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HOM

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TU3RAI01 SRF Experience with the Cornell High-Current ERL Injector Prototype cavity, cryomodule, SRF, cryogenics 694
 
  • M. Liepe
    Cornell University, Ithaca, New York
  • S.A. Belomestnykh, E.P. Chojnacki, Z.A. Conway, V. Medjidzade, H. Padamsee, P. Quigley, J. Sears, V.D. Shemelin, V. Veshcherevich
    CLASSE, Ithaca, New York
 
 

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


Cornell University has developed and fabricated a SRF injector cryomodule for the acceleration of the high current (100 mA) beam in the Cornell ERL injector prototype. The injector cryomodule is based on superconducting rf technology with five 2-cell rf cavities operated in cw mode. To support the acceleration of a low energy, ultra low emittance, high current beam, the beam tubes on one side of the cavities have been enlarged to propagate Higher-Order-Mode power from the cavities to broadband rf absorbers located at 80 K between the cavities. The axial symmetry of these absorbers, together with two symmetrically placed input couplers per cavity, avoids transverse on-axis fields, which would cause emittance growth. Each cavity is surrounded by a LHe vessel and equipped with a frequency tuner including fast piezo-driven fine tuners for fast frequency control. The cryomodule provides the support and precise alignment for the cavity string, the 80 K cooling of the ferrite loads, and the 2 K LHe cryogenic system for the high cw heat load of the cavities. In this paper results of the commissioning phase of this injector cryomodule will be reported.

 

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TU5PFP006 Wakefield Damping for the CLIC Crab Cavity cavity, dipole, damping, wakefield 815
 
  • P.K. Ambattu, G. Burt, R.G. Carter, A.C. Dexter
    Cockcroft Institute, Lancaster University, Lancaster
  • V.A. Dolgashev
    SLAC, Menlo Park, California
  • R.M. Jones, V.F. Khan
    UMAN, Manchester
 
 

Funding: The work is supported by STFC


A crab cavity is required in the CLIC to allow effective head-on collision of bunches at the IP. A high operating frequency (X-band) for the crab cavity is preferred as the deflection voltage required and the RF phase tolerance are inversely proportional to the operating frequency. However, the strong inter-bunch wakefields deteriorate the quality of the colliding bunches. The short bunch spacing of the CLIC scheme and the crab cavity's high sensitivity to dipole kicks demands very high damping of the inter-bunch wakes. A crab cavity requires special attention to the damper design as its wakefield spectrum is entirely different from that of an accelerating cavity. In addition to the higher-order modes, the orthogonally polarised dipole mode (same order mode) and the fundamental monopole mode (lower order mode) also need to be damped, however their resonant frequencies make damping these modes complicated. The same order mode suppression requires the use of an azimuthally asymmetric damper. This paper investigates the nature of the wakefields in the CLIC crab cavity and the possibility of using choke-mode damping and various types of waveguide damping to suppress them effectively.

 
TU5PFP008 RF Measurements on Variations of the ALBA Dampy Cavity cavity, impedance, vacuum, storage-ring 821
 
  • M.L. Langlois, M. Cornelis, D. Einfeld, F. Peréz
    CELLS-ALBA Synchrotron, Cerdanyola del Vallès
 
 

The Dampy cavity, operating at 500 MHz and up to 160 kW, normal conducting HOM damped, will be used in the ALBA storage ring. The pre-series has shown two problems. First, the HOM damping is very efficient but for one mode. The longitudinal impedance of the E011 mode was found to be around 11 kΩ, slightly above ALBA stability threshold. Second, overheating close to the dampers flanges induces a vacuum leak after several thermal cyclings. The maximum achieved operational dissipated power is 40 kW, if power is further increased a leak opens at one of the dampers flanges. In order to alleviate this latter drawback, two modifications have been implemented in two different cavities. The pre-series has been provided with short-circuits bridging waveguide ridges and cavity body. These are supposed to decrease the current in the area of the flanges. The first production cavity features a reduced thermal impedance between the water cooling channels and the area of overheating by replacing stainless steel by copper in the critical area. Both these cavities are currently under test and this paper will show the results.

 
TU5PFP036 Design of the Fundamental Mode Damper and the HOM Dampers for the 56 MHz SRF Cavity cavity, simulation, SRF, higher-order-mode 900
 
  • H. Hahn, S. Bellavia, I. Ben-Zvi, E. M. Choi
    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 56 MHz Superconducting RF cavity is developed for the luminosity enhancement of the Relativistic Heavy Ion Collider (RHIC). The 56 MHz SRF cavity enables to adiabatically rebucket the beam from the 28 MHz accelerating cavities, which with shorter bunch lengths will enhance the luminosity significantly. The 56 MHz SRF cavity fundamental mode must be damped during injection and acceleration by a fundamental mode damper (FD), which is physically withdrawn at store for operation. The cavity frequency changes from the withdrawing motion but is kept below the beam frequency at store by a judicious axial placement of the FD. Physics studies by numerical simulations, tests of the FD in the prototype cavity, and the challenging engineering issues are here addressed. In addition, higher-order mode (HOM) dampers are necessary for the stable operation of the 56 MHz SRF cavity. The HOM’s are identified and the external Q factors are obtained from tests of the prototype cavity and are compared to simulations with the CST MWS program. The HOM damper blocks the fundamental mode by a 5 element high pass filter. The HOM stability criteria of the cavity are satisfied with four HOM dampers.

 
TU5PFP040 Novel Geometries for the LHC Crab Cavity cavity, damping, dipole, radio-frequency 909
 
  • B.D.S. Hall, G. Burt
    Cockcroft Institute, Lancaster University, Lancaster
  • R. Calaga
    BNL, Upton, Long Island, New York
  • J.R. Delayen, R.A. Rimmer, H. Wang
    JLAB, Newport News, Virginia
  • J.D.A. Smith
    Lancaster University, Lancaster
 
 

In 2017 the LHC is envisioned to increase is luminosity via an upgrade. This upgrade is likely to require a large crossing angle hence a crab cavity is required to align the bunches prior to collision. There are two possible schemes for crab cavity implementation, global and local. In a global crab cavity the crab cavity is far from the IP and the bunch rotates back and forward as it traverses around the accelerator in a closed orbit. For this scheme a two cell elliptical squashed cavity at 800 MHz is preferred. To avoid any potential beam instabilities all the modes of the cavities must be damped strongly, however crab cavities have lower order and same order modes in addition to the usual higher order modes and hence a novel damping scheme must be used to provide sufficient damping of these modes. In the local scheme two crab cavities are placed at each side of the IP two start and stop rotation of the bunches. This would require crab cavities much smaller transversely than in the global scheme but the frequency cannot be increased any higher due to the long bunch length of the LHC beam. This will require a novel compact crab cavity design.

