CURRENT INDUSTRIAL SRF CAPABILITIES AND FUTURE PLANS

Size: px
Start display at page:

Download "CURRENT INDUSTRIAL SRF CAPABILITIES AND FUTURE PLANS"

Transcription

1 CURRENT INDUSTRIAL SRF CAPABILITIES AND FUTURE PLANS Hanspeter Vogel ACCEL Instruments GmbH Friedrich Ebert Strasse 1, Bergisch Gladbach, Germany Corresponding author: Hanspeter Vogel ACCEL Instruments Friedrich Ebert Strasse Bergisch Gladbach, Germany Phone: FAX: vogel@accel.de ABSTRACT Industrial capabilities in view of SRF technology for accelerators cover design, engineering, manufacturing, preparation, test, assembly, and support for taking components and systems into operation. Capabilities will be presented by showing various examples of past and present activities. Future plans in Industry are driven by application of SRF technology in an increasing number of projects in different scale and scope, covering Synchrotrons, small linacs for FEL, up to the X-FEL linac or the ILC. Keywords: Industrial capabilities, SRF technology, Design, Engineering, Manufacturing, Industry.

2 1. INTRODUCTION Industrial capabilities in the field of superconducting radio frequency (SRF) technology for accelerators cover a wide range starting with design and engineering, covering manufacturing, preparation, and testing of SRF cavities and components and finally performing assembly of SRF accelerating modules and installation of complete accelerators at the customers site with taking the accelerator into operation and personnel training. A variety of components are required to build complete SRF modules and SRF accelerators, some of them are standard items, some of them are considered key-components like cavities or rf-couplers. Beside the more general aspects of design and engineering the focus within this review is laid on the key components mentioned above for manufacturing, preparation, testing, and assembly technology. Future planning in industry is depending on the development of projects and application of SRF technology. A review of today s industrial capabilities is given focused on tasks like supporting planning and research, prototype production, and studies in cases of large scale project like the international linear collider (ILC) or the X-FEL project at DESY. 1

3 2. DESIGN OF SRF MODULES AND ACCELERATORS Based on the increasing demand of SRF technology for accelerator projects from not only the institutions with a strong background in SRF R&D, but also from customers and projects with less SRF experience a few specialized companies have built up the capabilities for supporting SRF based projects with increasing design capabilities and resources. The design of complete accelerator modules includes not only the detailed rf design and layout of the cavity, but also the mechanical and the cryogenic layout of the auxiliary components involving other related disciplines like vacuum and cryogenic technology, mechanical aspects Figure 1: the 3 nd harmonic srf Landau module for BESSY and systems technology. As a typical example the completely turn-key delivered Landau- Module is described here, a SRF accelerator module based on a scaled version of the CESR II type cavity, that was delivered to BESSY [1]. The parameters of this accelerating module are summarized in table 1. The available space in the BESSY storage ring limited the overall length of the module to below 800 mm. Nevertheless the cryogenic standby losses of the module were designed to be below 10 Watt by counter flow heat exchangers at the beam tubes, a design that was confirmed later by the measurements. Concerning the cavity design for this particular application the 500 MHz CESR design was scaled to 1,5 GHz including auxiliary components like in-vacuum HOM loads, and a piezo driven tuning system. After cavity manufacturing, preparation with buffered chemical polishing (BCP) and high pressure water rinsing (HPR) a cryogenic rf test was performed at DESY to prove the required performance. 2

4 The cavity was subsequently assembled with all other module components and delivered to BESSY were the cryogenic test of the module was conducted. Frequency 1500 MHz, Mono mode Cavity r/q (V 2 acc/2p diss ) 45.4 Ω V acc 500 kv (5MV/m) I max 500 ma Tuning Range +/- 600 khz Op. temperature 4.5 K Unloaded Q 2.2*10 8 Stand by losses < 10 W Diss. rf power 12.5 W HOM absorber Ferrite loads at room temperature Total length 800 mm Table 1: Parameters of the 3 rd harmonic Landau-Module for BESSY Beside the application in electron linear accelerators and storage rings SRF technology is used in several operating and proposed linear accelerator for light and heavy ions such as ALPI at Legnaro National Laboratory, ATLAS at Argonne National Laboratory, ISSAC at TRIUMF, the Indus project., and the proposed LINAG at GANIL and RIA in US. Furthermore a 40 MeV proton and deuteron linear accelerator in under construction at SOREQ, Israel, based on a complete turn-key supply by ACCEL[2]. Within this project detailed studies were performed resulting in a accelerator design with Figure 2: SRF module with half wave resonators for a 40 MeV proton deuteron linear accelerator superconducting half wave resonators (HWR) for the linac at a particle energy as low as 1,5 MeV/u after particle generation with a standard ECR source and first acceleration and bunching with a radio frequency quadrupole (RFQ) operated in cw mode. Detailed beam dynamics simulation for the complete linac resulted in the layout of the various cavities to accommodate the increasing particle velocity, the two different particle species (protons and deuterons) and the arrangements of accelerating cavities and focusing elements. Figure 2 shows the design of the SRF module with 6 HWR and 3 superconducting solenoids for 3

5 focusing. Figure 3 shows the results of the beam dynamic simulations. Figure 3: beam dynamic simulation for the 40 MeV proton linace showing expected longitudinal emittance and envelope (upper graph) and the transversal emittance (lower graph). Both safely below the target values 3. ENGINEERING OF SRF MODULES AND COMPONENTS Detailed engineering for SRF modules and components is performed in industry either based on developments made in institutes or based on a close cooperation with institutes developing and applying SRF technology. For the electron cooler project at Brookhaven National Laboratory [3] a SRF module with a 700 MHz 5 cell cavity is developed by Advanced Energy Systems (AES) Figure 4: SRF module with a 700 MHz five cell cavity for the BNL Electron Cooler Project as shown in figure 4. 4

6 ACCEL is delivering and offering a SRF module based on the cavities of the TESLA collaboration and the module developed by Forschungzentrum Rossendorf (FZR)[4] under a license agreement. This module houses two TESLA type cavities and was developed for cw operation. After a detailed in house engineering review two such modules are under fabrication for the 4GLS project at Daresbury (GB)[5]. Figure 5 shows the module which will be delivered with guaranteed performance for accelerating field, cavity Q, rf power, and cryogenic parameters. The guaranteed performance in view of the accelerating gradient has been agreed for 25 MV per module. Performance results of TESLA cavities produced and completely prepared (BCP, HPR) at industry are presented in chapter 5. Figure 5: srf accelerating module based on the TESLA cavities, designed for cw operation (Forschungszentrum Rossendorf) 5

7 4. MANUFACTURING OF SRF CAVITES AND MODULES 4.1 CAVITY PROTOTYPING SRF technology is migrating from its original applications with spherical cavities for acceleration of electrons or high beta ions, HWR, QWR, or spoke-shaped cavities for the low velocity ions into new applications. University of Frankfurt has developed a CH mode cavity for ion acceleration with 18 spokes as shown in figure 6 and 7. Fig 6 shows the 3D layout of this cavity and the alternating arranged spokes in the cavity and fig 7 the central part of the cavity with these spokes before completion with the end caps[6]. Figure 7: view into the central part of the cavity before closing with end caps (cmp fig. 6) Figure 6: 3D layout of the CH Mode cavity developer by University of Frankfurt For the manufacturing planning of this cavity the manufacturing sequences for niobium forming, machining, welding, rf-measurements, and intermediate testing has been extensively analyzed. Additional developments for the tooling and fixtures were necessary for the actual production steps. A similar challenging project was the development of a 3 ½ cell cavity based on TESLA technology for a SRF photocathode Electron-Gun (Design FZ Rossendorf [7]) with improved focusing of the electron beam by a superposed TE Mode. The specific feature of this design required a complex mechanical design to allow independent tuning of the accelerating cells and the TE-mode cell. Fig. 8 shows the details of 6

