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diagnostics

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MOOA01 Instrumentation Requirements for Different Accelerator Types emittance, synchrotron, proton, controls 1
 
  • B.J. Holzer
    CERN, Geneva
 
 

At present more than 15000 particle accelerators exist worldwide, being built and optimised to handle a large variety of particle beams for basic research and applications in industry and medicine. Diagnostic tools have been developed and optimised according to the special requirements of these machines and to meet the demands of their users. Storage rings for ultra cooled heavy ion beams, third generation synchrotrons for the production of high brilliant radiation, super conducting protons machines working at the energy frontier and finally linear electron accelerators for FEL applications or high energy physics are just the most prominent representatives of the large variety of accelerators and each of them needs highly sophisticated tools to measure and optimise the corresponding beam parameters. Accordingly the issue addressed here is not to cover in full detail the different diagnostic devices but rather to concentrate on the aspects and needs as seen by the accelerator physicists and machine designers.

 

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MOOA03 Beam Diagnostic System of XFEL/SPring-8 cavity, electron, FEL, status 11
 
  • H. Maesaka, A. Higashiya, S.I. Inoue, S.M. Matsubara, T. Ohshima, Y. Otake, T. Shintake, M. Yabashi
    RIKEN/SPring-8, Hyogo
  • H. Ego, H. Tomizawa, K. Yanagida
    JASRI/SPring-8, Hyogo-ken
 
 

We present the design and performance of the beam diagnostic system of XFEL/SPring-8. The XFEL accelerator requires sub-um resolution beam position monitors (BPM), few-um resolution screen monitors, high-speed beam current monitors and a ten femtosecond resolution temporal structure measurement system. We designed an rf cavity BPM which has a resonant frequency of 4760 MHz and a position resolution of less than 1 um. For the screen monitor, thin stainless-steel foil (0.1 mm thick) is used to reduce beam divergence. In addition, a custom-made lens system having few-micron resolution was designed. For the beam measurement, we developed a differential current transformer (CT) with four ports, two are positive and the others are negative, to reduce common-mode noise. The rise time of the CT output pulse is 0.1 ns. To measure the temporal structure of a beam, we developed a C-band (5712 MHz) transverse deflecting cavity that has a disk-loaded backward traveling wave structure. The iris shape of the cavity is a race-track to separate x- and y-mode. This cavity can resolve a beam into femtosecond fragments. Thus, the beam diagnostic system satisfies the demands of the XFEL machine.

 

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MOOB01 Highlights from BIW'08 instrumentation, radiation, photon, synchrotron 14
 
  • F. Sannibale
    LBNL, Berkeley, California
 
 

The 13th edition of the Beam Instrumentation Workshop (BIW08) took place at the Granlibakken Conference Center on the beautiful shores of Lake Tahoe in California during the first week of May 2008. About 130 participants registered for the workshop. Included in the program during the three and a half days were three tutorials, eight invited and seven contributed oral presentations, and more than 50 poster contributions. A discussion group session, and the vendor exhibition simultaneously held with the single day poster session, afforded many opportunities for informal discussion and idea exchange between attendees. During the workshop, the 2008 Faraday Cup Award that recognizes innovative achievements in beam diagnostics was also presented. In this talk, I will present the highlights from BIW08. The overall quality of the contributions was notably high, which made the selection of the topics for this talk quite difficult. Although I endeavored to produce a balanced choice of highlights, the final list is surely incomplete due to time limitations of the talk, and also it unavoidably reflects my personal point of view and preferences.

 

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MOOB02 Commissioning Results of Beam Diagnostics for the PETRA III Light Source feedback, wiggler, damping, emittance 19
 
  • K. Balewski, A. Brenger, H.T. Duhme, V. Gharibyan, J. Klute, K.K. Knaack, I. Krouptchenkov, G. Kube, T. Lensch, J. Liebing, Re. Neumann, Ru. Neumann, G. Priebe, F. Schmidt-Föhre, H.-Ch. Schröder, R. Susen, S. Vilcins, M. Werner, Ch. Wiebers, K. Wittenburg
    DESY, Hamburg
 
 

PETRA III is a new hard x-ray synchrotron radiation source which will be operated at 6 GeV with an extremely low horizontal emittance of 1 nmrad. This new facility is the result of a conversion of the existing storage ring PETRA II into a light source. The conversion comprises the complete rebuilding of one eighth of the 2304 m long storage ring, which will then house 14 undulator beam lines, the optical and experimental hutches, and the modernization and refurbishment of the remaining seven eighths. In addition two 100 m long damping wiggler sections have been installed which are required to achieve the small design emittance. Construction, installation and technical commissioning have been finished middle of March and then the commissioning with beam started. In this paper we present the results that have been achieved during commissioning with special emphasis on the role of diagnostic systems.