 
TU5PFP048 Robustness of the Superconducting Multicell Cavity Design for the Cornell Energy Recovery Linac cavity, linac, dipole, damping 933
 
  • M. Liepe, G.Q. Stedman, N.R.A. Valles
    Cornell University, Ithaca, New York
 
 

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


Cornell University is developing an Energy-Recovery-Linac driven x-ray light source. One of the major components of this accelerator will be its 5 GeV superconducting main linac. The design of the superconducting RF cavities in this main linac has been optimized primarily for two objectives: (1) low RF losses from the accelerating mode to minimize refrigeration cost and (2) strong Higher-Order-Mode damping to preserve low emittance and prevent beam break-up at high beam current (100 mA). In this paper we study the robustness of this optimized cavity design with respect to small cell shape fluctuations from fabrication errors.

 
TU5PFP051 Superconducting Multicell Cavity Design for the Energy Recovery Linac at Cornell cavity, linac, dipole, damping 939
 
  • V.D. Shemelin, M. Liepe
    CLASSE, Ithaca, New York
 
 

Funding: DOE


The first phase of the Cornell Energy Recovery Linac was the high current, low emittance injector. At present the injector is under commissioning. The next phase calls for the development of multicell cavity for the main linac. The cavities need to have low RF losses to minimize refrigeration and strong HOM damping to preserve low emittance and prevent beam break-up at high current (100 mA). Here we present the RF design of the cavity meeting these requirements.

 
TU5PFP053 Cryogenic Test of a Coaxial Coupling Scheme for Fundamental and Higher Order Modes in Superconducting Cavities cavity, coupling, damping, vacuum 945
 
  • J.K. Sekutowicz
    DESY, Hamburg
  • P. Kneisel
    JLAB, Newport News, Virginia
 
 

A coaxial coupling device located in the beam pipe of the TESLA type superconducting cavities provides for better propagation of Higher Order Modes (HOMs) and their strong damping in appropriate HOM couplers. Additionally, it also provides efficient coupling for fundamental mode RF power into the superconducting cavity. The whole coupling device can be designed as a detachable system. If appropriately dimensioned, the magnetic field can be minimized to a negligible level at the flange position. This scheme, presented previously*, provides for several advantages: strong HOM damping, flangeable solution, exchangeability of the HOM damping device on a cavity, less complexity of the superconducting cavity, possible cost advantages. This contribution will describe the results of the first cryogenic test.


*J. Sekutowicz et al., Proceedings LINAC08, Victoria, Canada, 2008.

 
TU5PFP058 Construction of a 3.9 GHz Superconducting RF Cavity Module at Fermilab cavity, vacuum, cryomodule, SRF 957
 
  • H.T. Edwards, T.T. Arkan, M.H. Foley, M. Ge, E.R. Harms, A. Hocker, T.N. Khabiboulline, M.W. McGee, D.V. Mitchell, D.R. Olis, A.M. Rowe, N. Solyak
    Fermilab, Batavia
 
 

Funding: Work supported by the U.S. Department of Energy under contract No. DE-AC02-07CH11359.


Fermilab is in a collaboration with DESY to provide a cryomodule containing 4-3.9 GHz superconducting RF cavities to be placed in TTF/FLASH. The purpose of this 'Third Harmonic' module is to linearize the nonlinear beam energy-time profile produced by the 1.3 GHz accelerating gradient. The completed module has now been shipped to DESY and is awaiting cold, powered testing and installation into FLASH later this year. We report on experience with fabricating, testing, assembling, and shipping the module and its components with a focus on cavity test results.

 
TU5PFP061 Improved Input and Output Couplers for SC Acceleration Structure cavity, emittance, cryomodule, linac 966
 
  • V.P. Yakovlev, I.G. Gonin, T.N. Khabiboulline, A. Latina, A. Lunin, V. Poloubotko, N. Solyak
    Fermilab, Batavia
 
 

Different couplers are described that allow the reduction of both transverse wake potential and RF kick in the SC acceleration structure of ILC. A simple rotation of the couplers reducing the RF kick and transverse wake kick is discussed for both the main linac and bunch compressors, along with possible limitations of this method. Designs of a coupler unit are presented which preserve axial symmetry of the structure, and provide reduced both the RF kick and transverse wake field.

 
TU5PFP064 SC Crab Cavity with Reduced Transverse Size for the LHC Upgrade cavity, dipole, impedance, damping 975
 
  • V.P. Yakovlev, I.G. Gonin, T.N. Khabiboulline, N. Solyak
    Fermilab, Batavia
 
 

In the paper the Crab Cavity is described for local Crab schemes for LHC that demand reduced transverse cavity dimensions small enough to fit limited space necessary for the beams separation. The results of the configuration cavity optimization are presented that include (a) the surface field minimization; (b) parasitic monopole and dipole spectrum optimization and dumping, (c) the input and the parasitic mode damping couplers design. The results of multipacting simulations, which were performed in order to understand the possible gradient limitations, are discussed also.

 
TU5PFP071 Development of 2-Cell SC Cavity System for ERL Injector Linac at KEK cavity, cryomodule, pick-up, SRF 987
 
  • S. Noguchi, E. Kako, M. Satoh, T. Shishido, K. Umemori, K. Watanabe, Y. Yamamoto
    KEK, Ibaraki
 
 

A cryomodule including three 2-cell sc cavities was designed for the ERL injector Linac, which is operated at the beam energy of 10 MeV and the beam current of 100 mA. A prototype 2-cell cavity with two input coupler ports and four HOM couplers was fabricated. The double input couplers is to reduce the power per coupler and to keep a symmetric filed configuration around the coupler port. Required rf power in the input couplers is about 200 kW in the cw operation. First vertical test of the 2-cell cavity will be carried out in March.