8 this arrangement with the TESLA shaped cell and the special TE-mode cell and the braces for later attachment of a mechanical tuning system. 4.2 SERIES PRODUCTION OF SRF CAVITIES Figure 8 : srf photogun cavity developed by Forschungszentrum Rossendorf The recently completed series production of SRF cavities comprises a total of 109 cavities for the superconducting part of the linear accelerator for the Spallation Neutron Source (SNS) in Oak Ridge, US[8]. Fig. 9 shows a medium beta SNS cavity in comparison with a TESLA cavity. The production of these 109 cavities comprised the following steps Optimization of manufacturing technologies Manufacturing Figure 9: medium beta cavity for the SNS linac (above) compared with a TESLA cavity (below) RF Measurements (tuning, Qext) BCP (internal, external), Guaranteed performance 7

9 and can be characterized by the following schedule. After about a one year of ramp-up of the production (first article production, tooling develpment) 2 types of cavities (medium and high Beta) were delivered with a mean delivery rate of 4 Cavities / Month during the project running time between 08/2001 and 08/2004. Further examples of series production are the 360 cavities for the CEBAF project at Jefferson Laboratory, the series production of about 240 cavities for the LEP project at CERN, using the CERN developed niobium sputter technology, and the almost 80 TESLA cavities produced so far. 4.3 TURN-KEY ACCELERATING MODULES Turn-key accelerating modules have been and will be delivered from industry on a regular basis. These deliveries are based on the design provided by the applying research laboratory as in previous projects like the LEP storage ring at CERN in Geneva. In this case CERN included European industry in the technology transfer and series production for the accelerating modules which have been produced following the CERN developed sputter technology. Other SRF modules are developed and delivered based on industrial in house engineering capabilities and the vital cooperation with leading institutions in SRF technology. As an example the cooperation and technology transfer agreement with CORNELL University is described here which forms the basis for ACCEL production of 500 MHz accelerating modules for storage rings or synchrotron light sources [9]. These single cell 500 MHz modules are based on the CESR II design, that was re-engineered and meanwhile delivered to CORNELL (2 modules), the Taiwan Light Source (NSRRC, 2 modules), and the Canadian Light Source (CLS, 2 modules). The modules are operating since more than?? years now without problems. DIAMOND Light Source (DLS, 3 modules) has also decided to use SRF modules for the synchrotron and 3 modules will be delivered during 8

10 the year Fig 10 shows the accelerating module with the electronic racks housing low level rf control system and instrumentation. In addition the cryogenic valve box housing the control LHe input and gas return control valves for the supply of the cryogenic liquids. The valve operation is controlled directly by the sensors in the module and forms part of the integrated cryogenic control system. Figure 10: complete turn-key accelerating system for storage rings based on CESR 500 MHz technology. Center: SRF Module Left: cryogenic distribution valve box Right: Electronic controls for rf, instrumentation, and cryogenics 5. PREPARATION AND TESTING Turn-key accelerating systems can only be provided if the preparation and testing can be performed within the industrial responsibility. In the following chapter the recent results of cavities prepared at ACCEL for our accelerator modules are summarized. Closed loop chemical processing plants, high pressure high purity water rinsing facilities as well as the necessary clean rooms are used for the preparation of TESLA type, 500 MHz single cell cavities, and Half Wave Resonators. The results of the vertical cold rf test of the 500 MHz cavities are summarized in fig 11 and show the reliability of the achieved results. All nine cavities manufactured and tested so far show basically the same performance and allow for guaranteed accelerating voltage of about 2 MV to 2.3 MV with sufficient cavity quality factors Q 0 to allow sufficient operation in the storage rings or synchrotrons The procedures of assembling these cavities into accelerating 9

11 modules are so far safely established not to deteriorate the cavity performance compared to the vertical test results as is shown in the next paragraph 6. TESLA cavities are well developed and their performance, with the goal of gradients around 35 MV/m necessary for the Linear Collider application, show sufficient room for operation in linacs for ERL or FEL application. TESLA cavities which have been produced and chemically prepared at ACCEL are shown in fig 12 in comparison with TESLA cavities prepared at DESY. ACCEL prepared cavities using the in house infrastructure do almost reach the DESY prepared performance and these cavities fulfill safely the performance parameters of about 15 MV/m at quality factors around Summary 500 MHz Single Cell Cavity vertical cold Tests 1E+10 Cornell1 Cornell2 SRRC1 SRRC2 Figure 11: test results of ACCEL prepared 500 MHz Cavities (vertical test) Qo 1E+09 1E Vacc [MV] CLS1 CLS2 DLS1 DLS2 DLS3 1E+11 Q 0 1E+10 1E E acc [MV/m] AC55 AC56 AC57 AC59 AC60 AC61 AC62 AC63 AC64 BE1 BE2 Figure 12: Comparison of TESLA cavity test results (vertical tests): ACxx cavities are prepared and tested at DESY most of them including 1400 C heat treatment. BE01 and BE02 have been prepared at ACCEL. 800 C heating has been performed using the DESY furnace, not heat treatment at 1400 C has been performed on these two cavities 10

12 6. ASSEMBLY, DELIVERY, AND TAKING-INTO-OPERATION Module assembly includes the integration of cavities with all auxiliary components like helium vessel, tuners, power couplers, eventually HOM couplers, magnetic and cryogenic shielding, instrumentation, all integrated in the vacuum vessel. Procurement of standard components with sufficient Figure 13: Overview on the assembly of the 352 MHz LEP modules. Background: a complete module with 4 cavities before closing of the vacuum tank 3 cavities completed with the Helium vesse land tuner arr prepared and standing in front of the module quality, the preparation of cavities, integration of all components while preserving the cavity performance, intermediate testing and an overall quality control system form the basis for the successful performance of the accelerator module. In Fig. 14 a comparison 1E+10 between the vertical test results of a 500 MHz cavity with the performance Q0 1E+09 Cavity Test Modul Test after module integration is shown. Although the measurement error is larger for the module measurement due to the fact that the cavity Q can only be measured by the rf induced helium losses, a significant difference 13.3 MV/m reached during Modul Test with 2 ms long pulses 1E Eacc [MV/m] Figure 14: vertical test results (blue) in comparison with the cavity performance in the module (red) between vertical and module test can not be observed. Thus the assembly procedures can be regarded as qualified for this kind of application for the 500 MHz modules. 11

13 7. CURRENT INDUSTRIAL CAPABILITIES, CONCLUSION Industrial Capabilities in SRF technology are available at different levels. Companies focused on engineering with a view to application of SRF technology. Companies offering manufacturing resources (prototyping and series production). Companies offering design, engineering, and manufacturing. Companies offering the complete scope from design up to operational training. On the background of the recent (August 2004) announced decision for SRF technology for the International Linear Collider (ILC) the following comments can be summarized: The ILC decision for SRF has given a push also to industry and new interest in SRF technology is visible Companies with capabilities in SRF technology are located in all of the three regions: North America, Europe and Asia/Pacific. For ERL like projects the user will find sufficient support in industry from engineering capability, prototyping, up to delivery of turn key systems. 8. FUTURE PLANS Obviously industrial future plans are driven by the SRF application in future projects. Insofar the decision in favor of SRF technology for the ILC is promising for the industrial future supply of SRF technology. In addition a number of near term projects which are funded or near funding and have decided to use SRF technology can be identified. 12