 

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MOOB03 SSRF Beam Diagnostics System Commissioning booster, feedback, linac, synchrotron 24
 
  • Y.B. Leng, Y.Z. Chen, K.R. Ye, W.M. Zhou
    SSRF, Shanghai
 
 

SSRF is a 432 m-circumference synchrotron light source with a 150MeV linac, a 3.5GeV full energy booster, and a 3.5GeV storage ring. Principal diagnostics systems have been installed and nearly all have been commissioned during past two years. Data have been obtained on beam position, beam profile, current, and synchrotron radiation diagnostics beamline on the storage ring. Multi bunch transverse feedback system has been applied on the ring. Results for the 150MeV electron beams in the linac, up to 3.5GeV in the booster, and 3.5GeV in the ring will be presented.

 

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MOPD01 Non-Destructive Beam Position Measurement in a Proton Therapy Beam Line proton, pick-up, cyclotron, ion 41
 
  • D.T. Fourie, L.S. Anthony, A.H. Botha, J.L. Conradie, J.G. De Villiers, J.L.G. Delsink, P.F. Rohwer, P.A. van Schalkwyk
    iThemba LABS, Somerset West
  • J. Dietrich
    FZJ, Jülich
 
 

Non-destructive beam position monitors (BPMs) have been in use at iThemba LABS for several years in the neutron therapy and radioisotope production beamlines, as well as in the transfer lines between the K200 separated-sector cyclotron and the two K8 injector cyclotrons. The sensitivity of these BPMs is limited by noise and pickup from the RF systems to about 300 nA in the high energy beam lines. For proton therapy, using the scattering method, position measurement at beam currents as low as 20 nA have to be made. A new and more sensitive BPM as well as the electronic measuring equipment, using RF pickup cancellation and improved filtering, have been developed and installed in the proton therapy beamline. The BPM, the electronic equipment and the results of measurements at beam currents down to 10 nA for 200 MeV protons are described.

 
MOPD06 Design of Beam Position Monitors for the IFMIF-EVEDA accelerator simulation, cryomodule, vacuum, status 53
 
  • I. Podadera Aliseda, B. Brañas, A. Ibarra
    CIEMAT, Madrid
  • J. Marroncle
    CEA, Gif-sur-Yvette
 
 

The IFMIF-EVEDA accelerator will be a 9 MeV, 125 mA CW deuteron accelerator which aims to validate the technology that will be used in the future IFMIF accelerator. Non-interceptive Beam Position Monitors pickups (BPMs) will be installed to measure the transverse beam position in the vacuum chamber in order to correct the dipolar and tilt errors. Depending on the location, the response of the BPMs must be optimized for a beam with an energy range from 5 up to 9 MeV and a current between 0.1 and 125 mA. Apart from the broadening of the electromagnetic field due to the low-beta beam, specific issues are affecting some of the BPMs: tiny space in the transport line between the RFQ and cryomodule (MEBT), cryogenic temperature inside the cryomodule, phase and energy measurement in the diagnostics plate, and debunching and big vacuum pipe aperture at the end of the high energy beam transport line. For this reason different types of BPMs are being designed for each location (MEBT, cryomodule, Diagnostics Plate and High Energy Beam Tranport Line). In this contribution, the design of each BPM will be presented, focusing on the electromagnetic response for high-current low-beta beams.

 
MOPD16 Comparative Studies of RF Beam Position Monitor Technologies for NSLS II brilliance, photon, vacuum, injection 80
 
  • O. Singh, I. Pinayev
    BNL, Upton, Long Island, New York
  • G. Decker, B.X. Yang
    ANL, Argonne, Illinois
 
 

Sub-micron beam stability is a necessary performance requirement for the NSLS II light source, a substantial challenge testing the limits for presently available RF beam position monitoring methods. Direct performance comparisons between commercially available bpms and Advanced Photon Source in-house developed bpm were made at the APS Storage Ring. Noise floor, fill pattern dependence, and intensity dependence were investigated and correlated with photon diagnostics at the beam diagnostic beamline at APS sector 35. Key results will be presented.

