Status of the SOLEIL project Commissioning from Linac to beamlines
|
|
|
- Felicia Newton
- 10 years ago
- Views:
Transcription
1 Status of the SOLEIL project Commissioning from Linac to beamlines On behalf of the commissioning team 2 D01-1-CX1/DT/DTC/absorption Y Axis Title X Axis Title 1
2 Site and Budget at Gif-sur-Yvette 25km south of Paris, France 350 permanent staff 19 Hectares Total budget for period 454 M Investments 248 M Functioning 53 M Salaries 153 M Functioning budget per year starting in 2010: ~ 45 M. CEA and CNRS own 28% and 72% of the Synchrotron Soleil company respectively. 2
3 SOLEIL Characteristics Electron energy: 2.75 GeV Extended spectral range From UV (5 ev) up to hard X-Rays (30 kev) 3 rd generation Many Insertion Device beamlines 21 straight sections available (29% of ring circ.) High brilliance (10 20 ) in the soft X-ray range small emittance and high intensity Best achievable beam position stability 3
4 24 beamlines 24 Beamlines approved by the Council + 1 beamline to be founded 18 on insertion devices and 7 on bending magnets Spectral range equally shared : 50% below 1.3 kev and 50% above Phase 1: 11 beamlines being built =>open to external Users in on insertion devices and 3 on bending magnets + 2 IR Phase 2: 7 beamlines open to external Users in on insertion devices and 2 on bending magnets + 7 beamlines on ID open to external Users in Straight sections still free + 14 bending magnet beamports! 4
5 LINAC and Booster designed for topping-up operation 2.75 GeV BOOSTER 2 super periods Circumference: 157 m 36 Dipoles : 0.67 T / 2.17 m LINAC 100 MeV 3 Hz rep Rate Output charge : 8 nc in 300 ns in multibunch mode (500 ma in SR) 44 Qpoles: 10.3 T/m m Emittance: nm.rad Power supplies cycling at 3 Hz 1.5 nc in 3 pulses (2ns) in 8 bunch mode (90 ma in SR) 5
6 LINAC turn key system provided by THALES: 1st beam on July 2nd 2005 Excellent performances: stability/reproducibility Spec. : (γε at 90 %) γε at 90 %) < 200.mm.mrad Final Acceptance pronounced on November 15th, 2005 Mode Long Pulse Short Pulse (1) Short Pulse (4) Beam Charge 10.6 nc 0.55 nc 2.27 nc Horizontal π mm.mrad Vertical π mm.mrad
7 Booster ring commissioning Tunes kept within ± 0.05 Booster Efficiency ~ % 1 st beam in the Booster at 110 MeV July 23rd, power supplies (Bruker( Bruker) ) ramped at 3 Hz: Tracking ± 0.2 % Beam decelerated down to 140 MeV 7
8 Storage Ring main parameters Energy Circumference RF frequency Harmonic number Betatron tunes (H/V) Natural chromaticities (H/V) Momentum compaction Momentum compaction α 1 / α 2 Radiation loss per turn (with IDs) Damping times Emittance Relative energy spread Natural bunch length (@ 4 MV) Coupling Multibunch mode Expected Beam Lifetime / / x x 10-4 / , 7, x GeV m MHz kev ms nm.rad mm % ma h 8
9 Specificities and innovative aspects High ratio (43 %) of ID straight sections over total 354 m circumference Extreme requirements for beam stability Specific super-conducting cavities (352 MHz) RF power generator: solid state amplifier of 4 x 190 kw (never done) Innovative insertion devices Al chamber vessels with NEG coating (56 % of the circumference) New type of BPM digital electronics: LIBERA module 9
10 Commissioning Milestones in effective weeks 5/14 First turn 6/04 First stored beam 6/04 First beam accumulation: 8.35mA 7/04 100mA achieved 7/10 5 A.h beam dose shutdown 7/11 9/4 (water + holidays) 9/13 First photons to a beamline (DIFFABS) 9/16 200mA 9/21 First photons to a beamline (TEMPO) 9/25 300mA achieved ; 30A.h 9/29 U20 at 5.5 mm gap 9/21 First photons to a beamline (ODE) 10/15 beam lifetime = 100mA in 312 bunches shutdown 10/16 12/01 (21 water circuit cleaning ) 12/12 First photons to a beamline (SAMBA) 12/13 first photons to a beamline (DESIRS) 12/21 75 A.h beam dose 12/21 beam lifetime 100mA in 312 bunches 10
11 Expected obstacles: 10mm inner height ID vacuum vessels since the first day on 10 medium straight sections HU256 U80 11
12 Unexpected obstacles: Bad mounting of some RF Fingers in short straight sections RF finger at 1.5 mm from beam axis! But the beam went nicely through these very small apertures! Problem fixed now (they all have been replaced) 12
13 Measured Closed Orbit With All Correctors switched OFF. (BPM offsets included after BBA) H-plane Rms = 3.1mm Max = 6.4mm V-plane Rms = 0.4mm Max = 1.4mm 13
