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HOM

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MO304 3.9 GHz Cavity Module for Linear Bunch Compression at FLASH cavity, electron, photon, simulation 41
 
  • H.T. Edwards, E.R. Harms
    Fermilab, Batavia
  • C. Behrens
    DESY, Hamburg
 
 

FNAL has contributed to FLASH at DESY the third harmonic accelerating system, which will provide better beams for the FEL facility. The FNAL accelerating module has been qualified above specs and will be operational in FLASH in Spring.

 

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MOP002 A High Phase Advance Damped and Detuned Structure for the Main Linacs of CLIC dipole, wakefield, coupling, beam-loading 49
 
  • R.M. Jones, A. D'Elia, V.F. Khan
    UMAN, Manchester
  • A. Grudiev, W. Wuensch, R. Zennaro
    CERN, Geneva
 
 

We report on the suppression of long-range wakefields in the main linacs of the CLIC collider. The wakefield is damped using a combination of detuning the frequencies of beam-excited higher order modes and by light damping, through slot-coupled manifolds. This unique accelerator, in the process of being fabricated, will be the first structure to demonstrate wakefield damping and the ability to sustain high accelerating gradients for CLIC. This serves as an alternative to the baseline CLIC design, which at present relies entirely on heavy damping. Detailed simulations are presented, on both the optimised surface fields resulting from the monopole mode, and from wakefield damping of the dipole modes. Preparations for the fabrication of a structure, suitable for high power testing, are also discussed. This design takes into account practical mechanical engineering issues and is the result of several optimisations since the original CLICDDS proposal[*].


*V.F. Khan and R.M. Jones, Presented at Particle Accelerator Conference (PAC 09), Vancouver, BC, Canada, 4-8 May 2009.

 
MOP029 S0-studies on ICHIRO 9-cell Cavities in Collaboration with KEK and Jlab cavity, superconductivity, electron, cathode 118
 
  • F. Furuta, K. Saito
    KEK, Ibaraki
  • G.V. Eremeev, R.L. Geng
    JLAB, Newport News, Virginia
  • T. Konomi
    Sokendai, Ibaraki
 
 

In 2008, KEK and Jlab did the collaboration of S0-study on ICHIRO 9-cell #5 which has no end groups on beam tubes. As S0 tight loop test, surface treatments and vertical tests were repeated on ICHIRO#5 at both of Jlab and KEK. Maximum gradients of 36.5MV/m at Jlab and 33.7MV/m at KEK were achieved so far. In this year, 2010, KEK and Jlab started new S0-study collaboration on ICHIRO 9cell #7 which has full end groups on beam tubes. ICHIR#7 was already sent to Jlab and VT as received was done. We will report the results of tight loop tests at Jlab.

 
MOP030 Status of Superconducting Cavity Development for ILC at MHI cavity, superconducting-cavity, status, niobium 121
 
  • H. Hitomi, H. Hara, K. Kanaoka, K. Sennyu, T. Yanagisawa
    MHI, Kobe
 
 

MHI's activities for ILC project will be shown.

 
MOP065 C-Band Magnetic Coupled Accelerating Structure Optimization impedance, coupling, simulation, insertion 202
 
  • S.V. Kutsaev, R.O. Bolgov, M. Gusarova, D.S. Kamenshikov, K.I. Nikolskiy, A.Yu. Smirnov, N.P. Sobenin, S.E. Toporkov
    MEPhI, Moscow
 
 

This paper presents the results of a research that analyzed the possibility of using a magnetic coupled disk-loaded structure (DLS-M) as an accelerating structure. DLS-M seems to have decent advantages comparing to the classical electrical coupled structure (DLS). The electrodynamics parameters of such a structure at various modes in C-band for a wide range of phase velocities as a function of aperture radii and coupling slot sizes are presented. Both forward and backward travelling wave regimes are considered. The essential parameters are compared to those of classical DLS. The design of an input coupler to the accelerator consisting of this type structure cells is also presented.