 
TU5PFP092 Status and Upgrade Plan of High Power RF System for the PLS Storage Ring cavity, klystron, storage-ring, status 1048
 
  • M.-H. Chun, M.H. Jung, I.S. Park, Y.U. Sohn, I.H. Yu
    PAL, Pohang, Kyungbuk
 
 

Funding: Supported by the Korea Ministry of Science and Technology mhchun@postech.ac.kr


The RF system for the Pohang Light Source (PLS) storage ring is operating at total maximum RF power of 300kW with four 75kW klystron amplifiers and four PF-type normal conductivity(NC) RF cavities for 190mA at 2.5GeV. The PLS will be upgraded from 2.5GeV/200mA to 3.0GeV/400mA in the near future. Therefore the RF system should be greatly upgraded to supply total 627kW beam power. We are investigated the some upgrade ways with adding NC cavities or new super conductivity(SC) RF cavities. According to the cavity type, the high power RF system will be adjusted the total RF power, and source type and quantity such as klystron or IOT. This paper describes the present operation status and several optional ways of high power RF system for the upgrade project of PLS storage ring



 
TU5PFP098 The Elettra Radiofrequency System Status and Developments cavity, storage-ring, booster, resonance 1066
 
  • C. Pasotti, M. Bocciai, L. Bortolossi, A. Fabris, M. Ottobretti, M. Rinaldi, R. Visintini
    ELETTRA, Basovizza
 
 

The full energy injection is now the standard procedure for the Elettra synchrotron radiation light source. The four RF storage ring plants have been benefited by this procedure in terms of reliability and stability of operation. The injector booster RF plant is running well. A new High Order Mode (HOM) diagnostic board has been implemented using the radiofrequency (RF) cavity’s signal to improve the HOM’s detection. The analysis and the performances of the new Inductive Output Tube (IOT)based RF power transmitter are presented.

 
TU6PFP040 A Compact Ring for Thom X-Ray Source cavity, dipole, emittance, impedance 1372
 
  • C. Bruni, Y. Fedala, J. Haissinski, M. Lacroix, B. Mouton, R. Roux, A. Variola, Z.F. Zomer
    LAL, Orsay
  • E. Bressi
    CNAO Foundation, Milan
  • P. Brunelle, M.-E. Couprie, J.-C. Denard, N. Guillotin, P. Lebasque, A. Loulergue, P. Marchand, F. Marteau, R. Nagaoka
    SOLEIL, Gif-sur-Yvette
  • P. Gladkikh
    NSC/KIPT, Kharkov
 
 

The goal of X-ray sources based on Compton back scattering processes is to develop a compact device, which could produce an intense flux of monochromatic X-rays. Compton back-scattering resuls from collisions between laser pulses and relativistic electron bunches. Due to the relative low value of the Compton cross section, a high charge electron beam, a low emittance and a high focusing at the interaction point are required for the electron beam. In addition, the X-ray flux is related to the characteristics of the electron beam, which are themselves dynamically affected by the Compton interaction. One possible configuration is to inject frequently into a storage ring with a low emittance linear accelerator without waiting for the synchrotron equilibrium. As a consequence, the optics should be designed taking into account the characteristics of the electron beam from the linear accelerator. The accelerator ring design for a 50 MeV electron beam, aiming at producing a flux higher than 1013 ph/s, will be presented.

 
WE2PBC04 Coupler Kicks in the Third Harmonic Module for the XFEL cavity, wakefield, simulation, acceleration 1858
 
  • E. Gjonaj, W. Ackermann, T. Lau, T. Weiland
    TEMF, TU Darmstadt, Darmstadt
  • M. Dohlus
    DESY, Hamburg
 
 

The rf and wakefield transverse kicks resulting from the asymmetry of input and HOM couplers in the third harmonic module for the XFEL are investigated. The fundamental mode is computed using eigenvalue analysis. The short range wakefields in a string of cavities are simulated with the PBCI code. Using the simulation data, the transverse kick factors associated with the presence of cavity couplers are evaluated.


* P. Pierini, "Third Harmonic Superconducting Cavity Prototypes for the XFEL", LINAC08.
** T. Khabiboulline, "New HOM Coupler Design For 3.9 Ghz Superconducting Cavities At FNAL", PAC07.

 

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WE5PFP015 Upgrade of the RF System of Siberia-2 Electron Storage Ring / SR Source cavity, storage-ring, impedance, electron 2018
 
  • I.K. Sedlyarov, V.S. Arbuzov, E.I. Gorniker, A.A. Kondakov, S.A. Krutikhin, I.V. Kuptsov, G.Y. Kurkin, S.V. Motygin, V.M. Petrov, A.M. Pilan, A.G. Tribendis, N. Vinokurov
    BINP SB RAS, Novosibirsk
  • V. Korchuganov
    RRC, Moscow
 
 

The project of upgraded RF System of Siberia-2 Electron Storage Ring / SR Source, Moscow, Russia, is presented. The upgraded RF system will allow to increase the total accelerating voltage up to 1.8MV and ensure operation of the storage ring with new superconducting wiggler at beam currents up to 0.3A. RF system operates at 181MHz. It consists of 3 single bi-metal cavities, 2 power amplifiers based on GU-101A tetrodes with output power of 200kW, power transmission lines and control system. Parameters of the upgraded RF system are given, the design of its main elements is shown.

 
WE5PFP018 Results from the CLIC X-Band Structure Test Program at NLCTA damping, linear-collider, collider, linac 2027
 
  • C. Adolphsen, G.B. Bowden, V.A. Dolgashev, L. Laurent, S.G. Tantawi, F. Wang, J.W. Wang
    SLAC, Menlo Park, California
  • S. Döbert, A. Grudiev, G. Riddone, W. Wuensch, R. Zennaro
    CERN, Geneva
  • Y. Higashi, T. Higo
    KEK, Ibaraki
 
 

Funding: Work supported by the DOE under contract DE-AC02-76SF00515


As part of a SLAC-CERN-KEK collaboration on high gradient X-band structure research, several prototype structures for the CLIC linear collider study have been tested using two of the high power (300 MW) X-band rf stations in the NLCTA facility at SLAC. These structures differ in terms of their manufacturing (brazed disks and clamped quadrants), gradient profile (amount by which the gradient increases along the structure which optimizes efficiency and maximizes sustainable gradient) and HOM damping (use of slots or waveguides to rapidly dissipate dipole mode energy). The CLIC goal in the next few years is to demonstrate the feasibility of a CLIC-ready baseline design and to investigate alternatives which could bring even higher efficiency. This paper summarizes the high gradient test results from the NLCTA in support of this effort.

 
WE5PFP035 Prototyping PEFP Low-Beta Copper Cavity and HOM Coupler cavity, damping, controls, SRF 2070
 
  • S. An, Y.-S. Cho, B.H. Choi, Y.M. Li, Y.Z. Tang, L. Zhang
    KAERI, Daejon
 
 

Funding: This work is supported by the Ministry of Education, Science and Technology of Korea.