14 Near term projects which are 4GLS, Peking University FEL, CORNELL-ERL, BNL- Electron Cooler, X-FEL at DESY, CEBAF-upgrade, SNS upgrade, and Synchrotron Light Sources such as SSRF (Shanghai). On the background of the above listed projects industrial support for the development of SRF applications can be summarized: Provide turn-key modules and Systems. Participate in and contribute to development issues (Cavities, Couplers, HOM dampers/absorbers ), provide prototypes, investigate reduction of manufacturing costs. Support project preparation/proposals with studies for large scale series production. Build up capacities and facilities for series production. We believe that industry is ready to support the increasing demand for SRF technology and is also ready to build up or extend further resources for future projects. However the investment in extension of resources must be financed by the budgets of the project or at least be secured by the projects. On the other hand it is obvious that from the project point of view the capabilities in industry should be ready as soon as the project start is visible. Consequently the timing for future investment is of great importance and should be mutually discussed between industry and institutions. ACKNOWLEDGEMENTS We thank our colleagues at ACCEL and at other industrial companies who have contributed to this article. The fruitful discussions with many partners in the institutes on the subject of industrialization and partnerships are appreciated. 13

15 REFERENCES [1] P. v. Stein, et al, A superconducting Landau Accelerator Module for BESSY II, proceedings of the 2001 Particle Accelerator Conference, Chicago. [2] Pekeler et al, A 40 MeV Linear Accelerator for Protons and Deuterons Using Superconducting Half Wave Resonators, proceedings rf the 2002 EPAC, Paris [3] Calaga et al, High Current Superconducting Cavities at RHIC. Proceedings of the 2004 EPAC, Luzern [4] Michael et al, Die Strahlungsquelle ELBE im Forschungszentrum Rossendorf, DACH Jahrestagung 2004, Salzburg [5] The 4 th Generation Light Source at Daresbury: [6] Podlech et al, Status of the Development of a Superconducting 352 MHz CH-Prototype Cavity, Proceedings of the 11 th SRF workshop, Lübeck, 2003 [7] Teichert et al, Status of the Rossendorf SRF-Gun Project, ww.mhf.desy.de/public/care04 [8] The Spallation Neutron Source. [9] Belomestnykh et al, Commissioning and Operations Results of the Industry-Produced CESR-Type SRF Cryomodules, proceedings of the 2005 PAC, Knoxville 14

Current Industrial SRF Capabilities and Future Plans

Current Industrial SRF Capabilities and Future Plans and Future Plans Capabilities in view of Design Engineering Manufacturing Preparation Testing Assembly Taking into operation Future Plans Participate in and contribute to development issues, provide prototypes

More information

SRF in Storage Rings. Michael Pekeler ACCEL Instruments GmbH Bergisch Gladbach Germany

SRF in Storage Rings. Michael Pekeler ACCEL Instruments GmbH Bergisch Gladbach Germany SRF in Storage Rings Michael Pekeler ACCEL Instruments GmbH 51429 Bergisch Gladbach Germany SRF in Storage Rings Michael Pekeler ACCEL Instruments GmbH 51429 Bergisch Gladbach Germany TESLA type cavity:

More information

Current Industrial SRF Capabilities and Future Plans

Current Industrial SRF Capabilities and Future Plans Current Industrial SRF Capabilities and Future Plans Review: Capabilities in view of Design Engineering Manufacturing Preparation Testing Assembly Taking into operation Comments on: Future Plans Participate

More information

ASSEMBLY PREPARATIONS FOR THE INTERNATIONAL ERL CRYOMODULE AT DARESBURY LABORATORY

ASSEMBLY PREPARATIONS FOR THE INTERNATIONAL ERL CRYOMODULE AT DARESBURY LABORATORY ASSEMBLY PREPARATIONS FOR THE INTERNATIONAL ERL CRYOMODULE AT DARESBURY LABORATORY P. A. McIntosh #, R. Bate, C. D. Beard, M. A. Cordwell, D. M. Dykes, S. M. Pattalwar and J. Strachan, STFC Daresbury Laboratory,

More information

RF STATUS OF SUPERCONDUCTING MODULE DEVELOPMENT SUITABLE FOR CW OPERATION: ELBE CRYOSTATS

RF STATUS OF SUPERCONDUCTING MODULE DEVELOPMENT SUITABLE FOR CW OPERATION: ELBE CRYOSTATS RF STATUS OF SUPERCONDUCTING MODULE DEVELOPMENT SUITABLE FOR CW OPERATION: ELBE CRYOSTATS J. Teichert, A. Büchner, H. Büttig, F. Gabriel, P. Michel, K. Möller, U. Lehnert, Ch. Schneider, J. Stephan, A.

More information

Packaging of Cryogenic Components

Packaging of Cryogenic Components Packaging of Cryogenic Components William J. Schneider Senior Mechanical Engineer Emeritus November 19-23 2007 1 Packaging of Cryogenic Components Day one Introduction and Overview 2 What is important?

More information

DEVELOPMENT OF A BETA 0.12, 88 MHZ, QUARTER WAVE RESONATOR AND ITS CRYOMODULE FOR THE SPIRAL2 PROJECT

DEVELOPMENT OF A BETA 0.12, 88 MHZ, QUARTER WAVE RESONATOR AND ITS CRYOMODULE FOR THE SPIRAL2 PROJECT DEVELOPMENT OF A BETA 0.12, 88 MHZ, QUARTER WAVE RESONATOR AND ITS CRYOMODULE FOR THE SPIRAL2 PROJECT G. Olry, J-L. Biarrotte, S. Blivet, S. Bousson, C. Commeaux, C. Joly, T. Junquera, J. Lesrel, E. Roy,

More information

SUPERCONDUCTING RF IN STORAGE-RING-BASED LIGHT SOURCES

SUPERCONDUCTING RF IN STORAGE-RING-BASED LIGHT SOURCES Presented at the 13th International Workshop on RF Superconductivity, Beijing, China, 2007 SRF 071120-03 SUPERCONDUCTING RF IN STORAGE-RING-BASED LIGHT SOURCES * S. Belomestnykh #, CLASSE, Cornell University,

More information

Structures for RIA and FNAL Proton Driver

Structures for RIA and FNAL Proton Driver Structures for RIA and FNAL Proton Driver Speaker: Mike Kelly 12 th International Workshop on RF Superconductivity July 11-15, 2005 Argonne National Laboratory A Laboratory Operated by The University of

More information

Project X Cavity RF and mechanical design. T. Khabiboulline, FNAL/TD/SRF

Project X Cavity RF and mechanical design. T. Khabiboulline, FNAL/TD/SRF Project X Cavity RF and mechanical design T. Khabiboulline, FNAL/TD/SRF TTC meeting on CW-SRF, 2013 Project X Cavity RF and mechanical design T 1 High ß Low ß 0.5 HWR SSR1 SSR2 0 1 10 100 1 10 3 1 10 4

More information

THE U. S. RIA PROJECT SRF LINAC*

THE U. S. RIA PROJECT SRF LINAC* THE U. S. RIA PROJECT SRF LINAC* K. W. Shepard, ANL, Argonne, IL 60540, USA Abstract The nuclear physics community in the U. S. has reaffirmed the rare isotope accelerator facility (RIA) as the number

More information

DESIGN STUDY OF A 176 MHZ SRF HALF WAVE RESONATOR FOR THE SPIRAL-2 PROJECT

DESIGN STUDY OF A 176 MHZ SRF HALF WAVE RESONATOR FOR THE SPIRAL-2 PROJECT DESIGN STUDY OF A 176 MHZ SRF HALF WAVE RESONATOR FOR THE SPIRAL-2 PROJECT J-L. Biarrotte*, S. Blivet, S. Bousson, T. Junquera, G. Olry, H. Saugnac CNRS / IN2P3 / IPN Orsay, France Abstract In November