 
MOP067 First High Power Tests of CLIC Prototype Accelerating Structures with HOM Waveguide Damping damping, linac, higher-order-mode, target 208
 
  • S. Döbert, A. Grudiev, G. Riddone, W. Wuensch, R. Zennaro
    CERN, Geneva
  • C. Adolphsen, F. Wang, J.W. Wang
    SLAC, Menlo Park, California
  • T. Higo, S. Matsumoto, K. Yokoyama
    KEK, Ibaraki
 
 

Prototype accelerating structures for the Compact Linear Collider (CLIC) are being developed and high-power tested in a collaboration between SLAC, KEK and CERN. Several undamped, low group-velocity and strongly tapered prototypes (of the so-called T18 design) have been operated above 100 MV/m average gradient at a very low breakdown rates. Recently two new structures with the same iris apertures but now including higher order mode damping waveguides in each cell (TD18 design) have been tested at SLAC and KEK. The damped versions could be processed to similar gradients but an increased breakdown rate was observed. The damping waveguides lead to a magnetic field enhancement in the outer diameter of the cells which results in increased pulsed surface heating. The maximum pulsed temperature rise is 80 deg at the design gradient of 100 MV/m compared to only 20 deg for the undamped version. The high-power tests of the two TD18 structures are analyzed with special emphasis on the influence on breakdown rate of the enhanced magnetic field and consequent increased pulsed surface temperature rise.

 
MOP068 Design of the CLIC Main Linac Accelerating Structure for CLIC Conceptual Design Report damping, linac, wakefield, impedance 211
 
  • A. Grudiev, W. Wuensch
    CERN, Geneva
 
 

The design of the CLIC main linac accelerating structure has been refined based on an improved understanding of the high-gradient limits given by rf breakdown and pulsed surface heating. In addition, compact couplers have been developed and HOM damping loads have been designed. The rf design has also been made consistent with details of the present manufacturing procedure, based on bonded asymmetrical disks, and with requirements coming from integration of the accelerating structure in the two-beam module which includes all subsystems. This completion and refinement of the structure design has been made to produce the self-consistent parameter set required for preparation of the CLIC conceptual design report.

 
MOP113 Multipacting Simulation of the Demountable Damped Cavity cavity, simulation, electron, coupling 328
 
  • T. Konomi
    Sokendai, Ibaraki
  • F. Furuta, K. Saito
    KEK, Ibaraki
 
 

We have designed Demountable Damped Cavity (DDC) as an ILC R&D. DDC has an axial symmetric structure, the coaxial waveguide HOM coupler and absorber at the end of beam pipe of SRF cavity. It is also demountable structure. These structures are expected to bring better cavity performance. However, DDC have many parallel faced surfaces and the multipacting might be a concerned issue. We have simulated MP on the DDC with CST-Studio and found MP could be not serious issue. In this paper we will report the simulation result in detail.

 
TU303 Status of the Cornell ERL Injector Cryomodule cavity, cryomodule, SRF, alignment 382
 
  • M. Liepe
    CLASSE, Ithaca, New York
 
 

The Cornell Energy Recovery Linac (ERL) Injector cryomodule is part of a prototype electron beam source to demonstrate production of CW 1.3 GHz, 100 mA average current, 2 ps, 77 pC bunches with emittance of 1 mm-mrad. After a successful initial run of the cryomodule with beam, an improvement program was initiated in the Fall 2009. The goals of the reconfiguration were to replace the RF absorbers in the beamline HOM loads that were subject to static charging, re-process the SRF cavities that exhibited a low Q that further decreased by 50% during the run, and improve diagnostic sensor accuracy within the cryomodule. The upgraded cryomodule was re-commissioned in early 2010 with excellent performance. Details of the investigation and remedies for HOM load charging, cavity Q recovery, and module assembly logistics will be presented along with the ERL Injector beam performance.