A superconducting radio frequency (SRF) cavity with a geometrical beta of 0.42 has been designed to accelerate a proton beam after 100 MeV at 700 MHz for an extended project of Proton Engineering Frontier Project (PEFP). In order to confirm the RF and mechanical properties of the cavity, and to produce documentation for a procurement and quality control for an industrial manufacture of the cavities, two prototype copper cavities have been produced, tuned and tested. In this paper, the copper cavity’s production, tuning and testing are introduced. The testing results show that the low-beta cavity and its tuning system can work as we design.

 
WE5PFP040 SRF Activities for ILC at MHI cavity, superconducting-cavity, niobium, SRF 2083
 
  • K. Sennyu, H. Hara, K. Kanaoka, M. Matsuoka, T. Yanagisawa
    MHI, Kobe
 
 

We report on the activities and achievements at MHI about cavity fabrication for ILC. Some new procedures of cavity fabrication for industrialization are reported.

 
WE5PFP041 1500 MHz Passive SRF Cavity for Bunch Lengthening in the NSLS-II Storage Ring cavity, SRF, damping, coupling 2086
 
  • J. Rose
    BNL, Upton, Long Island, New York
  • A.E. Bogle, T.L. Grimm
    Niowave, Inc., Lansing, Michigan
  • T. Yanagisawa
    MHI, Kobe
 
 

NSLS-II is a new ultra-bright 3GeV 3rd generation synchrotron radiation light source. The performance goals require operation with a beam current of 500mA and a bunch current of at least 0.5mA. Ion clearing gaps are required to suppress ion effects on the beam. The natural bunch length of 3mm is planned to be lengthened by means of a third harmonic cavity in order increase the Touschek limited lifetime. After an extensive investigation of different cavity geometries a passive, superconducting 2-cell cavity has been selected for prototyping. The cavity is HOM damped with ferrite absorbers on the beam-pipes. The 2-cell cavity simplifies the tuner design as compared to two independent cells. Tradeoffs between the damping of the higher order modes, thermal isolation associated with the large beam tubes and overall cavity length are described. A copper prototype has been constructed and measurements of fundamental and higher order modes will be compared to calculated values.

 
WE5PFP043 Beam Pipe HOM Absorber for 750 MHz RF Cavities cavity, SRF, factory, higher-order-mode 2092
 
  • M.L. Neubauer, R. Sah
    Muons, Inc, Batavia
  • E.P. Chojnacki, M. Liepe
    CLASSE, Ithaca, New York
  • H. Padamsee
    Cornell University, Ithaca, New York
 
 

Funding: Supported in part by USDOE Contract. DE-AC05-84-ER-40150


Superconducting HOM-damped (higher-order-mode-damped) RF systems are needed for present and future storage ring and linac applications. Superconducting RF (SRF) systems typically contain unwanted frequencies or higher order modes (HOM) that must be absorbed by ferrite and other lossy ceramic-like materials that are brazed to substrates mechanically attached to the drift tubes adjacent to the SRF cavity. These HOM loads must be thermally and mechanically robust and must have the required broadband microwave loss characteristics, but the ferrites and their attachments are weak under tensile stresses and thermal stresses and tend to crack. A HOM absorber with improved materials and design will be developed for high-gradient 750 MHz superconducting cavity systems. RF system designs will be numerically modeled to determine the optimum ferrite load required to meet the broadband loss specifications. Several techniques for attaching ferrites to the metal substrates will be studied, including full compression rings and nearly-stress-free ferrite assemblies. Prototype structures will be fabricated and tested for mechanical strength.

 
WE5PFP047 A Compact Alternative Crab Cavity Design at 400-MHz for the LHC Upgrade cavity, damping, simulation, electron 2104
 
  • Z. Li, L. Xiao
    SLAC, Menlo Park, California
 
 

Funding: This work was supported by DOE Contract No. DE-AC02-76SF00515 and used resources of NERSC supported by DOE Contract No. DE-AC02-05CH11231, and of NCCS supported by DOE Contract No. DE-AC05-00OR22725.


Crab cavities are proposed for the LHC upgrade to improve the luminosity. In the local crabbing scheme, the crab cavities are located close to the interaction region and the transverse separation between the two beam lines at the crab cavity location can only accommodate an 800-MHz cavity of the conventional elliptical shape. Thus the baseline crab cavity design for the LHC upgrade is focused on the 800-MHz elliptical cavity shape although a lower frequency cavity is preferable due to the long bunch length. In this paper, we present a compact 400-MHz design as an alternative to the 800-MHz baseline design. The compact design is of a half-wave resonator (HWR) shape that has a small transverse dimension and can fit into the available space in the local crabbing scheme. The optimization of the HWR cavity shape and the couplers for the HOM, LOM, and SOM damping will be presented.

 
WE5PFP048 800MHz Crab Cavity Conceptual Design for the LHC Upgrade cavity, coupling, simulation, damping 2107
 
  • L. Xiao, Z. Li, C.-K. Ng, A. Seryi
    SLAC, Menlo Park, California
 
 

Funding: This work was supported by DOE Contract No. DE-AC02-76SF00515 and used resources of NERSC supported by DOE Contract No. DE-AC02-05CH11231, and of NCCS supported by DOE Contract No. DE-AC05-00OR22725.


In this paper, we present a 800MHz crab cavity conceptual design for LHC upgrade, including the cell shape optimization, and LOM, SOM, HOM and input coupler design. The compact coax-to-coax coupler scheme is proposed to couple to the LOM and SOM modes which can provide strong coupling to the LOM and SOM modes. HOM coupler design uses a two-stub antenna with a notch filter to couple to the HOM modes in the horizontal plane and reject the operating mode at 800MHz. All the damping results for the LOM/SOM/HOM modes satisfy their damping requirements. The multipacting in cell and couplers is simulated as well. And the issue of the cross-coupling between the input coupler and LOM/SOM couplers due to cavity asymmetry is addressed. The power coming out of the LOM/SOM/HOM couplers are estimated. All the simulations are carried out using SLAC developed parallel EM simulation codes Omega3P, S3P and Track3P.