 
MOPD21 SNS Beam Diagnostics: Present Status and Future Plans laser, neutron, linac, emittance 95
 
  • A.V. Aleksandrov
    ORNL, Oak Ridge, Tennessee
 
 

The Spallation Neutron Source accelerator systems will deliver a 1.0 GeV, 1.4 MW proton beam to a liquid mercury target for neutron scattering research. The accelerator complex consists of an H- injector, capable of producing one-ms-long pulses at 60 Hz repetition rate with 38 mA peak current, a 1 GeV linear accelerator, an accumulator ring and associated transport lines. The accelerator systems are equipped with variety of beam diagnostics. The beam diagnostics played important role during beam commissioning, they are used for accelerator tuning and monitoring beam status during production runs. The requirements to the various diagnostics systems are changing in the process of beam power ramp up. This talk will give an overview of the evolution of the major SNS beam diagnostics systems: commissioning, operation, power ramp up, and power upgrade.

 
MOPD24 An Overview of the Proposed Beam Diagnostic for ASTRID2 injection, storage-ring, emittance, synchrotron 101
 
  • J.S. Nielsen, N. Hertel, S.P. Møller
    ISA, Aarhus
 
 

This paper presents an overview of the proposed beam diagnostic for Astrid2, which is the new 580 MeV 3rd generation synchrotron light source to be build in Aarhus, Denmark. Astrid2 will use the present Astrid1 as booster, allowing for full energy injection and thereby top-up-operation. The diagnostics will include viewers, beam current monitors, electronic beam position monitors, striplines, etc. The description will include both the storage ring and the transfer beam line.

 
MOPD27 SPIRAL2 Injector Diagnostics ion, linac, emittance, ion-source 110
 
  • P. Ausset
    IPN, Orsay
  • T.A. André, C. Doutresssoulles, B. Ducoudret, C. Jamet, W. Le Coz, F. Lepoittevin, E. Swartvagher, J.L. Vignet
    GANIL, Caen
  • C. Maazouzi, C.O. Olivetto, C. Ruescas
    IPHC, Strasbourg Cedex 2
 
 

The future SPIRAL2 facility will be composed of a multi-beam driver accelerator (5mA/40Mev deuterons, 5mA/33MeV protons, 1mA/14.5 MeV/u heavy ions) and a dedicated building for the production of radioactive ion beams (RIBs). RIBs will be accelerated by the existing cyclotron CIME for the post acceleration and sent to GANIL’s experimental areas. The injector, constituted by an ion source, a deuterons/protons source, a room temperature RFQ and the MEBT line, will produce and accelerate beams to an energy of 0,75MeV/u. An Intermediate Test Bench (B.T.I.) is being built to commission the SPIRAL2 Injector through the first re-buncher of the MEBT line in a first step and the last re-buncher in a second step. The B.T.I. is designed to perform a wide variety of measurements and functions and to go more deeply in the understanding of the behaviour of diagnostics under high average intensity beams operations. A superconducting LINAC with two types of cavity will allow reaching 20 MeV/u for deuterons beam. This paper describes injector diagnostic developments and gives information about the current progress.

 
MOPD30 Beam Diagnostics for SPIRAL2 RNB Facility controls, ion, target, radiation 116
 
  • P. Anger, T.A. André, A. Delannoy, E. Gueroult, B. Jacquot, C. Jamet, G. Ledu, A. Savalle, F. Varenne, J.L. Vignet
    GANIL, Caen
  • J.-M. Fontbonne, N. Orr
    LPC, Caen
 
 

The SPIRAL2 project is based on a multi-beam driver facility in order to allow both ISOL and low-energy in-flight techniques to produce intense radioactive ion beams (RIB) in a new Facility. A superconducting linac capable of accelerating 5-mA deuterons up to 40 MeV is used to bombard both thick and thin targets. These primary beams will be used for the RIB production by several reaction mechanisms (fusion, fission, etc.) The production of high intensity RIB will be based on fission of uranium target induced by neutrons. These exotic particles will be produced, ionized, selected in a dedicated production building and transported to the existing CIME cyclotron for post acceleration. After this, they will be used in the present experimental area of GANIL. The construction phase of SPIRAL2 was officially started in 2005. The beam diagnostics for the production facility allow a pre-tuning with a stable beam followed by an extrapolation to the radioactive beam. Some diagnostic devices may also provide for equipment protections and for the safety systems. An overview is presented of the diagnostics which will allow tuning and control of the RIB in this new production facility.

