physics. The LHeC is presently being evaluated in the form of two options, “ring-ring” and “linac-ring”, either of which operate simultaneously with pp or ion-ion collisions in other LHC interaction regions. Each option takes advantage of recent advances in radio-frequency, in linear acceleration, and in other associated technologies, to achieve ep luminosity as large as 1033 cm-2s-1.

 

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FR5RFP047 Analysis of the Transverse SPS Beam Coupling Impedance with Short and Long Bunches 4640
 
  • B. Salvant
    EPFL, Lausanne
  • G. Arduini, H. Burkhardt, H. Damerau, W. Höfle, E. Métral, G. Papotti, G. Rumolo, B. Salvant, R. Tomás, S.M. White
    CERN, Geneva
  • R. Calaga, R. De Maria
    BNL, Upton, Long Island, New York
 
 

The upgrade of the CERN Large Hadron Collider (LHC) would require a four- to fivefold increase of the single bunch intensity presently obtained in the Super Proton Synchrotron (SPS). Operating at such high single bunch intensities requires a detailed knowledge of the sources of SPS beam coupling impedance, so that longitudinal and transverse impedance reduction campaigns can be planned and performed effectively if needed. In this paper, the transverse impedance of the SPS is studied by injecting a single long bunch into the SPS, and observing its decay without RF. This particular setup enhances the resolution of the frequency analysis of the longitudinal and transverse bunch signals acquired with strip line couplers connected to a fast data acquisition. It also gives access to the frequency content of the transverse impedance. Results from measurements with short and long bunches in the SPS performed in 2008 are compared with simulations and theoretical predictions.