 
WE5PFP050 Preparations for Assembly of the International ERL Cryomodule at Daresbury Laboratory cryomodule, cavity, cryogenics, SRF 2113
 
  • P.A. McIntosh, R. Bate, C.D. Beard, D.M. Dykes, S.M. Pattalwar
    STFC/DL/ASTeC, Daresbury, Warrington, Cheshire
  • S.A. Belomestnykh, M. Liepe, H. Padamsee, J. Sears, V.D. Shemelin, V. Veshcherevich
    CLASSE, Ithaca, New York
  • A. Büchner, F.G. Gabriel, P. Michel
    FZD, Dresden
  • M.A. Cordwell, J. Strachan
    STFC/DL, Daresbury, Warrington, Cheshire
  • J.N. Corlett, D. Li, S.M. Lidia
    LBNL, Berkeley, California
  • T. Kimura, T.I. Smith
    Stanford University, Stanford, California
  • D. Proch, J.K. Sekutowicz
    DESY, Hamburg
  • A. Quigley
    STFC/DL/SRD, Daresbury, Warrington, Cheshire
 
 

The collaborative development of an optimised cavity/cryomodule solution for application on ERL facilities, has now progressed to final assembly and testing of the cavity string components and their subsequent cryomodule integration. This paper outlines the verification of the various cryomodule sub-components and details the processes utilised for final cavity string integration. The paper also describes the modifications needed to facilitate this new cryomodule installation and ultimate operation on the ALICE facility at Daresbury Laboratory.

 
WE5PFP053 Design of Superconducting Parallel Bar Deflecting and Crabbing RF Structures cavity, damping, simulation, RF-structure 2120
 
  • J.R. Delayen, 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


A new concept for a deflecting and crabbing rf structure based on half-wave resonant lines was introduced recently*. It offers significant advantages to existing designs and, because of it compactness, allows low frequency operation. This concept has been further refined and optimized for superconducting implementation. Results of this optimization and application to a 400 MHz crabbing cavity and a 499 MHz deflecting cavity are presented.


*A New TEM-Type Deflecting and Crabbing RF Structure, J. R. Delayen and H. Wang, Proc. LINAC08

 
WE5PFP054 HOM Survey of the First CEBAF Upgrade Style Cavity Pair cavity, impedance, cryomodule, dipole 2123
 
  • F. Marhauser, E. Daly, G.K. Davis, M.A. Drury, C. Grenoble, J. Hogan, R. Manus, J.P. Preble, C.E. Reece, R.A. Rimmer, K. Tian, H. Wang
    JLAB, Newport News, Virginia
 
 

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


For the planned CEBAF upgrade ten new cryomodules are required to increase the beam energy to the envisaged 12 GeV. Extensive cavity and cryomodule R&D has been done previously, including the installation of a new cryomodule dubbed “Renascence” in CEBAFs north linac in 2007. It houses both seven-cell low loss and high gradient type of cavities thereby serving as a testbed to address and cope with crucial technological challenges. Based on this experience a final iteration on the upgrade cavity has been performed to improve various aspects of HOM-damping and thermal stability. Two such cavities have been produced and qualified. A thorough cavity HOM-survey has been performed to verify the integrity of the cavities and to guarantee the impedance requirements of each crucial HOM. This paper details the results of HOM-surveys performed for the first two upgrade style low loss cavities tested both individually in a vertical Dewar and horizontally in a dedicated cavity pair cryomodule. The safety margin to the worst beam break-up scenario at 12 GeV has been concluded.

 
WE5PFP055 Improved Performance of JLab 7-Cell Cavities by Electropolishing cavity, niobium, SRF, accelerating-gradient 2126
 
  • C.E. Reece, A.C. Crawford, R.L. Geng
    JLAB, Newport News, Virginia
 
 

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


The great majority of experience in niobium SRF cavity processing at Jefferson Lab is with BCP etching. This has been used on CEBAF cavities and others totaling over 500 in number. With improved process quality control, field emission is now largely controlled and other factors limit performance. All of the prototype cavities developed for the 12 GeV upgrade, although meeting minimum requirements, have demonstrated a Q-drop in the 17 – 23 MV/m range that is not remedied by 120 C bake. Most of these cavities received >250 micron removal by BCP etch. Three of these cavities are being electropolished using the protocol under development within ILC R&D activities. The first such cavity was transformed from Q = 3 ·1010 at 17 MV/m to quench from 1010 at 35 MV/m. The details of this and two subsequent electropolished JLab 7-cell cavities will be reported.

 
WE5PFP056 A Family of L-Band SRF Cavities for High Power Proton Driver Applications cavity, damping, cryomodule, impedance 2129
 
  • R.A. Rimmer, F. Marhauser
    JLAB, Newport News, Virginia
 
 

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


Recent global interest in high duty factor or CW superconducting linacs with high average beam power highlights the need for robust and reliable SRF structures capable of delivering high average RF power to the beam with moderate HOM damping, low interception of halo and good efficiency. Potential applications include proton or H- drivers for spallation neutron sources, neutrino physics, waste transmutation, subcritical reactors, and high-intensity high-energy physics experiments. We describe a family of SRF cavities with a range of Betas capable of transporting beam currents in excess of 10 mA CW with large irises for minimal interception of halo and HOM and power couplers capable of supporting high average power operation. Goals include an efficient cell shape, high packing factor for efficient real-estate gradient and strong HOM damping to ensure stable beam operation. Designs are being developed for low-frequency (e.g. 650-975 MHz), but can easily be scaled to high-frequency (e.g. 1.3-1.5 GHz), depending on the application. We present the results of conceptual design studies, simulations and prototype measurements.

 
WE6RFP002 Design of an ERL Linac Cryomodule cavity, linac, cryomodule, SRF 2781
 
  • E.P. Chojnacki, S.A. Belomestnykh, S.S. Chapman, R.D. Ehrlich, G.H. Hoffstaetter, M. Liepe, H. Padamsee, J. Sears, E.N. Smith, V. Veshcherevich
    CLASSE, Ithaca, New York
 
 

Funding: Work supported by NSF, New York State, and Cornell University


A cryomodule design for the Cornell Energy Recovery Linac (ERL) will be based on TTF technology, but must have several unique features dictated by the ERL beam parameters. The main deviations from TTF are that the HOM loads must be on the beamline for sufficient damping, that the average power through the RF couplers is low, and that cw beam operation introduces higher heat loads. Several of these challenges were addressed for the Cornell ERL Injector, from which fabrication and operational insight was gained. A baseline design for the Cornell ERL Linac cryomodule will be presented that includes fabrication and operational considerations along with thermal and mechanical analyses.

 
WE6RFP009 Investigations on Absorber Materials at Cryogenic Temperatures cavity, cryogenics, cryomodule, superconductivity 2799
 
  • F. Marhauser, T.S. Elliott, R.A. Rimmer
    JLAB, Newport News, Virginia
 
 

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


In the framework of the ongoing CEBAF 12 GeV upgrade program improvements are being made to refurbish cryomodules housing JLab’s original 5-cell cavities. Recently we have started to look into a possible simplification of the HOM-absorber design combined with the need to find alternative material candidates. The absorbers are implemented in two HOM-waveguides immersed in the helium bath and need to operate at 2K. We therefore have built a cryogenic setup to perform measurements on sample load materials to investigate their lossy characteristics and variations from room temperature down to 2K. Initial results are presented in this paper.