 
MOPD31 Beam Diagnostics in the CNAO Injection Lines commissioning emittance, electron, dipole, ion 119
 
  • G. Balbinot, E. Bressi, M. Caldara, A. Parravicini, M. Pullia, M. Spairani
    CNAO Foundation, Milan
  • C. Biscari
    INFN/LNF, Frascati (Roma)
  • J. Bosser
    CERN, Geneva
 
 

The CNAO, the first Italian center for deep hadrontherapy, is presently in its final step of installation. It will deliver treatments with active scanning both with Proton and Carbon ion beams. Commissioning of the low energy injection lines has been successfully concluded in January 2009. CNAO beams are generated by two ECR sources which are both able to produce both particle species. The beam energy in the Low Energy Beam Transfer (LEBT) line is 8 keV/u. A compact and versatile tank containing a complete set of diagnostic tools has been intensively used for the line commissioning: in a length of 390mm it houses two wire scanners, for vertical and horizontal beam transverse profile, a Faraday Cup, for current measurement, and two vertical and horizontal plates for beam halo suppression , emittance measurements, beam collimation and particles selection. Using one tank devices, phase space distribution reconstruction can be quickly performed as well as synchronous profiles and intensity measurements. Commissioning results and measurements are presented.

 
MOPD32 Beam Diagnostics at the ALBA Linac linac, klystron, synchrotron, vacuum 122
 
  • U. Iriso, A. Olmos, F. Peréz
    CELLS-ALBA Synchrotron, Cerdanyola del Vallès
 
 

The commissioning of the ALBA Linac (Autumn 2008) required a careful measurement of the beam parameters. This paper describes the diagnostics devices installed at the ALBA Linac and our experience with them.

 
MOPD33 Diagnostics Overview of the Taiwan Photon Source storage-ring, booster, synchrotron, emittance 125
 
  • K.T. Hsu, K.H. Hu, C.H. Kuo, C.Y. Wang
    NSRRC, Hsinchu
 
 

A new high brilliant 3 GeV storage-ring-based light source - Taiwan Photon Source (TPS) - is planned to be built at the National Synchrotron Radiation Research Center. Various diagnostics will be deployed to satisfy stringent requirements for commissioning, operation, and top-off injection of the TPS. Specifications and an overview of the planned beam instrumentation system for the TPS will be summarized in this report. Efforts in diagnostic devices and subsystems will also be addressed.

 
MOPD42 ProfileView - A Data Acquisition System for Beam Induced Fluorescence Monitors controls, electron, instrumentation, radiation 134
 
  • R. Haseitl, C.A. Andre, F. Becker, P. Forck
    GSI, Darmstadt
 
 

At the GSI Linac and transfer lines several Beam Induced Fluorescence Monitors (BIF) for transverse profile determination are installed. The non-intercepting measurement principle is based on the excitation of residual gas molecules by the beam and the detection of the fluorescence photons with image intensified cameras. This allows simultaneous profile determination at multiple positions without beam disturbance. The software ProfileView is a data acquisition system to visualize and record the profiles of several BIF monitors along the beamline. One BIF monitor comprises two image intensified cameras with remote irises, timing interface, gas pressure control and remote reset functionality. The basic functions needed for daily operation are combined in an easy-to-use graphical user interface. Beside this 'operator mode' an 'expert mode' can be called by advanced users to control every hard- or software parameter of the whole system separately. This contribution describes the software design and its realization for communication and data display.

 
TUOA01 Sliced Beam Parameter Measurements emittance, simulation, quadrupole, FEL 146
 
  • D. Alesini, M. Castellano, E. Chiadroni, L. Cultrera, G. Di Pirro, M. Ferrario, L. Ficcadenti, D. Filippetto, G. Gatti, E. Pace, C. Vaccarezza, C. Vicario
    INFN/LNF, Frascati (Roma)
  • A. Cianchi, B. Marchetti
    INFN-Roma II, Roma
  • A. Mostacci
    Rome University La Sapienza, Roma
  • C. Ronsivalle
    ENEA C.R. Frascati, Frascati (Roma)
 
 

One of the key diagnostics techniques for the full characterization of beam parameters for LINAC-based FELs foresees the use of RF deflectors. With these devices it is possible to completely characterize both the longitudinal and the transverse phase space. In the talk I will present the main design considerations for time resolved (sliced) beam parameter measurements using RF deflectors. Measurement setups for longitudinal pulse shape as well as phase space and transverse beam slice emittance characterizations are described. The main sources of errors are discussed and the design criteria of these devices are presented. In particular the SPARC RF deflector and the related diagnostic lines as well as recent measurement results from the SPARC facility are shown. RF deflectors in use or planned to be used in other FEL labs are then illustrated with an overview of these activities.