 

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TUP005 Status of Development of the cERL Superconducting Injector Linac pick-up, cavity, linac, target 401
 
  • K. Watanabe, E. Kako, S. Noguchi, M. Satoh, T. Shishido, Y. Yamamoto
    KEK, Ibaraki
 
 

Development of the superconducting injector Linac for compact ERL has been continuing at KEK. The cryomodule including three two-cell SC cavities was designed. Two prot-type two-cell cavities were fabricated, and the vertival test were carried out after the standard surface preparation at STF. The high power tests of the input couplers were also carried out at the test stand with 300 kW cw klystron. The status of the cERL injector cryomodue will be reported.

 
TUP006 Development of a Main Linac Module for Compact ERL Project cavity, linac, cryomodule, superconducting-cavity 404
 
  • K. Umemori, T. Furuya, H. Sakai, T. Takahashi
    KEK, Ibaraki
  • M. Sawamura
    JAEA/ERL, Ibaraki
  • K. Shinoe
    ISSP/SRL, Chiba
 
 

A construction of the Compact ERL is planned in KEK, Japan. A demonstration of the performance of the main linac super-conducting accelerating system is one motivation of the project. We have been designing a cryo-module, which works under CW operation, and contains two 9-cell cavities, with input couplers, frequency tuners and HOM dampers. Most of these components have been specially developed for ERL operation. Two proto-type of the 9-cell cavity were constructed. First one was vertically tested and suffered from field emissions. Second one is now waiting a measurement. High power component tests have been carried out for input coupler. At first, large temperature rise was observed at a ceramic window part due to unexpected dipole resonance. After that, new version of window was designed and successfully passed 20kW CW power with reflection. Proto-types of HOM damper were also constructed. Cooling tests have been performed for them to verify cooling ability against more than 100W heat load, under vacuum condition. A cryo-module will be completed in 2012, and cooling tests and beam tests will follow.

 
TUP010 Test Results of Components for CW and Near-CW Operation of a Superconducting Linac cavity, linac, SRF, cathode 413
 
  • J.K. Sekutowicz, M. Ebert, F. Mittag
    DESY, Hamburg
  • P. Kneisel
    JLAB, Newport News, Virginia
  • R. Nietubyc
    The Andrzej Soltan Institute for Nuclear Studies, Centre Swierk, Swierk/Otwock
 
 

The European XFEL will use superconducting TESLA cavities operating with 650 μs long bunch trains. With 220 ns bunch spacing and 10 Hz RF-pulse repetition rate up to 27000 high quality bunches/s will be delivered to insertion devices generating unprecedented high average brilliance photon beams at very short wavelength. While many experiments can take advantage of full bunch trains, others prefer an increased several μ-seconds intra pulse distance between bunches, or short bursts with kHz repetition rate. With the nominal RF-pulse structure these features will lead to a substantially reduced number of bunches per second and therefore to significantly lower average brilliance. We discuss here an R&D program aiming for a far future upgrade of the European XFEL; operation in the cw and/or near-cw mode. The program profits from the continuous improvement in performance of TESLA cavities, which allows for longer RF-pulses in comparison with the current design. We present test results of a SRF electron injector and a new RF-power source, and some modification of the HOM damping scheme, which will avoid the necessity of re-assembly of the XFEL accelerator for the upgraded operations.

 
TUP013 Commissioning and Early Operating Experience of the FLASH Third Harmonic RF System cavity, FEL, cryomodule, superconducting-cavity 422
 
  • E.R. Harms, H.T. Edwards
    Fermilab, Batavia
  • M. Hüning, E. Vogel
    DESY, Hamburg
 
 

A Third Hamonic/3.9 GHz superconducting RF module was recently installed in the FLASH facility at DESY. Ultra short bunches with high peak current are required to efficiently create high brilliance coherent light and these can be produced by means of a 2-stage transverse magnetic chicane bunch compression scheme coupled with off-crest acceleration. The long bunch tails and reduced peak current which result from the nonlinearities of the RF since wave can be eliminated by the addition of a 3rd harmonic RF system. Such a system can also allow for the creation of uniform intensity bunches of adjustable length necessary for seeded operation. We present here a summary of commissioning and early operating experience of the newly-installed device.