More information

DEVELOPMENT OF ROOM TEMPERATURE AND SUPERCONDUCTING CH-STRUCTURES H. Podlech IAP, Universität Frankfurt/Main, Germany. Abstract

DEVELOPMENT OF ROOM TEMPERATURE AND SUPERCONDUCTING CH-STRUCTURES H. Podlech IAP, Universität Frankfurt/Main, Germany. Abstract EU contract number RII3-CT-2003-506395 CARE Conf-04-011-HIPPI DEVELOPMENT OF ROOM TEMPERATURE AND SUPERCONDUCTING CH-STRUCTURES H. Podlech IAP, Universität Frankfurt/Main, Germany Abstract Abstract In

More information

OVERVIEW OF INPUT POWER COUPLER DEVELOPMENTS, PULSED AND CW*

OVERVIEW OF INPUT POWER COUPLER DEVELOPMENTS, PULSED AND CW* Presented at the 13th International Workshop on RF Superconductivity, Beijing, China, 2007 SRF 071120-04 OVERVIEW OF INPUT POWER COUPLER DEVELOPMENTS, PULSED AND CW* S. Belomestnykh #, CLASSE, Cornell

More information

Amit Roy Director, IUAC

Amit Roy Director, IUAC SUPERCONDUCTING RF DEVELOPMENT AT INTER-UNIVERSITY ACCELERATOR CENTRE (IUAC) (JOINT PROPOSAL FROM IUAC & Delhi University (DU)) Amit Roy Director, IUAC to be presented by Kirti Ranjan (DU / Fermilab) Overview

More information

REVIEW ON SUPERCONDUCTING RF GUNS

REVIEW ON SUPERCONDUCTING RF GUNS REVIEW ON SUPERCONDUCTING RF GUNS D. Janssen #, A. Arnold, H. Büttig, U. Lehnert, P. Michel, P. Murcek, C. Schneider, R. Schurig, F. Staufenbiel, J. Teichert, R. Xiang, Forschungszentrum Rossendorf, Germany.

More information

5.5 SNS Superconducting Linac

5.5 SNS Superconducting Linac JP0150514 ICANS - XV 15 th Meeting of the International Collaboration on Advanced Neutron Sources November 6-9, 2000 Tsukuba, Japan Ronald M. Sundelin Jefferson Lab* 5.5 SNS Superconducting Linac 12000

More information

REVIEW OF HIGH POWER CW COUPLERS FOR SC CAVITIES. S. Belomestnykh

REVIEW OF HIGH POWER CW COUPLERS FOR SC CAVITIES. S. Belomestnykh REVIEW OF HIGH POWER CW COUPLERS FOR SC CAVITIES S. Belomestnykh HPC workshop JLAB, 30 October 2002 Introduction Many aspects of the high-power coupler design, fabrication, preparation, conditioning, integration

More information

Development of superconducting crossbar-h-mode cavities for proton and ion accelerators

Development of superconducting crossbar-h-mode cavities for proton and ion accelerators PHYSICAL REVIEW SPECIAL TOPICS - ACCELERATORS AND BEAMS 13, 041302 (2010) Development of superconducting crossbar-h-mode cavities for proton and ion accelerators F. Dziuba, 1 M. Busch, 1 M. Amberg, 1 H.

More information

To produce more powerful and high-efficiency particle accelerator, efforts have

To produce more powerful and high-efficiency particle accelerator, efforts have Measuring Unloaded Quality Factor of Superconducting RF Cryomodule Jian Cong Zeng Department of Physics and Astronomy, State University of New York at Geneseo, Geneseo, NY 14454 Elvin Harms, Jr. Accelerator

More information

Overview of ERL Projects: SRF Issues and Challenges. Matthias Liepe Cornell University

Overview of ERL Projects: SRF Issues and Challenges. Matthias Liepe Cornell University Overview of ERL Projects: SRF Issues and Challenges Matthias Liepe Cornell University Overview of ERL projects: SRF issues and challenges Slide 1 Outline Introduction: SRF for ERLs What makes it special

More information

DESIGN AND BEAM DYNAMICS STUDIES OF A MULTI-ION LINAC INJECTOR FOR THE JLEIC ION COMPLEX

DESIGN AND BEAM DYNAMICS STUDIES OF A MULTI-ION LINAC INJECTOR FOR THE JLEIC ION COMPLEX DESIGN AND BEAM DYNAMICS STUDIES OF A MULTI-ION LINAC INJECTOR FOR THE JLEIC ION COMPLEX Speaker: P.N. Ostroumov Contributors: A. Plastun, B. Mustapha and Z. Conway HB2016, July 7, 2016, Malmö, Sweden

More information

A few results [2,3] obtained with the individual cavities inside their horizontal cryostats are summarized in Table I and a typical Q o

A few results [2,3] obtained with the individual cavities inside their horizontal cryostats are summarized in Table I and a typical Q o Particle Accelerators, 1990, Vol. 29, pp. 47-52 Reprints available directly from the publisher Photocopying permitted by license only 1990 Gordon and Breach, Science Publishers, Inc. Printed in the United

More information

SRF Cavities A HIGHLY PRIZED TECHNOLOGY FOR ACCELERATORS. An Energetic Kick. Having a Worldwide Impact

SRF Cavities A HIGHLY PRIZED TECHNOLOGY FOR ACCELERATORS. An Energetic Kick. Having a Worldwide Impact Frank DiMeo SRF Cavities A HIGHLY PRIZED TECHNOLOGY FOR ACCELERATORS An Energetic Kick A key component of any modern particle accelerator is the electromagnetic cavity resonator. Inside the hollow resonator

More information

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

ERL Prototype at BNL. Work supported by Brookhaven Science Associates, LLC under Contract No. DE-AC02-98CH10886 with the U.S. Department of Energy. ERL Prototype at BNL Ilan Ben-Zvi, for the Superconducting Accelerator and Electron Cooling group, Collider-Accelerator Department Brookhaven National Laboratory & Center for Accelerator Science and Education

More information

The European Spallation Source. Dave McGinnis Chief Engineer ESS\Accelerator Division IVEC 2013

The European Spallation Source. Dave McGinnis Chief Engineer ESS\Accelerator Division IVEC 2013 The European Spallation Source Dave McGinnis Chief Engineer ESS\Accelerator Division IVEC 2013 Overview The European Spallation Source (ESS) will house the most powerful proton linac ever built. The average

More information

Development of Superconducting CH-Cavities for the EUROTRANS and IFMIF Project 1

Development of Superconducting CH-Cavities for the EUROTRANS and IFMIF Project 1 1 AT/P5-01-POSTER Development of Superconducting CH-Cavities for the EUROTRANS and IFMIF Project 1 F. Dziuba 2, H. Podlech 2, M. Buh 2, U. Ratzinger 2, A. Bechtold 3, H. Klein 2 2 Institute for Applied

More information

Commissioning of the ALICE SRF Systems at Daresbury Laboratory Alan Wheelhouse, ASTeC, STFC Daresbury Laboratory ESLS RF 1 st 2 nd October 2008

Commissioning of the ALICE SRF Systems at Daresbury Laboratory Alan Wheelhouse, ASTeC, STFC Daresbury Laboratory ESLS RF 1 st 2 nd October 2008 Commissioning of the ALICE SRF Systems at Daresbury Laboratory Alan Wheelhouse, ASTeC, STFC Daresbury Laboratory ESLS RF 1 st 2 nd October 2008 Overview ALICE (Accelerators and Lasers In Combined Experiments)