 

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TUOA04 Electron Beam Diagnostics for the European XFEL cavity, undulator, electron, linac 158
 
  • D. Nölle
    DESY, Hamburg
 
 

The European XFEL is an X-ray free-electron-laser that is currently being built in Hamburg. It is organized as an international Project and will be a large scale user facility. Based on superconducting TESLA technology electron beams of high average power will be send to several undulator lines simultaneously to produce hard X-Rays with high average intensity and a peak brilliance by far superior to any 3rd generation light source. This paper will present the current status of the planning, the development and the prototyping process for this facility. It will cover as well as the BPM system, the other main diagnostic systems, like beam size measurements, charge, dark current and beam loss and protection systems.

 

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TUPB06 Transverse Profile Monitors based on Fluorescence for IFMIF-EVEDA Accelerator neutron, radiation, photon, optics 173
 
  • J.M. Carmona, B. Brañas, A. Ibarra, I. Podadera Aliseda
    CIEMAT, Madrid
 
 

The IFMIF-EVEDA accelerator will be a 9 MeV, 125 mA (CW) deuteron LINAC with the purpose of validating the technology that will be used in the future IFMIF accelerator. In such low energy and high current prototype accelerator, any device intercepting the beam could be destroyed. Thus, non interceptive profile monitors will be installed inside of a Diagnostics-Plate and along the High Energy Transport Line. CIEMAT group investigates a profile monitor based on the fluorescence of the residual gas. A high neutron and gamma flux environment (due to high deuteron beam current) stands for a hostile environment for most of electronic devices and fibers. The design must guarantee not only good spatial resolution but a reliable operation in such environment. Hence, different options for detectors, optical windows, fibers and shielding concepts have been considered to overcome these aspects. Transverse profilers will be used as well as a tool to perform emittance measurements through quad-scans. In this contribution, the design of a transverse profiler prototype for EVEDA, together with a brief discussion about mechanisms that can play a role in profile falsification will be presented.

 
TUPB07 The Beam Profile Monitor for SPIRAL2 ion, linac, target, controls 176
 
  • J.L. Vignet, M. Blaizot, S.C. Cuzon, A. Delannoy, J.-C. Foy, P. Gangnant, E. Gueroult, C. Houarner
    GANIL, Caen
 
 

The SPIRAL2 project is based on a multi-beam driver in order to allow both ISOL and low-energy in-flight techniques to produce Radioactive Ion beams (RIB). A superconducting light/heavy-ion LINAC capable of accelerating 5 mA deuterons up to 40 MeV and 1 mA ions up to 14.5 MeV/u is used to bombard both thick and thin targets. These beams could be used for the production of intense RIB by several reaction mechanisms (fusion, fission, transfer, etc.). In order to visualize the SPIRAL2 beam dynamics, several beam profile monitors are under development. Multiwire beam profile monitors (SEM) will be used on the driver and RIB lines, a non interceptive beam profile monitor (RGM) should be mounted on the LINAC diagnostics box and before the experiment facility, and a low intensity beam profile monitor (EFM) on the RIB lines. Signal acquisition from these monitors will be accomplished through new associated electronics which digitize 94 channels in a parallel system. Each channel integrates the current of the associated wire or strip and performs a current-voltage conversion. The dedicated GANIL data display software has been adapted for these new monitors.

 
TUPB13 IR Photon Array Detector for Bunch by Bunch Transverse Beam Diagnostics positron, synchrotron, collider, radiation 194
 
  • A. Bocci, M. Cestelli Guidi, A. Clozza, A. Drago, A.G. Grilli, A. Marcelli, A.R. Raco, R.S. Sorchetti
    INFN/LNF, Frascati (Roma)
  • A. De Sio, E.P. Emanuele, E. Pace
    Università degli Studi di Firenze, Firenze
  • L. Gambicorti
    INOA, Firenze
  • J.P. Piotrowski
    VIGO System S.A., Ozarow Maz.
 