 
WE6RFP057 Wake Fields in Photonic Crystal Accelerator Structures and Application to RF Sources wakefield, cavity, lattice, 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.

 
WE6RFP081 Design of Advanced Photonic Bandgap (PBG) Structures for High Gradient Accelerator Applications damping, simulation, dipole, wakefield 2986
 
  • R.A. Marsh, B.J. Munroe, M.A. Shapiro, R.J. Temkin
    MIT/PSFC, Cambridge, Massachusetts
 
 

Funding: Work supported by DOE HEP, under contract DE-FG02-91ER40648


The design of advanced photonic bandgap (PBG) accelerator structures is examined. PBG structures are chosen for their wakefield damping. A potential disadvantage of PBG structures, as well as damped detuned structures, is the increased wall currents at the structure surface due to the reduced surface area, leading to higher pulsed wall heating. Research is carried out to improve the pulsed heating performance of PBG structure concepts while maintaining higher order mode damping. Wakefield damping parameters are discussed and a quantitative figure of merit is expressed to evaluate and compare PBG concepts. Pulsed heating performance in PBG structures is improved by breaking perfect symmetry and allowing deformation of both rod and lattice geometry. A final design for an improved pulsed heating performance PBG structure for breakdown testing at 11.424 GHz is presented and discussed.

 
WE6RFP082 Design of Photonic Bandgap (PBG) Accelerator Structures with Reduced Symmetry dipole, damping, simulation, wakefield 2989
 
  • B.J. Munroe, R.A. Marsh, M.A. Shapiro, R.J. Temkin
    MIT/PSFC, Cambridge, Massachusetts
 
 

Funding: Work supported by DOE HEP, under contract DE-FG02-91ER40648


The design of a new photonic bandgap (PBG) accelerator structure based on a pentagonal array of rods is presented. The goal of this structure is to damp the higher order modes (HOMs) present in the structure. By removing the bilateral symmetry present in the four and six rod PBG structures the five rod photonic quasi-crystal (PQC) structure is able to damp the symmetric dipole mode. The field pattern and mode Q factors for the fundamental and dipole modes are presented for various values of the ratio of rod radius to rod spacing. These results are compared to the equivalent results for the six rod structure. The ratio of the Q factors is also calculated, and found to show an optimal value near a rod radius to rod spacing ratio of 0.17 in both cases.

 
WE6RFP103 Development of X-band Photonic Band Gap Accelerating Structure cavity, coupling, simulation, damping 3041
 
  • Z.P. Li
    USTC, Hefei, Anhui
  • S. Dong, X.D. He, C.-F. Wu
    USTC/NSRL, Hefei, Anhui
 
 

Funding: National Nature Science Foundation of China, Grant No. 10675116 and 10375060


We present the new experimental results for an X-band (11.42GHz) metallic PBG accelerating cavity. A coupler of a single cavity was fabricated and cold tested. An X-band traveling-wave PBG accelerator was designed based on CST MWS transient analysis. The X-band PBG accelerator is now under construction, future work will focus on the structure to be cold tested and tuned.

 
TH4GBC06 X-Band Photonic Bandgap (PBG) Structure Breakdown Experiment klystron, accelerating-gradient, damping, wakefield 3163
 
  • R.A. Marsh, M.A. Shapiro, R.J. Temkin
    MIT/PSFC, Cambridge, Massachusetts
  • V.A. Dolgashev, S.G. Tantawi
    SLAC, Menlo Park, California
 
 

Funding: Work supported by DoE HEP, under contracts DE-FG02-91ER40648 and DE-AC02-76-SF00515


In order to understand the performance of photonic bandgap (PBG) structures under realistic high gradient operation, an X-band (11.424 GHz) PBG structure was designed for high power testing in a standing wave breakdown experiment at SLAC. The PBG structure was hot tested to gather breakdown statistics, and achieved an accelerating gradient of 65 MV/m at a breakdown rate of two breakdowns per hour at 60 Hz, and accelerating gradients above 110 MV/m at higher breakdown rates, for a total pulse length of 320 ns. High pulsed heating occurred in the PBG structure, with many shots above 270K, and an average of 170K for 35 x 106 shots. Damage was observed in scanning electron microscope imaging. No breakdown damage was observed on the iris surface, the location of peak electric field, but pulsed heating damage was observed on the inner rods, the location of magnetic fields as high as 1 MA/m. Breakdown in accelerator structures is generally understood in terms of electric field effects. PBG structure results highlight the unexpected role of magnetic fields on breakdown. We think that relatively low electric field in combination with high magnetic field on the rod surface may trigger breakdowns.

 

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Slides

 
TH5PFP045 SRF Cavity Geometry Optimization for the ILC with Minimized Surface E.M. Fields and Superior Bandwidth cavity, dipole, wakefield, higher-order-mode 3300
 
  • I.R.R. Shinton, R.M. Jones, N. Juntong
    UMAN, Manchester
 
 

The main linacs of the ILC consist of nine-cell cavities based on the TESLA design. In order to facilitate reaching higher gradients we have re-designed the cavity shape. This leads to a reduction, comparable to several current designs, in both the ratio of the surface electric field to the accelerating field (Es/Ea) and the magnetic field to the accelerating field (Bs/Ea). The bandwidth of the accelerating mode is also optimized. This new shape, which we refer to as the New Low Surface Field (NLSF) design, bears comparison with the Ichiro, Re-entrant and LSF designs.

 
TH5PFP088 HOM Sensitivity in the PEP-II HER Vacuum Chamber lattice, 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.

 
TH5PFP089 Trapped Mode Study for a Rotatable Collimator Design for the LHC Upgrade vacuum, simulation, damping, collimation 3416
 
  • L. Xiao, C.-K. Ng, J.C. Smith
    SLAC, Menlo Park, California
  • F. Caspers
    CERN, Geneva
 
 

Funding: This work was supported by DOE Contract No. DE-AC02-76SF00515 and used resources of NERSC supported by DOE Contract No. DE-AC02-05CH11231, and of NCCS supported by DOE Contract No. DE-AC05-00OR22725.


A rotatable collimator is proposed for the LHC phase II collimation upgrade. When the beam crosses the collimator, trapped modes will be excited that result in beam energy loss and collimator power dissipation. Some of the trapped modes can also generate transverse kick on the beam and affect the beam operation. In this paper the parallel eigensolver code Omega3P is used to search for all the trapped modes below 2GHz in the collimator, including longitudinal modes and transverse modes. The loss factors and kick factors of the trapped modes are calculated as function of the jaw positions. The amplitude ratio between transverse and longitudinal trapped mode intensity can be used as a direct measure of the position of the beam. We present simulation results and discuss the results.