 
TH102 SRF and Cryomodule R+D for ERL's cavity, SRF, booster, linac 712
 
  • J. Knobloch
    HZB, Berlin
 
 

A review of the SRF and cryomodule R&D for various ERL projects around the world. Many challenging R&D problems will be addressed such as high average current SRF injectors and CW high gradient SRF modules.

 
THP004 Layout and Machine Optimisation for the SPL at CERN cavity, linac, klystron, proton 761
 
  • F. Gerigk, S. Atieh, S. Calatroni, O. Capatina, E. Ciapala, M. Eshraqi, L.M.A. Ferreira, R. Garoby, M. Hernandez Flano, W. Höfle, E. Lebbos, A.M. Lombardi, E. Montesinos, Th. Otto, V. Parma, P.A. Posocco, T. Renaglia, M. Schuh, V. Vlachoudis, W. Weingarten, S. Weisz
    CERN, Geneva
  • R. Calaga
    BNL, Upton, Long Island, New York
 
 

During the past 2 years the Superconducting Proton Linac (SPL) study has grown into an international collaboration with the goal of optimising the architecture of a pulsed superconducting (SC) high-power proton linac. This effort includes the study and prototyping of major technical components, such as SC high-gradient cavities, power couplers, the RF distribution system, HOM couplers, cryo-modules, focusing elements, etc. Even though the effort is driven by CERN specific needs, the established design principles are valid for a range of superconducting linac projects. In this paper we report on the latests decisions concerning the machine architecture and on the ongoing R&D effort for technical components.

 
THP009 Critical Dipole Modes in JLAB Upgrade Cavities cavity, damping, cryomodule, dipole 776
 
  • F. Marhauser, J. Henry, H. Wang
    JLAB, Newport News, Virginia
 
 

The 12GeV upgrade of CEBAF is currently in progress. Ten new cryomodules will be installed at completion of the project to increase the energy from 6GeV to 12GeV. Each cryomodule houses eight seven-cell Low Loss type cavities. The damping of HOMs is crucial to prevent from beam break-up (BBU) instabilities at the desired beam currents as experienced with an upgrade demonstration cryomodule which needed to be de-installed recently. Detailed HOM surveys of a complete string of cavities in a cryomodule as well as individual cavities revealed the existence of critical dipole modes below and above beam tube cutoff that needed extensive experimental and numerical analyses. Results and their consequences for the 12 GeV upgrade cryomodules are detailed.

 
THP011 First Beam Spectra of sc Third Harmonic Cavity at FLASH cavity, simulation, electron, FEL 782
 
  • P. Zhang, R.M. Jones, I.R.R. Shinton
    UMAN, Manchester
  • N. Baboi, B. Lorbeer, P. Zhang
    DESY, Hamburg
  • T. Flisgen, H.-W. Glock, U. van Rienen
    Rostock University, Faculty of Computer Science and Electrical Engineering, Rostock
 
 

Third harmonic superconducting cavities have been designed and fabricated by FNAL to minimise the energy spread along bunches in the FLASH facility at DESY. A module, consisting of four nine-cell 3.9 GHz cavities, has been installed in FLASH. The first measurement with beam excitation is presented, and the comparisons to transmission measurement without beam and simulations are made. Higher order modes (HOMs) are able to propagate to adjacent cavities through attached beam tubes. Modes from 1.3 GHz cavities in the module nearby also propagate into this module.


*Work supported by European Commission under the FP7 Research Infrastructures grant agreement No.227579.

 
THP012 Higher Order Modes in Third Harmonic Cavities at FLASH cavity, simulation, dipole, impedance 785
 
  • R.M. Jones, I.R.R. Shinton, P. Zhang
    UMAN, Manchester
  • N. Baboi
    DESY, Hamburg
  • T. Flisgen, H.-W. Glock, U. van Rienen
    Rostock University, Faculty of Computer Science and Electrical Engineering, Rostock
 
 

Transverse modes in the 3.9 GHz cavities designed and fabricated by FNAL are reported on. These modes have the potential to cause significant emittance dilution if they not sufficiently suppressed. Recent experiments, both probe-based and beam-excited, have indicated significant discrepancies between modes predicted in stand-alone 9-cell cavities compared to those in 4-cavity modules. We employ a suite of computer codes and circuit models to analyze these modes, coupled through beam tubes whose cut-off is above that of the first dipole band. We also report on preparations to instrument the higher order mode couplers with electronics suitable for diagnosing both the beam and cavity position, based on modes with sufficient R/Q values.