More information

INSTRUMENTATION AND CONTROL SYSTEM FOR THE INTERNATIONAL ERL CRYOMODULE

INSTRUMENTATION AND CONTROL SYSTEM FOR THE INTERNATIONAL ERL CRYOMODULE INSTRUMENTATION AND CONTROL SYSTEM FOR THE INTERNATIONAL ERL CRYOMODULE S. M. Pattalwar, R. Bate, G. Cox, P.A. McIntosh and A. Oates, STFC, Daresbury Laboratory, Warrington, UK Abstract ALICE is a prototype

More information

Cryogenics, Cryomodule & Superconductivity for Accelerator Programme in Asia

Cryogenics, Cryomodule & Superconductivity for Accelerator Programme in Asia Cryogenics, Cryomodule & Superconductivity for Accelerator Programme in Asia T S Datta Inter- University Accelerator Centre New Delhi. India (On behalf of Core Committee) ACFA 22, Dongguan ( T S Datta)

More information

Superconducting RF System. Heung-Sik Kang

Superconducting RF System. Heung-Sik Kang Design of PLS-II Superconducting RF System Heung-Sik Kang On behalf of PLS-II RF group Pohang Accelerator Laboratory Content 1. Introduction 2. Physics design 3. Cryomodules 4. Cryogenic system 5. High

More information

Triple-spoke compared with Elliptical-cell Cavities

Triple-spoke compared with Elliptical-cell Cavities Triple-spoke compared with Elliptical-cell Cavities Ken Shepard - ANL Physics Division 2th International Workshop on RF Superconductivity Argonne National Laboratory Operated by The University of Chicago

More information

CEBAF Overview June 4, 2010

CEBAF Overview June 4, 2010 CEBAF Overview June 4, 2010 Yan Wang Deputy Group Leader of the Operations Group Outline CEBAF Timeline Machine Overview Injector Linear Accelerators Recirculation Arcs Extraction Systems Beam Specifications

More information

The Superconducting Radio Frequency Quadrupole Structures Review

The Superconducting Radio Frequency Quadrupole Structures Review The Superconducting Radio Frequency Quadrupole Structures Review Augusto Lombardi INFN- Laboratori Nazionali di Legnaro, via Romea 4 I-35020 Legnaro (PD) Abstract Since 1985 the idea of using the fast

More information

SUPERCONDUCTING PROTOTYPE CAVITIES FOR THE SPALLATION NEUTRON SOURCE (SNS) PROJECT *

SUPERCONDUCTING PROTOTYPE CAVITIES FOR THE SPALLATION NEUTRON SOURCE (SNS) PROJECT * SUPERCONDUCTING PROTOTYPE CAVITIES FOR THE SPALLATION NEUTRON SOURCE (SNS) PROJECT * G. Ciovati, P. Kneisel, J. Brawley, R. Bundy, I. Campisi, K. Davis, K. Macha, D. Machie, J. Mammosser, S. Morgan, R.

More information

Engineering Challenges and Solutions for MeRHIC. Andrew Burrill for the MeRHIC Team

Engineering Challenges and Solutions for MeRHIC. Andrew Burrill for the MeRHIC Team Engineering Challenges and Solutions for MeRHIC Andrew Burrill for the MeRHIC Team Key Components Photoinjector Design Photocathodes & Drive Laser Linac Cavities 703.75 MHz 5 cell cavities 3 rd Harmonic

More information

Aurélien Ponton. First Considerations for the Design of the ESS Cryo-Modules

Aurélien Ponton. First Considerations for the Design of the ESS Cryo-Modules Accelerator Division ESS AD Technical Note ESS/AD/0001 Aurélien Ponton First Considerations for the Design of the ESS Cryo-Modules 16 March 2010 First considerations for the design of the ESS cryo-modules

More information

Status of superconducting module development suitable for cw operation: ELBE cryostats

Status of superconducting module development suitable for cw operation: ELBE cryostats Status of superconducting module development suitable for cw operation: ELBE cryostats, A. Büchner, H. Büttig, F. Gabriel, P. Michel, K. Möller, U. Lehnert, Ch. Schneider, J. Stephan, A. Winter Forschungszentrum

More information

SNS CRYOMODULE PERFORMANCE*

SNS CRYOMODULE PERFORMANCE* SNS CRYOMODULE PERFORMANCE* J. Preble*, I. E. Campisi, E. Daly, G. K. Davis, J. R. Delayen, M. Drury, C. Grenoble, J. Hogan, L. King, P. Kneisel, J. Mammosser, T. Powers, M. Stirbet, H. Wang, T. Whitlatch,

More information

QUARTER WAVE COAXIAL LINE CAVITY FOR NEW DELHI LINAC BOOSTER*

QUARTER WAVE COAXIAL LINE CAVITY FOR NEW DELHI LINAC BOOSTER* QUARTER WAVE COAXIAL LINE CAVITY FOR NEW DELHI LINAC BOOSTER* P.N. Prakash and A.Roy Nuclear Science Centre, P.O.Box 10502, New Delhi 110 067, INDIA and K.W.Shepard Physics Division, Argonne National Laboratory,

More information

Progresses on China ADS Superconducting Cavities

Progresses on China ADS Superconducting Cavities Progresses on China ADS Superconducting Cavities Peng Sha IHEP, CAS 2013/06/12 1 Outline 1. Introduction 2. Spoke012 cavity 3. Spoke021 cavity 4. Spoke040 cavity 5. 650MHz β=0.82 5-cell cavity 6. High

More information

ADVANCES IN CW ION LINACS*

ADVANCES IN CW ION LINACS* Abstract Substantial research and development related to continuous wave (CW) proton and ion accelerators is being performed at ANL. A 4-meter long 60.625-MHz normal conducting (NC) CW radio frequency

More information

Low and Medium-β Superconducting Cavities. A. Facco INFN-LNL

Low and Medium-β Superconducting Cavities. A. Facco INFN-LNL Low and Medium-β Superconducting Cavities A. Facco INFN-LNL Definition low-, medium- and high-β: Just cavities with β

More information

ALICE SRF SYSTEM COMMISSIONING EXPERIENCE A. Wheelhouse ASTeC, STFC Daresbury Laboratory

ALICE SRF SYSTEM COMMISSIONING EXPERIENCE A. Wheelhouse ASTeC, STFC Daresbury Laboratory ALICE SRF SYSTEM COMMISSIONING EXPERIENCE A. Wheelhouse ASTeC, STFC Daresbury Laboratory ERL 09 8 th 12 th June 2009 ALICE Accelerators and Lasers In Combined Experiments Brief Description ALICE Superconducting

More information

OPERATING EXPERIENCE WITH = 1 HIGH CURRENT ACCELERATORS*

OPERATING EXPERIENCE WITH = 1 HIGH CURRENT ACCELERATORS* Presented at the 11 th Workshop on RF Superconductivity SRF 2003, Lubeck/Travemunde, Germany SRF 031215-19 OPERATING EXPERIENCE WITH = 1 HIGH CURRENT ACCELERATORS* S. Belomestnykh # Laboratory for Elementary-Particle

More information

THE CRYOGENIC SYSTEM OF TESLA

THE CRYOGENIC SYSTEM OF TESLA THE CRYOGENIC SYSTEM OF TESLA S. Wolff, DESY, Notkestr. 85, 22607 Hamburg, Germany for the TESLA collaboration Abstract TESLA, a 33 km long 500 GeV centre-of-mass energy superconducting linear collider

More information

SUPERCONDUCTING CAVITIES AND CRYOMODULES FOR PROTON AND DEUTERON LINACS

SUPERCONDUCTING CAVITIES AND CRYOMODULES FOR PROTON AND DEUTERON LINACS Proceedings of LINAC2014, Geneva, Switzerland THIOA04 SUPERCONDUCTING CAVITIES AND CRYOMODULES FOR PROTON AND DEUTERON LINACS G. Devanz, CEA-Irfu CEA-Saclay, Gif-sur-Yvette 91191, France Abstract We review