 

Beam diagnostics based on synchrotron radiation can use imaging techniques that allow monitoring beam transverse dimensions in real time. In particular the bunch-by-bunch transverse beam diagnostics is a powerful method that allows investigations of transient phenomena in which bunch motion and beam instabilities are correlated to the position in the bunch train. Such diagnostic methods need photon array detectors with response time in the ns down to ps range and dedicated fast electronics. At DAΦNE, the e+/e- collider of LNF/INFN, preliminary measurements with a prototype of an IR array detector made by 32x2 pixels are in progress. The array has pixel of 50x50 μm2 characterized by a response time of about 1 ns per pixel measured with the IR emission of the SINBAD beamline. The array detector and the 64 channels dedicated electronics has been installed at the 3+L experiment, a dedicated diagnostics of the e+ DAΦNE ring used to monitor the transverse dimensions of the beam. In this paper we describe the apparatus built to obtain IR imaging of a SR source and a turn-by-turn and a bunch-by-bunch transverse diagnostics of the stored bunches with a sub-ns time resolution

 
TUPB14 Diagnostics for High Power Ion Beams with Coherent Fiber for IFMIF-EVEDA Injector proton, radiation, simulation, neutron 197
 
  • F. Senée, G. Adroit, R. Gobin, B. Pottin, O. Tuske
    CEA, Gif-sur-Yvette
 
 

Optical diagnostics based on the excitation of residual gas molecules are routinely used for high intensity beam characterization. Beam intensity, beam position and profile are measured by means of a CCD sensor. In addition species fraction and profile of each beam are measured using a Doppler shift method. As part of IFMIF-EVEDA* project, CEA is in charge of the design and realization of the 140mA-100keV cw deuteron source and low energy beam transport line. In the beam line, (D,d) reaction will occur and high neutron flux will be emitted when deuteron beam interacts with surfaces. Moreover gamma ray and activation will also occur. In order to protect diagnostics, coherent optic fibers could be used to transport the beam image outside the irradiated zone. A comparative study of two coherent fibers will be presented (FUJIKURA & SCHOTT), along with the characterization in magnification and attenuation of a 610 mm long fiber and its associated optics. To estimate the capability of such fibers to transport beam image, a dedicated experiment has been performed with proton beam produced by the SILHI source. The beam transverse profile has been compared with and without the optic fiber.


* International Fusion Materials Irradiation Facility - Engineering Validation and Engineering Design Activities

 
TUPB22 Design Report of a Non-Destructive Emittance Instrument for RAL's Front End Test Stand FETS emittance, laser, dipole, ion 213
 
  • C. Gabor
    STFC/RAL/ASTeC, Chilton, Didcot, Oxon
  • A.P. Letchford
    STFC/RAL, Chilton, Didcot, Oxon
  • J.K. Pozimski
    Imperial College of Science and Technology, Department of Physics, London
 
 

The RAL front end FETS is currently under construction to demonstrate an H-ion beam with up to 18 kW at 3 MeV. Due to the beam power photo detachment techniques are the preferable choice for emittance instruments. Typically, measurements will be performed in just one transverse plane by using a magnet to separate ion beam from produced neutrals. Another general technique to work out a 2D emittance bases on several beam profiles applying an image reconstruction method called maximum entropy (MaxEnt). Combining both methods in one device has the significant advantage of reducing technical and physical problems which may occur by doubling magnet or laser beam path. Drawback of MaxEnt is the necessity of sufficient phase space advance to achieve reasonable results which can be either optimised by moving the particle detector or with additional focusing. The paper presents a conceptual design study discussing all possible constraints given by beam parameters and chopper/ MEBT. Simulations will help to estimate performance and errors.

 
TUPB28 Loss Monitor on Basis of Diffusive Radiation from Rough Surfaces radiation, photon, vacuum, scattering 231
 
  • S.G. Arutunian, Zh.S. Gevorkian, K.B. Oganesyan
    YerPhI, Yerevan
 
 

Diffusive Radiation (BR) is originated by the passage of charged particles through or near a randomly inhomogeneous medium. DR appears when the conditions for multiple scattering of pseudophotons are fulfilled in the medium. Such a situation can be realized when a charged particle slides over a rough metallic surface. One of the important properties of DR is that the emission maximum lies at large angles from particle velocity direction. Therefore it can be used for detection of beam touch to the accelerators vacuum chamber wall in case when generated photons will be observed on the opposite side of the vacuum chamber. Such a diagnostics can be especially useful for observation of storage ring beams halo. Corresponding proposal is presented in the paper.