 
THP015 A Review of the 1.3GHz Superconducting 9-Cell Cavity Fabrication for DESY cavity, higher-order-mode, linac, electron 794
 
  • J. Iversen, R. Bandelmann, G. Kreps, W.-D. Möller, D. Proch, J.K. Sekutowicz, W. Singer
    DESY, Hamburg
 
 

Since 1993 DESY ordered 165 1.3GHz 9-cell superconducting cavities. The cavities have been developed for TeV-Energy Superconducting Linear Accelerator (TESLA) and are used in the linac of the Free Electron Laser in Hamburg (FLASH). The fabrication of all cavities was done in 9 production groups at industry. From the beginning the industrialization was carried out in close collaboration between DESY and the industry. From order to order the cavity design was optimized and the fabrication sequences were improved to realize stable and better cavity performance and to safe costs. Now a final cavity design for the European XFEL is defined. We summarize the development phases and design changes up to the final XFEL design. An outlook on the near future production of hundreds of cavities for XFEL based on our experience will be given.

 
THP018 Recent Results of 1.3 GHz 9-cell Superconducting Cavities in KEK-STF cavity, radiation, superconducting-cavity, electron 800
 
  • Y. Yamamoto, H. Hayano, E. Kako, S. Noguchi, M. Satoh, T. Shishido, K. Umemori, K. Watanabe
    KEK, Ibaraki
 
 

MHI#10 and #11 cavities are measured in KEK-STF as the s0 plan for ILC. After these vertical tests, they will be sent to J-Lab and tested at least once there. Moreover, two new cavities without HOM coupler are fabricated and measured in STF, which are made by two new vendors (HITACHI and TOSHIBA). As the international collaboration, one cavity from IHEP in Beijing will be sent to KEK, optical inspected, high pressure rinsed and vertical tested. Although MHI#8 cavity for S1-Global reached 38MV/m, it could not achieve ILC specification (35MV/m, 0.8x109) due to the heavy field emission. To overcome this problem, the various tests were done in the stage of the surface treatment. For example, the EP parameters and the rinsing procedure were changed. In this report, the recent results of the vertical tests including the surface treatment in KEK-STF will be presented in detail.

 
THP021 Higher Order Mode Heating Analysis for the ILC Superconducting Linacs* cavity, linac, scattering, coupling 803
 
  • K.L.F. Bane, C. Adolphsen, C.D. Nantista
    SLAC, Menlo Park, California
 
 

The superconducting cavities and interconnects in the 12 km long linacs of the International Linear Collider (ILC) are designed to operate at 2K where cooling costs are very expensive. Thus it is important to ensure that any additional cryogenic heat loads are small in comparison to those from static losses and the fundamental 1.3 GHz accelerator mode. One potential heat source is the higher order modes (HOM) excited by the beam. Such modes will be damped by specially designed HOM couplers that are attached to the cavities (for trapped modes), and by 70K ceramic dampers that are located in each of the eight or nine cavity cryomodules (for propagating modes). Brute force calculations of the higher frequency, non-trapped modes excited in a string of cryomodules is limited by computing capacity. We present, instead, an approach that combines scattering matrix and wakefield calculations to study the effectiveness of the dampers in limiting the heat deposited in the 2K cryogenic system.