 
TH6REP004 Development of a Fast Signal-Gating Circuit for Observation of Fast Glitch of Photon Beam Intensity at NSRRC photon, controls, feedback, SRF 3956
 
  • F.-T. Chung, H.-P. Chang, Y.K. Lin, Y.-H. Lin, Y.-C. Liu, C.H. Lo, Ch. Wang, M.-S. Yeh
    NSRRC, Hsinchu
 
 

Stability of photon beam intensity, I0, is one of the most important performance merits of a modern light source. The photon intensity measured at dragon beam line (BL11) is routinely used as a reference signal for I0 stability measurements. At NSRRC, a highly stable I0 intensity is maintained in most percentage of the user beam time. Meanwhile, glitches of I0 intensity up to few tens of percentage had been observed once every few operating hours, which was a puzzle before its reason had been identified later. A spontaneous large variation of photon intensity (I/I0) caused difficulties for users operating their experiments. Here, we report our development of a dedicated electronic circuit with functionality of single-gate, which was very helpful to clarify the puzzle of I0 glitches observed at NSRRC.

 
TH6REP034 Evaluation of Bergoz Instrumentation NPCT vacuum, instrumentation, cavity, radio-frequency 4021
 
  • D.J. Martin, S. Allison, B. Scott, J.J. Sebek, T.A. Trautwein
    SLAC, Menlo Park, California
 
 

Funding: Operated by Stanford University for the U. S. Department of Energy under Contract DE-AC02-76-SF00515 and Office of Basic Energy Sciences.


The Bergoz Instrumentation New Parametric Current Transformer (NPCT) has been evaluated at the SPEAR3 synchrotron light source. The device was tested for vacuum performance and residual gas and was found suitable for installation in the storage ring. The NPCT was installed during August 2008 and has measured beam currents to 500 mA. Performance is compared to the earlier PCT design. The NPCT Sensor Head has been instrumented with thermal sensors for characterization of the internal operating temperature.

 
TH6REP087 Firmware Development for SNS New Timing Master simulation, neutron, target, controls 4162
 
  • R. Štefanič, J. Dedič
    Cosylab, Ljubljana
  • D. Curry
    ORNL RAD, Oak Ridge, Tennessee
  • D.H. Thompson
    ORNL, Oak Ridge, Tennessee
 
 

Funding: This manuscript has been authored by UT-Battelle, LLC, under contract DE-AC05-00OR22725 with the U.S. Department of Energy.


Implementation of a timing system master device is a complicated task, since a lot of details have to be taken into account even once the architecture decisions have been laid down. At SNS/ORNL timing master controller is being upgraded in collaboration with Cosylab and this paper focuses on some details of its implementation. New timing system master device is based on agile FPGA circuitry and the main focus of this paper is its firmware implementation. Provided are implementation details for event distribution supporting multiple event sources and priorities. Discussed are mechanisms, ensuring deterministic behavior, different methods of encoding that have been employed, and host-independent distribution of time stamp frames. The concept of the super-cycle is explained and its implementation is laid down. Taken into account that implementation for such a complex device involves extensive testing, paper provides insight into verification it was applied. Advantages of the SystemC based test-benches over traditional VHDL-only verification are discussed.

 
FR5PFP071 Thermal Analysis of SCRF Cavity Couplers Using Parallel Multiphysics Tool TEM3P cavity, simulation, vacuum, cryogenics 4473
 
  • V. Akcelik, K. Ko, L. Lee, Z. Li, C.-K. Ng
    SLAC, Menlo Park, California
  • G. Cheng, R.A. Rimmer, H. Wang
    JLAB, Newport News, Virginia
 
 

Funding: This work was supported by DOE Contract No. DE-AC02-76SF00515 and used resources of NERSC supported by DOE Contract No. DE-AC02-05CH11231, and of NCCS supported by DOE Contract No. DE-AC05-00OR22725.


SLAC has developed a multi-physics simulation code TEM3P for simulating integrated effects of electromagnetic, thermal and structural effects. TEM3P shares the same finite element infrastructure with EM finite elements codes developed at SLAC. This enables simulations within a single framework. Parallel implementation allows large scale computation, and high fidelity and high accuracy simulations can be performed in faster time. In this paper, TEM3P is used to analyze thermal loading in the coupler end-groups of the JLAB SCRF cavity. The results are benchmarked against measurements.

 
FR5PFP079 Highly Accurate Frequency Calculations of Crab Cavities Using the VORPAL Computational Framework cavity, simulation, extraction, collider 4493
 
  • T.M. Austin
    Tech-X, Boulder, Colorado
  • L. Bellantoni
    Fermilab, Batavia
  • J.R. Cary
    CIPS, Boulder, Colorado
 
 

Funding: US DOE, COMPASS SciDAC-2, Grant Number DE-FC02-07ER41499


We have applied the Werner-Cary method* for extracting modes and mode frequencies from time-domain simulations of crab cavities, as are needed for the ILC and the beam delivery system of the LHC. This method for frequency extraction relies on a small number of simulations and post-processing using the SVD algorithm with Tikhonov regularization. The time domain simulations were carried out using the VORPAL computational framework, which is based on the eminently scalable finite-difference time-domain algorithm. A validation study was performed on an aluminum model of the 3.9 GHz RF separators built originally at Fermi National Accelerator Laboratory in the US. Comparisons with measurements of the A15 cavity show that this method can provide accuracy to within 0.01% of experimental results after accounting for manufacturing imperfections. To capture the near degeneracies two simulations requiring in total a few hours on 600 processors were employed. This method has applications across many areas including obtaining MHD spectra from time-domain simulations.


*J. Comp. Phys. 227, 5200-5214 (2008)

 
FR5PFP086 HOM Maps of RF Cavities for Particle Tracking Codes cavity, simulation 4508
 
  • I.V. Pogorelov, D.T. Abell, P. Stoltz
    Tech-X, Boulder, Colorado
 
 

Funding: Supported in part by the DOE Office of Science, Office of High-Energy Physics under grant No. DE-FG02-06ER84485.


We present our recently developed capability for generating High-Order Mode (HOM) maps of rf cavity fields for use in particle tracking code-based simulations. We use VORPAL field data as a starting point, and follow the approach of* to produce the maps that are subsequently incorporated into the MaryLie/IMPACT and Synergia frameworks. We present and discuss the results of applying this new modeling tool to crab cavity simulations.