 
TUPB37 Coherent Optical Transition Radiation as a Tool for Ultra-Short Electron Bunch Diagnostics electron, laser, radiation, undulator 251
 
  • G. Geloni, P. Ilinski, E. Saldin, E. Schneidmiller, M.V. Yurkov
    DESY, Hamburg
 
 

In this contribution we describe how Coherent Optical Transition Radiation can be used as a diagnostic tool for characterizing electron bunches in X-ray Free-electron lasers. The proposed method opens up new possibilities in the determination of ultra-short, ultra-relativistic electron bunch distributions.

 
TUPB42 A Compact Single Shot Electro-Optical Bunch Length Monitor for the SwissFEL laser, electron, FEL, vacuum 263
 
  • B. Steffen, V. Schlott
    PSI, Villigen
  • F. Müller
    IAP Univ. Bern, Bern
 
 

The knowledge and control of electron bunch lengths is one of the key diagnostics in XFEL accelerators to reach the desired peak current in the electron beam. A compact electro-optical monitor was designed and build for bunch length measurements at the Swiss FEL. It is based on a mode locked ytterbium fiber laser probing the field-induced birefringence in an electro-optically active crystal (GaP) with a chirped laser pulse. The setup allows the direct time resolved single-shot measurement of the Coulomb field (THz-radiation) of the electron beam -and therefore the bunch length- with an accuracy as good as 200fs. Simulations of the signals expected at the SwissFEL and the results of first test at the SLS linac will be presented.

 
TUPD06 Optimisation Studies of a Resonant Capacitive Pick-Up for Beam Position Monitoring of Low Intensity, Low Velocity Antiproton Beams at FLAIR pick-up, antiproton, coupling, monitoring 300
 
  • J. Harasimowicz
    Cockcroft Institute, Warrington, Cheshire
  • J. Harasimowicz, C.P. Welsch
    The University of Liverpool, Liverpool
 
 

The Ultra-low energy Storage Ring (USR) at the future Facility for Low-energy Antiproton and Ion Research (FLAIR) at GSI, Germany will decelerate antiproton beams of very low intensities from 300 keV down to 20 keV. Such beams can be easily disturbed by standard monitoring devices and the development of new sensitive diagnostic techniques is required. To overcome the limitations related to a very low number of particles, a low signal-to-noise ratio and ultra-low kinetic energies, a resonant capacitive pick-up has been proposed as a beam position monitor. In the planned solution, the signal gain will be realised by the use of a specially designed resonant circuit optimized to meet the requirements of the USR. The current overall design studies of the resonant capacitive pick-up, including simulations of the beam displacement sensitivity and linearity for different pick-up geometries and the equivalent resonant circuit optimisation, will be discussed.

 
TUPD24 High Dynamic Range Spectral Analysis in the kHz Band instrumentation, impedance, power-supply, controls 348
 
  • M. Gasior, A. Boccardi
    CERN, Geneva
 
 

Many beam instrumentation signals of large circular accelerators are in the kHz range and can thus be digitised with powerful high resolution ADCs. A particularly large dynamic range can be achieved if the signals are analysed in the frequency domain. This report presents a system employing audio ADCs and FPGA-based spectral analysis, initially developed for tune measurement applications. Technical choices allowing frequency domain dynamic ranges beyond 140 dB are summarised.

 
TUPD30 Measurement Devices for the SPARC Synchronization System cavity, laser, linac, FEL 363
 
  • M. Bellaveglia, D. Alesini, A. Gallo, C. Vicario
    INFN/LNF, Frascati (Roma)
 
 

The SPARC FEL facility is under commissioning at the Frascati National Laboratories of INFN. The synchronization system is working as expected and various devices are used to monitor its performances. In particular this paper is focused on a comparison between the results obtained using different methods and instruments to perform laser, RF and beam synchronization measurements. Both electro-optical and full electrical techniques are used to obtain information about the phase noise of the RF fields inside the accelerating structures, the phase noise of the IR laser oscillator, the time of arrival of the laser UV pulse on the cathode and the time of arrival of the accelerated electron bunch at a selected reference position along the linac.