 
THP024 Design Sensitivities of the Superconducting Parallel-Bar Cavity cavity, luminosity, superconductivity, higher-order-mode 812
 
  • S.U. De Silva, J.R. Delayen
    ODU, Norfolk, Virginia
 
 

The superconducting parallel-bar cavity has properties that makes it attractive as a deflecting or crabbing rf structure. For example it is under consideration as an rf separator for the Jefferson Lab 12 GeV upgrade and as a crabbing structure for a possible LHC luminosity upgrade. In order to maintain the purity of the deflecting mode and avoid mixing with the near accelerating mode caused by geometrical imperfection, a minimum frequency separation is needed which depends on the expected deviations from perfect symmetry. We have done an extensive analysis of the impact of several geometrical imperfections on the properties of the parallel-bar cavities and the effects on the beam, and present the results in this paper.

 
THP034 Baseline Cavity Design for Cornell's Energy Recovery Linac cavity, linac, higher-order-mode, dipole 830
 
  • N.R.A. Valles, M. Liepe
    CLASSE, Ithaca, New York
 
 

This paper discusses the baseline superconducting RF cavity design to be used in Cornell's Energy Recovery Linac, a next generation light source. We discuss the methods used to obtain the design and present the cavity's figures of merit. The baseline cavity design is ready for prototyping, which will begin in the fall of 2010. Finally, we introduce small variations in the center cell design to increase the threshold current through the cavity by increasing the higher order mode relative frequency spread in the main linac, that have the effect of more than doubling the threshold current to 450 mA.

 
THP054 A Diplexer to Operate Two Cavity Eigenmodes in Parallel cavity, gun, SRF, coupling 875
 
  • A. Arnold
    FZD, Dresden
 
 

To fulfil the demand of future high power and high luminosity FEL and Storage Ring sources, an intensive electron beam with short bunch length, small emittance and large bunch charge is required. Laser driven superconducting radio frequency (SRF) photocathode guns in combination with SRF LINACs appear to be the best solution. First long term operation was demonstrated at the FZD*. In difference to the normal conducting guns, the application of static magnetic fields is not possible. Instead, the use of a transverse electric (TE) mode in parallel to the accelerating mode was proposed. Numerical simulations have shown that such RF focusing can be applied to compensate emittance growth**. This contribution will introduce a possibility to use the existing coaxial RF coupler of TESLA like cavities, as RF power input for TE modes in parallel. An additional coupler component outside the module satisfies the job of combining two frequencies from different sources to one load. Thus, it corresponds to the working principle of a high power RF diplexer. Based on the 3 1/2 cell FZD SRF gun, a concrete technical implementation and results of its operation at the cold cavity will be presented.


* J. Teichert et al., AIP Conf. Proc. 1149, 1119 - 1124 (2009).
** K. Flöttmann, D. Janssen, V. Volkov, Phys. Rev. ST Accel. Beams 7, 090702 (2004).

 
THP120 First Test Result of the IHEP-01 Large Grain 9-Cell Cavity cavity, niobium, SRF, target 1022
 
  • J. Gao, J.P. Dai, Z.D. Guo, M. Hou, Z.Q. Li, L.L. Men, Q.Y. Wang, Q. Xiao, J.Y. Zhai
    IHEP Beijing, Beijing
  • H. Hayano, E. Kako, S. Noguchi, M. Sawabe, T. Shishido, N. Toge, K. Watanabe, Y. Yamamoto
    KEK, Ibaraki
  • T.X. Zhao
    IHEP Beiing, Beijing
 
 

The combination of the low-loss shape and large grain niobium material is expected to be the possible way to achieve higher gradient and lower cost for ILC 9-cell cavities. As the key component of the 'IHEP 1.3 GHz SRF Accelerating Unit and Horizontal Test Stand Project', a low-loss shape 9-cell cavity using Ningxia large grain niobium (IHEP-01) was fabricated and surface treated (CBP, CP, annealing, pre-tuning) at IHEP. Then the cavity was shipped to KEK STF for ultrasonic cleaning, high pressure rinsing, baking and vertical test. The cavity reached 20 MV/m in the first vertical test on July 1st 2010. The quench location has been found by T-mapping and optical inspection. The strong field emission and equator defects will be removed by further treatment. The fabrication procedure, surface treatment recipes and the first test results are summarized in this paper.