More information

Cryogenics for Large Accelerators

Cryogenics for Large Accelerators Cryogenics for Large Accelerators Dr. Sergiy Putselyk Deutsches Elektronen-Synchrotron (DESY) MKS Division Notkestrasse 85 22607 Hamburg (Germany) Phone: +49 40 89983492 Fax: +49 40 89982858 E-Mail: Sergiy.Putselyk@desy.de

More information

The low level radio frequency control system for DC-SRF. photo-injector at Peking University *

The low level radio frequency control system for DC-SRF. photo-injector at Peking University * The low level radio frequency control system for DC-SRF photo-injector at Peking University * WANG Fang( 王芳 ) 1) FENG Li-Wen( 冯立文 ) LIN Lin( 林林 ) HAO Jian-Kui( 郝建奎 ) Quan Sheng-Wen( 全胜文 ) ZHANG Bao-Cheng(

More information

Status of the ESS Accelerator Workpackage

Status of the ESS Accelerator Workpackage Status of the ESS Accelerator Workpackage Peter McIntosh STFC Daresbury Laboratory UK ESS Interactions and Opportunities Rutherford Appleton Laboratory 3 Dec 2014 The ESS Linac The European Spallation

More information

Motivation: ERL based e linac for LHeC

Motivation: ERL based e linac for LHeC Erk Jensen, for the LHeC team and the RF group ERL 2013, BINP, Novosibirsk, 09 Sep 2013 09 Sep 2013 1 Motivation: ERL based e linac for LHeC ( O. Brünings presentation) NB.: This is a 09 Sep 2013 2 Some

More information

Nb 3 Sn Present Status and Potential as an Alternative SRF Material. S. Posen and M. Liepe, Cornell University

Nb 3 Sn Present Status and Potential as an Alternative SRF Material. S. Posen and M. Liepe, Cornell University Nb 3 Sn Present Status and Potential as an Alternative SRF Material S. Posen and M. Liepe, Cornell University LINAC 2014 Geneva, Switzerland September 2, 2014 Limits of Modern SRF Technology Low DF, high

More information

Status of Projects using TESLA Cavities. Mike Dykes, ASTeC, Head of RF.

Status of Projects using TESLA Cavities. Mike Dykes, ASTeC, Head of RF. Status of Projects using TESLA Cavities Mike Dykes, ASTeC, Head of RF. Daresbury ERLP OUTLINE Status of other Projects 4GLS Daresbury ERLP Injector Linac Cryogenics Summary Projects Cornell ERL BESSY University

More information

OVERVIEW OF REGIONAL INFRASTRUCTURES FOR SCRF DEVELOPMENT

OVERVIEW OF REGIONAL INFRASTRUCTURES FOR SCRF DEVELOPMENT OVERVIEW OF REGIONAL INFRASTRUCTURES FOR SCRF DEVELOPMENT Carlo Pagani, University of Milano and INFN Milano - LASA, Italy Abstract The perspective of building the International Linear Collider, ILC, as

More information

CHALLENGES IN ILC SCRF TECHNOLOGY *

CHALLENGES IN ILC SCRF TECHNOLOGY * CHALLENGES IN ILC SCRF TECHNOLOGY * Detlef Reschke #, DESY, D-22603 Hamburg, Germany Abstract With a baseline operating gradient of 31,5 MV/m at a Q-value of 10 10 the superconducting nine-cell cavities

More information

CEBAF waveguide absorbers. R. Rimmer for JLab SRF Institute

CEBAF waveguide absorbers. R. Rimmer for JLab SRF Institute CEBAF waveguide absorbers R. Rimmer for JLab SRF Institute Outline Original CEBAF HOM absorbers Modified CEBAF loads for FEL New materials for replacement loads High power loads for next generation FELs

More information

S. Ghosh On behalf of Linac, IFR, Cryogenics, RF and beam transport group members. Inter University Accelerator Centre New Delhi India

S. Ghosh On behalf of Linac, IFR, Cryogenics, RF and beam transport group members. Inter University Accelerator Centre New Delhi India S. Ghosh On behalf of Linac, IFR, Cryogenics, RF and beam transport group members Inter University Accelerator Centre New Delhi 110067 India Highlights of presentation 1. Introduction to Linear accelerator

More information

Advances in CW Ion Linacs

Advances in CW Ion Linacs IPAC 2015 P.N. Ostroumov May 8, 2015 Content Two types of CW ion linacs Example of a normal conducting CW RFQ Cryomodule design and performance High performance quarter wave and half wave SC resonators

More information

Superconducting RF for Energy-Recovery Linacs

Superconducting RF for Energy-Recovery Linacs Superconducting RF for Energy-Recovery Linacs M. Liepe LEPP, Cornell University, Ithaca, NY 14853, USA J. Knobloch BESSY GmbH, D-12489 Berlin, Germany Abstract Since superconducting RF for particle accelerators

More information

LOW BETA CAVITY DEVELOPMENT FOR AN ATLAS INTENSITY UPGRADE

LOW BETA CAVITY DEVELOPMENT FOR AN ATLAS INTENSITY UPGRADE LOW BETA CAVITY DEVELOPMENT FOR AN ATLAS INTENSITY UPGRADE M. P. Kelly, Z. A. Conway, S. M. Gerbick, M. Kedzie, T. C. Reid, R. C. Murphy, B. Mustapha, S.H. Kim, P. N. Ostroumov, Argonne National Laboratory,

More information

SRF EXPERIENCE WITH THE CORNELL HIGH-CURRENT ERL INJECTOR PROTOTYPE

SRF EXPERIENCE WITH THE CORNELL HIGH-CURRENT ERL INJECTOR PROTOTYPE SRF EXPERIENCE WITH THE CORNELL HIGH-CURRENT ERL INJECTOR PROTOTYPE M. Liepe, S. Belomestnykh, E. Chojnacki, Z. Conway, V. Medjidzade, H. Padamsee, P. Quigley, J. Sears, V. Shemelin, V. Veshcherevich,

More information

HIGH POWER COUPLER FOR THE TESLA TEST FACILITY

HIGH POWER COUPLER FOR THE TESLA TEST FACILITY Abstract HIGH POWER COUPLER FOR THE TESLA TEST FACILITY W.-D. Moeller * for the TESLA Collaboration, Deutsches Elektronen-Synchrotron DESY, D-22603 Hamburg, Germany The TeV Energy Superconducting Linear

More information

ERLP Status. Mike Dykes

ERLP Status. Mike Dykes ERLP Status Mike Dykes Content ASTeC RF & Diagnostics Group Work of the Group 4GLS ERLP Photo-injector Accelerating Modules Summary High Power RF Engineering Andy Moss SRS Support; DIAMOND; ERLP; MICE;

More information

CAGE CAVITY: A LOW COST, HIGH PERFORMANCE SRF ACCELERATING STRUCTURE*

CAGE CAVITY: A LOW COST, HIGH PERFORMANCE SRF ACCELERATING STRUCTURE* CAGE CAVITY: A LOW COST, HIGH PERFORMANCE SRF ACCELERATING STRUCTURE* J. Noonan, T.L. Smith, M. Virgo, G.J. Waldsmidt, Argonne National Laboratory J.W. Lewellen, Los Alamos National Laboratory Abstract

More information

Frequency Tuning and RF Systems for the ATLAS Energy Upgrade. Gary P. Zinkann

Frequency Tuning and RF Systems for the ATLAS Energy Upgrade. Gary P. Zinkann Frequency Tuning and RF Systems for the ATLAS Energy Upgrade Outline Overview of the ATLAS Energy Upgrade Description of cavity Tuning method used during cavity construction Description and test results