*D.T. Abell, "Numerical computation of high-order transfer maps for rf cavities", Phys. Rev. ST Accel. Beams 9, 052001, (2006).

 
FR5PFP091 Wakefield Computations with the PBCI Code Using a Non-Split Finite Volume Method controls, wakefield, cavity, simulation 4516
 
  • E. Gjonaj, T. Lau, T. Weiland
    TEMF, TU Darmstadt, Darmstadt
 
 

We report on a new numerical technique for the computation of geometrical wakes in three-dimensional LINAC structures. The method utilises an explicit Finite-Volume Time-Domain (FVTD) formulation. The numerical dispersion in all three axial directions is completely eliminated by choice of an appropriate staggering of the field components on the grid. Thus, contrary to most of the previously reported techniques no splitting of the time-evolution operator is necessary. This results in large savings in computational time as well as in an improved numerical accuracy. We have implemented this new technique in PBCI code and present some preliminary results.

 
FR5PFP094 Enhanced Method for Cavity Impedance Calculations impedance, cavity, wakefield, resonance 4523
 
  • F. Marhauser, R.A. Rimmer, K. Tian, H. Wang
    JLAB, Newport News, Virginia
 
 

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


With the proposal of medium to high average current accelerator facilities the demand for cavities with extremely low HOM impedances is increasing. Modern numerical tools are still under development to more thoroughly predict impedances that need to take into account complex absorbing boundaries and lossy materials. With the usually large problem size it is preferable to utilize massive parallel computing when applicable and available. Apart from such computational issues, we have developed methods using available computer resources to enhance the information that can be extracted from a cavities’ wake potential computed in time domain. In particular this is helpful for a careful assessment of the extracted RF power and the mitigation of potential beam breakup or emittance diluting effects, a figure of merit for the cavity performance. The methods are described as well as examples of their implementation.

 
FR5RFP002 Design of a 20.8/35.1 GHz Higher-Order-Mode Dielectric-Loaded Power Extractor Set electron, coupling, single-bunch, gun 4538
 
  • F. Gao, W. Gai, W. Liu
    ANL, Argonne
  • F. Gao, T. Wong
    Illinois Institute of Technology, Chicago, Illinois
  • C.-J. Jing
    Euclid TechLabs, LLC, Solon, Ohio
 
 

We report on the design of a dual-frequency higher-order-mode dielectric-loaded power extraction set. This power extraction set consists of a dual-frequency dielectric-loaded decelerating structure (decelerator) and two changeable output couplers. In the decelerator, the TM02 mode synchronizes with an ultra-relativistic electron beam at 20.8GHz, and the TM03 mode synchronizes with the beam at 35.1GHz. These frequencies are both harmonics of 1.3GHz, the operating frequency of the electron gun and linac at the Argonne Wakefield Accelerator. The power generated in the unwanted TM01 mode is effectively suppressed for bunch train operation with a novel mode suppression technique. To extract power from the decelerator to standard rectangular waveguides, a TM02-TE10 output coupler was designed with S21 = -0.26dB at 20.8GHz, and a TM03-TE10 output coupler with S21 = -0.66dB at 35.1GHz. 90.4MW and 8.68MW rf power are expected to be extracted from a drive beam with charge of 50nC per bunch, at 20.8GHz and 35.1GHz respectively.

 
FR5RFP031 Impedance Calculations for the NSLS-II Storage Ring impedance, vacuum, cavity, storage-ring 4595
 
  • A. Blednykh, M.J. Ferreira, S. Krinsky
    BNL, Upton, Long Island, New York
 
 

Impedance of two vacuum chamber components, Bellows and BPM, is considered in some detail. In order to avoid generation of Higher-Order Modes (HOM’s) in the NSLS-II bellows, we designed a new low-impedance RF shielding consisting of 6 wide and 2 narrow metal plates without opening slots between them. The short-range wakepotential has been optimized taking into account vertical offset of RF fingers from their nominal position. The results were compared with data of bellows designed at other laboratories. Narrow-band impedance of the BPM Button has been studied. TE-modes in the BPM button were suppressed by a factor of 8 by modification of existing housings. Two new types of housings are shown. The total impedance of the NSLS-II storage ring is discussed in terms of the loss factor and the vertical kick factor for a 3mm-Gaussian bunch.

 
FR5RFP045 Wake and Higher Order Mode Computations for CMS Experimental Chamber at the LHC vacuum, wakefield, higher-order-mode, betatron 4634
 
  • R. Wanzenberg
    DESY, Hamburg
  • E. Métral
    CERN, Geneva
 
 

Wakefields and trapped Higher Order Modes in the CMS experimental chamber at the LHC are investigated using a geometrical model which closely reflects the presently installed vacuum chamber. The basic rf-parameters of the higher order modes (HOMs) including the frequency, loss parameter,and the Q-value are provided. To cover also transient effects the short range wakefields and the total loss parameter has been calculated, too. Most numerical calculations are performed with the computer code MAFIA. The calculations of the Modes is complemented with an analysis of the multi-bunch instabilities due to the longitudinal and dipole modes in the CMS vacuum chamber.

 
FR5RFP086 Analysis of the Wake Field Effects in the PEP-II SLAC B-Factory vacuum, wakefield, positron, cavity 4740
 
  • A. Novokhatski, J. Seeman, M.K. Sullivan, U. Wienands
    SLAC, Menlo Park, California
 
 

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


We present the history and analysis of different wake field effects throughout the operational life of the PEP-II SLAC B-factory. Although the impedance of the high and low energy rings is small, the high current intense beams generated a lot of power. These wake field effects are: heating and damage of vacuum beam chamber elements like RF seals, vacuum valves , shielded bellows, BPM buttons and ceramic tiles; vacuum spikes, vacuum instabilities and high detector background; beam longitudinal and transverse instabilities. We also discuss the methods used to eliminate these effects. Results of this analysis and the PEP-II experience may be very useful in the design of new storage rings and light sources.

 
FR5REP053 Higher Order Modes in the SC Cavities of the SPL cavity, simulation, linac, emittance 4887
 
  • F. Gerigk, M. Schuh, J. Tuckmantel
    CERN, Geneva
  • C.P. Welsch
    KIP, Heidelberg
 
 

In this paper is analysed the influence of Higher Order Modes (HOM) on the operation of the superconducting linac section of the SPL, the Superconducting Proton Linac being designed at CERN. For this purpose, the characteristics of the HOMs in the 2 different beta families (0.65, 0.92 both at 704 MHz) of the SPL are calculated to estimate their effect on the cryogenic system and on the beam stability. For both criteria the maximum external Q of the HOMs is defined.