 
TUPD39 Investigation of the Light Yield of Luminescent Screens for High Energetic and High Brilliant Electron Beams electron, background, radiation, ion 387
 
  • G. Kube
    DESY, Hamburg
  • W. Lauth
    IKP, Mainz
 
 

For the European XFEL with a maximum beam energy of 20 GeV and an average beam power of up to 300 kW it is planned to install beam profile monitors in the dump sections in order to control beam position and size. Usually OTR monitors are used for electron profile measurements. For intense beams however, thermal load in the screen material may result in resolution degradation and even screen damage. To overcome this problem the beam can be swept over the screen, but the strong OTR light emission directivity will reduce the optical system's collection efficiency. Therefore it is planned to use luminescent screens because of their robustness and isotropic light emission. While only little information is available about scintillator properties for applications with high energetic electrons, a test experiment has been performed at the 855 MeV beam of the Mainz Microtron MAMI in order to study light yield and robustness of different screen materials like Aluminum and Zirconium oxide under electron bombardment. The results will be compared to independent measurements from studies with heavy ion beams.

 
TUPD45 Screen Monitor Design for the SwissFEL electron, gun, emittance, vacuum 405
 
  • R. Ischebeck, B. Beutner, V. Schlott, B. Steffen
    PSI, Villigen
 
 

A screen monitor containing OTR foils and scintillator crystals has been designed to measure the transverse profile of electron bunches in the PSI-XFEL. In conjunction with quadrupole magnets in FODO cells and a transverse deflecting structure, the screen monitors will be used to measure transverse and longitudinal phase space projections of the electron pulses in the 250 MeV Injector. Tomographic methods will be used to reconstruct the phase space distributions.

 
WEOA02 Intensity and Profile Measurement for Low Intensity Ion Beams in an Electrostatic Cryogenic Storage Ring shielding, cryogenics, ion, vacuum 418
 
  • T. Sieber, K. Blaum, M. Grieser, F. Laux, D. Orlov, A. Wolf, R. von Hahn
    MPI-K, Heidelberg
 
 

The cryogenic storage ring CSR is a 35 m circumference electrostatic ring, for molecular- and atomic physics experiments at MPI-K Heidelberg. It will operate at pressures down to 10-13 mbar and temperatures <10 K. The beam intensities will be in the range of 1 nA to 1 uA, particle energies are between 20 - 300 keV. An intensity measurement for coasting beams below 1 uA requires magnetic field detection devices, which are much more sensitive than existing DC beam transformers. The highest sensitivity is currently achieved with DC SQUID based cryogenic current comparators (CCCs). At GSI, a prototype of such a CCC was successfully tested in the mid 90’s, reaching a resolution of ~250 pA/Hz1/2. Recently a resolution of 40 pA/Hz1/2 could be achieved under laboratory conditions at Jena University, however, the CCC sensitivity in an accelerator environment depends strongly on efficient shielding and mechanical decoupling. We describe our work on adaptation and improvement of the CCC beam transformer for the CSR. Furthermore a concept for an ionisation profile monitor is discussed, which in addition to low beam intensities, has to cope with extremely low gas densities at 10-13 mbar.

 

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WEOA04 Beam Diagnostic Developments for FAIR synchrotron, ion, impedance, storage-ring 424
 
  • M. Schwickert, P. Forck, T. Giacomini, P. Kowina, H. Reeg, A. Schlörit
    GSI, Darmstadt
 
 

The FAIR (Facility for Antiprotons and Ions Research) accelerator complex is currently designed and projected at GSI. The unique features of the central machine SIS100, like e.g. the acceleration of high intensity beams of 2.5·1013 protons and 5·1011 Uranium ions, the operation close to the space charge limit leading to a large tune spread and the extreme UHV conditions of the cryogenic system for fast ramped superconducting magnets, make challenging demands on the beam diagnostic components. This contribution describes the general concept of beam diagnostics for FAIR and reports on the present status of prototype studies. Exemplarily the achievements for a novel type of dc transformer, beam position monitors and the ionization profile monitor are discussed and first measurements with prototype setups are presented.

 

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WEOB01 Beam Diagnostics and RF Systems Requirements for the SwissFEL Facility linac, klystron, photon, emittance 427
 
  • Y. Kim, B. Beutner, H.-H. Braun, A. Citterio, M. M. Dehler, A. Falone, R. Ganter, T. Garvey, S. Hunziker, R. Ischebeck, B. Keil, M. Pedrozzi, S. Reiche, T. Schilcher, V. Schlott, B. Steffen
    PSI, Villigen
 
 

In this paper, we describe four very different operating modes of the SwissFEL facility, the requirements of the challenging beam diagnostics and ultra-stable RF systems needed for two special operating modes with 10 pC, and the present status of developing beam diagnostics and RF systems for the PSI 250 MeV injector test facility, which is under construction.

 

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