More information

XFEL Cryo System. Project X Collaboration Meeting, FNAL September 8-9, 2010 Bernd Petersen DESY MKS (XFEL WP10 & WP13) 1 st stage. Possible extension

XFEL Cryo System. Project X Collaboration Meeting, FNAL September 8-9, 2010 Bernd Petersen DESY MKS (XFEL WP10 & WP13) 1 st stage. Possible extension XFEL Cryo System Possible extension 1 st stage Project X Collaboration Meeting, FNAL September 8-9, 2010 (XFEL WP10 & WP13) Outline 2 XFEL accelerator structure TESLA technology Basic cryogenic parameters

More information

Latest Developments in Superconducting RF Structures for beta=1 Particle Acceleration

Latest Developments in Superconducting RF Structures for beta=1 Particle Acceleration Latest Developments in Superconducting RF Structures for beta=1 Particle Acceleration Peter Kneisel Jefferson Lab Newport News, Virginia, USA June 28, 2006 EPAC 2006, Edinburgh 1 Outline Challenges of

More information

Cavity development for TESLA

Cavity development for TESLA Cavity development for TESLA Lutz.Lilje@desy.de DESY -FDET- Cavity basics History: Limitations and solutions»material inclusions»weld defects»field emission»increased surface resistance at high field Performance

More information

KEK ERL CRYOMODULE DEVELOPMENT

KEK ERL CRYOMODULE DEVELOPMENT KEK ERL CRYOMODULE DEVELOPMENT H. Sakai*, T. Furuya, E. Kako, S. Noguchi, M. Sato, S. Sakanaka, T. Shishido, T. Takahashi, K. Umemori, K. Watanabe and Y. Yamamoto KEK, 1-1, Oho, Tsukuba, Ibaraki, 305-0801,

More information

Third Harmonic Superconducting passive cavities in ELETTRA and SLS

Third Harmonic Superconducting passive cavities in ELETTRA and SLS RF superconductivity application to synchrotron radiation light sources Third Harmonic Superconducting passive cavities in ELETTRA and SLS 2 cryomodules (one per machine) with 2 Nb/Cu cavities at 1.5 GHz

More information

Crab Cavities for FCC

Crab Cavities for FCC Crab Cavities for FCC R. Calaga, A. Grudiev, CERN FCC Week 2017, May 30, 2017 Acknowledgements: O. Bruning, E. Cruz-Alaniz, K. Ohmi, R. Martin, R. Tomas, F. Zimmermann Livingston Plot 100 TeV FCC-hh: 0.5-3x1035

More information

THE HIGH LUMINOSITY PERFORMANCE OF CESR WITH THE NEW GENERATION SUPERCONDUCTING CAVITY

THE HIGH LUMINOSITY PERFORMANCE OF CESR WITH THE NEW GENERATION SUPERCONDUCTING CAVITY Presented at the 1999 Particle Accelerator Conference, New York City, NY, USA, March 29 April 2 CLNS 99/1614 / SRF 990407-03 THE HIGH LUMINOSITY PERFORMANCE OF CESR WITH THE NEW GENERATION SUPERCONDUCTING

More information

Review of New Shapes for Higher Gradients

Review of New Shapes for Higher Gradients Review of New Shapes for Higher Gradients Rong-Li Geng LEPP, Cornell University Rong-Li Geng SRF2005, July 10-15, 2005 1 1 TeV 800GeV 500GeV ILC(TESLA type) energy reach Rapid advances in single-cell cavities

More information

SARAF commissioning & safety issues. L. Weissman on behalf of the SARAF team SPIRAL week 2010

SARAF commissioning & safety issues. L. Weissman on behalf of the SARAF team SPIRAL week 2010 SARAF commissioning & safety issues L. Weissman on behalf of the SARAF team SPIRAL week 2010 1 Outline commissioning of SARAF project : RFQ status Cryomodule status Accumulated beam operation experience

More information

Cornell ERL s Main Linac Cavities

Cornell ERL s Main Linac Cavities Cornell ERL s Main Linac Cavities N. Valles for Cornell ERL Team 1 Overview RF Design Work Cavity Design Considerations Optimization Methods Results Other Design Considerations Coupler Kicks Stiffening

More information

HIGH POWER PULSED TESTS OF A BETA=0.5 5-CELL 704 MHZ SUPERCONDUCTING CAVITY

HIGH POWER PULSED TESTS OF A BETA=0.5 5-CELL 704 MHZ SUPERCONDUCTING CAVITY HIGH POWER PULSED TESTS OF A BETA=0.5 5-CELL 704 MHZ SUPERCONDUCTING CAVITY G. Devanz, D. Braud, M. Desmons, Y. Gasser, E. Jacques, O. Piquet, J. Plouin, J.- P. Poupeau, D. Roudier, P. Sahuquet, CEA-Saclay,

More information

Recent Progress in the Superconducting RF Program at TRIUMF/ISAC

Recent Progress in the Superconducting RF Program at TRIUMF/ISAC Recent Progress in the Superconducting RF Program at TRIUMF/ISAC Abstract R.E. Laxdal, K. Fong, M. Laverty, A. Mitra, R. Poirier, I. Sekachev, V. Zvyagintsev, TRIUMF, Vancouver, BC, V6T2A3, Canada A heavy

More information

Performance of Superconducting Cavities for the European XFEL. Detlef Reschke DESY for the EU-XFEL Accelerator Consortium

Performance of Superconducting Cavities for the European XFEL. Detlef Reschke DESY for the EU-XFEL Accelerator Consortium Performance of Superconducting Cavities for the European XFEL Detlef Reschke DESY for the EU-XFEL Accelerator Consortium Outline 2 European XFEL Linear Accelerator Cavity Production Vertical Acceptance

More information

TESLA TeV Collider Project Overview

TESLA TeV Collider Project Overview Hamburg-Zeuthen Linear Collider Meeting TESLA TeV Collider Project Overview Carlo Pagani Milano & DESY carlo.pagani@desy.de The TESLA Challenge Physical limit is 50 MV/m > 25 MV/m could be obtained Common

More information

A 3 GHz SRF reduced-β Cavity for the S-DALINAC

A 3 GHz SRF reduced-β Cavity for the S-DALINAC A 3 GHz SRF reduced-β Cavity for the S-DALINAC D. Bazyl*, W.F.O. Müller, H. De Gersem Gefördert durch die DFG im Rahmen des GRK 2128 20.11.2018 M.Sc. Dmitry Bazyl TU Darmstadt TEMF Upgrade of the Capture

More information

The TESLA Linear Collider. Winfried Decking (DESY) for the TESLA Collaboration

The TESLA Linear Collider. Winfried Decking (DESY) for the TESLA Collaboration The TESLA Linear Collider Winfried Decking (DESY) for the TESLA Collaboration Outline Project Overview Highlights 2000/2001 Publication of the TDR Cavity R&D TTF Operation A0 and PITZ TESLA Beam Dynamics

More information

PROGRESS IN IFMIF HALF WAVE RESONATORS MANUFACTURING AND TEST PREPARATION

PROGRESS IN IFMIF HALF WAVE RESONATORS MANUFACTURING AND TEST PREPARATION PROGRESS IN IFMIF HALF WAVE RESONATORS MANUFACTURING AND TEST PREPARATION G. Devanz, N. Bazin, G. Disset, H. Dzitko, P. Hardy, H. Jenhani, J. Neyret, O. Piquet, J. Plouin, N. Selami, CEA-Saclay, France

More information

Superconducting 1.3 GHz Cavities for European XFEL

Superconducting 1.3 GHz Cavities for European XFEL Superconducting 1.3 GHz Cavities for European XFEL W. Singer, J. Iversen, A. Matheisen, X. Singer (DESY, Germany) P. Michelato (INFN, Italy) Presented by Waldemar Singer Main issues: preparation phase

More information

Superconducting Cavity Fabrication for ILC in Japan

Superconducting Cavity Fabrication for ILC in Japan Superconducting Cavity Fabrication for ILC in Japan -Industrial Activities- Masanori MATSUOKA (Mitsubishi Heavy Industries, Ltd.) Norihiko OZAKI (Linear Collider Forum of of Japan) Tuesday, Augsut 16,

More information

3.9 GHz work at Fermilab

3.9 GHz work at Fermilab 3.9 GHz work at Fermilab + CKM 13-cell cavity Engineering and designing W.-D. Moeller Desy, MHF-sl Protocol of the meeting about 3 rd harmonic cavities during the TESLA collaboration meeting at DESY on

More information

HIGH POWER INPUT COUPLERS FOR THE STF BASELINE CAVITY SYSTEM AT KEK

HIGH POWER INPUT COUPLERS FOR THE STF BASELINE CAVITY SYSTEM AT KEK HIGH POWER INPUT COUPLERS FOR THE STF BASELINE CAVITY SYSTEM AT KEK E. Kako #, H. Hayano, S. Noguchi, T. Shishido, K. Watanabe and Y. Yamamoto KEK, Tsukuba, Ibaraki, 305-0801, Japan Abstract An input coupler,

More information

TESLA Progress on R1 & R2 issues

TESLA Progress on R1 & R2 issues TESLA Progress on R1 & R2 issues Carlo Pagani Milano & DESY carlo.pagani@desy.de The TESLA Challenge for LC Physical limit at 50 MV/m > 25 MV/m could be obtained Common R&D effort for TESLA Higher conversion

More information

200 MHz 350 MHz 750 MHz Linac2 RFQ2 202 MHz 0.5 MeV /m Weight : 1000 kg/m Ext. diameter : 45 cm

200 MHz 350 MHz 750 MHz Linac2 RFQ2 202 MHz 0.5 MeV /m Weight : 1000 kg/m Ext. diameter : 45 cm M. Vretenar, CERN for the HF-RFQ Working Group (V.A. Dimov, M. Garlasché, A. Grudiev, B. Koubek, A.M. Lombardi, S. Mathot, D. Mazur, E. Montesinos, M. Timmins, M. Vretenar) 1 1988-92 Linac2 RFQ2 202 MHz

More information

Herwig Schopper CERN 1211 Geneva 23, Switzerland. Introduction

Herwig Schopper CERN 1211 Geneva 23, Switzerland. Introduction THE LEP PROJECT - STATUS REPORT Herwig Schopper CERN 1211 Geneva 23, Switzerland Introduction LEP is an e + e - collider ring designed and optimized for 2 100 GeV. In an initial phase an energy of 2 55

More information

Dong-O Jeon Representing RAON Institute for Basic Science

Dong-O Jeon Representing RAON Institute for Basic Science SRF in Heavy Ion Projects Dong-O Jeon Representing RAON Institute for Basic Science Acknowledgement Thanks go to Y. Chi (IEHP) and P. Ostroumov for providing slides about C-ADS and ATLAS Upgrade. 2 Design

More information

RECORD QUALITY FACTOR PERFORMANCE OF THE PROTOTYPE CORNELL ERL MAIN LINAC CAVITY IN THE HORIZONTAL TEST CRYOMODULE

RECORD QUALITY FACTOR PERFORMANCE OF THE PROTOTYPE CORNELL ERL MAIN LINAC CAVITY IN THE HORIZONTAL TEST CRYOMODULE RECORD QUALITY FACTOR PERFORMANCE OF THE PROTOTYPE CORNELL ERL MAIN LINAC CAVITY IN THE HORIZONTAL TEST CRYOMODULE N. Valles, R. Eichhorn, F. Furuta, M. Ge, D. Gonnella, D.N. Hall, Y. He, V. Ho, G. Hoffstaetter,

More information

High average power fundamental input couplers for the Cornell University ERL: requirements, design challenges and first ideas

High average power fundamental input couplers for the Cornell University ERL: requirements, design challenges and first ideas High average power fundamental input couplers for the Cornell University ERL: requirements, design challenges and first ideas S. Belomestnykh, M. Liepe, H. Padamsee, V. Shemelin, and V. Veshcherevich Laboratory

More information

2 nd and Final Announcement

2 nd and Final Announcement 2 nd and Final Announcement Workshop Information The International Workshop on Superconducting Radio Frequency (SRF) devices was founded in 1983 as a platform of communication for the application of superconductivity

More information

HIGHER ORDER MODES FOR BEAM DIAGNOSTICS IN THIRD HARMONIC 3.9 GHZ ACCELERATING MODULES *

HIGHER ORDER MODES FOR BEAM DIAGNOSTICS IN THIRD HARMONIC 3.9 GHZ ACCELERATING MODULES * HIGHER ORDER MODES FOR BEAM DIAGNOSTICS IN THIRD HARMONIC 3.9 GHZ ACCELERATING MODULES * N. Baboi #, N. Eddy, T. Flisgen, H.-W. Glock, R. M. Jones, I. R. R. Shinton, and P. Zhang # # Deutsches Elektronen-Synchrotron

More information

Proceedings of the Fourth Workshop on RF Superconductivity, KEK, Tsukuba, Japan

Proceedings of the Fourth Workshop on RF Superconductivity, KEK, Tsukuba, Japan ACTVTES ON RF SUPERCONDUCTVTY N FRASCAT, GENOVA, MLAN0 LABORATORES R. Boni, A. Cattoni, A. Gallo, U. Gambardella, D. Di Gioacchino, G. Modestino, C. Pagani*, R. Parodi**, L. Serafini*, B. Spataro, F. Tazzioli,

More information

ReA3 Marc Doleans (On behalf of the ReA3 team)

ReA3 Marc Doleans (On behalf of the ReA3 team) ReA3 Marc Doleans (On behalf of the ReA3 team) HIAT09, 08/06/2009, Slide 1 Building addition Office building (~100 staff + conf. rooms) ReA3 Experimental area 9100 sqft HIAT09, 08/06/2009, Slide 2 Why

More information

SUPERCONDUCTING RESONATORS DEVELOPMENT FOR THE FRIB AND ReA LINACS AT MSU: RECENT ACHIEVEMENTS AND FUTURE GOALS

SUPERCONDUCTING RESONATORS DEVELOPMENT FOR THE FRIB AND ReA LINACS AT MSU: RECENT ACHIEVEMENTS AND FUTURE GOALS SUPERCONDUCTING RESONATORS DEVELOPMENT FOR THE FRIB AND ReA LINACS AT MSU: RECENT ACHIEVEMENTS AND FUTURE GOALS A. Facco #+, E. Bernard, J. Binkowski, J. Crisp, C. Compton, L. Dubbs, K. Elliott, L. Harle,

More information

Energy Recovering Linac Issues

Energy Recovering Linac Issues Energy Recovering Linac Issues L. Merminga Jefferson Lab EIC Accelerator Workshop Brookhaven National Laboratory February 26-27, 2002 Outline Energy Recovery RF Stability in Recirculating, Energy Recovering

More information

Behavior of the TTF2 RF Gun with long pulses and high repetition rates

Behavior of the TTF2 RF Gun with long pulses and high repetition rates Behavior of the TTF2 RF Gun with long pulses and high repetition rates J. Baehr 1, I. Bohnet 1, J.-P. Carneiro 2, K. Floettmann 2, J. H. Han 1, M. v. Hartrott 3, M. Krasilnikov 1, O. Krebs 2, D. Lipka

More information