14 Closed Orbit Correction after the Application of the Beam Based Alignment 56 correctors in each plane and 120 BPMs. H-orbit rms = 68µm max = 225µm rms HCOR 1.1 A 1 A 48 singular values V-orbit rms = 58µm max = 190µm 32 singular values rms VCOR 2.0 A 0.4 A 14
15 Quadrupole Beam Based Alignment Minimize the merit function Statistics of the offsets (first iteration) σ x = 153 µm X mean =132µm σ z = 170 µm Z mean =-150µm 15
16 Storage Ring: magnetic measurements Very careful metrology to reach excellent alignment alignment of the Magnetic measurement bench May 2004-Aug Magnetic measurements of 326 electro-magnets: magnetic axis centering, field properties Rotating coil bench built to reach magnetic centering to ± 25 µm and tilt ±0.1mrad 16
17 Storage Ring: Q-Magnet Q alignment Z (mm) ANS Qpoles (magnetic centres) Altimetry Mar 06 with N3 optical level rms: appr mm : Cell S (m) Before alignment Mar06 After alignment Apr06 Smoothing May06 17
18 β functions at the BPMs after LOCO application: comparison measured and theoretical values H Plan V Plan ~ 5 % differences further tuning needed 18
19 Betatron Coupling from Closest Tune Approach without any skew quadrupole correction Tunes ν min =0.003 Without coupling correction 2 κ 2 with =ν x -ν z -p (no vertical dispersion & single resonance approximation) υmin / = (2 + υ / min Guignard, CERN ) ν x = ν z = , p=8 κ = 0.08 % 19
20 Beam Emittance Measurements Source point in Dipole n # 2 cell # 2 Pinhole H : 25 µm V : 10 µm converter X Visible Visible Optics X optics CCD Measured Vertical Projection Camera with good linearity Image analysis by Gaussian fit and Deconvolutions Error bar on emittances : β value at source point : +/- 5 % possible beta beat Instrument parameters : a few 10-3 on H, a few 10-2 on V Vertical profile distortion remains to be understood Measured Horizontal Projection ε x = 3.9 nm.rad ± 0.25 ε z = 11 pm.rad ± 2 κ 0.3% (natural coupling) Design: ε x = GeV 20
21 Tune shifts with energy Good Agreement with model 0,5 0,45 0,4 nux measured nux calculated nuz measured nuz calculated DP/P > 0: loss on half Integer resonance (0.02 wide) DP/P < 0: loss on longitudinal beam dynamics α 1 = α 2 = ,35 0,3 0,25 0,2 0,15 0,1 0, DP/P (%) f RF f RF ) p/p (%) ξx = +3 ξz = +3 f rf = 8 khz 21
22 Vertical Acceptance Measured Ixτ vs. vertical position of scrapers (up and down) DOWN scraper UP scraper 200 ma UP scraper 11 ma Scraper is located in a long Straight section Measured ~ +/- 5mm. I x tau (ma x h) Simulations parameters: κ = 1% Zmin = ±5mm in medium straight sections 100 z (mm) Simulated Dynamic Aperture (long straight section) 22
23 Horizontal Acceptance Measured: - 15mm Deduced from turn by turn data kicking the beam with one injection kicker Confirmed by inserting the scrapers at septum equivalent position and kicking the beam with the same kicker Beam loss: Septum Position (-15mm) 23
24 Vibration measurements on SR girders Experimental Modal Analysis 1 st mode on quadrupole girder (transversal flexion) at 45 Hz! (design value 40 Hz) nd mode on quadrupole girder (vertical flexion) at 56 Hz
25 Typical noise spectrum BPM + Beam: 0 to 500 Hz Girder 47 Hz 50 Hz 47 Hz 50 Hz Noise < 2 microns Noise < 2 microns 25
26 Insertion devices commissioning HU m 2x HU80 2x U20 2x HU256 26
27 HU80-TEMPO Commissioning: Feed-Forward Forward Correction Test Horizontal BPM Data Minimal Gap (15.5 mm) Helical Mode (Phase = 20 mm) Vertical BPM Data 27
28 Multibunch Instabilities Mixture of resistive-wall (RW) and ion induced instabilities in both vertical & horizontal planes. No instability observed in the longitudinal plane. Instability threshold [ma] Signature of ions 3/4 filling 2/4 filling uniform filling Simulation 0 0,00 0,10 0,20 0,30 0,40 Instability threshold [ma] ions + RW 20 3/4 filling 10 ions uniform filling Vertical normalised chromaticity Horizontal normalised chromaticity - Behaviour of ion-induced instability depends much on the beam filling pattern. - Vertical threshold at low chromaticity in rather good agreement with prediction. - Horizontal threshold much lower than expected.(90 ma) - Single bunch current thresholds seem to be a factor 2 smaller than simulation 28
29 Dedicated superconducting RF cavities 0.1 phase stability 6 % RF acceptance No RF trip 1 st cryomodule will enable alone operation up to 300 ma. A 2 nd cryomodule is being built by ACCEL for operation at 500 ma (early 2008) 29
30 Storage Ring RF plant 4 x 190 kw power amplifiers Full Cost (with PS and WG distribution) Booster : 200 k for 40 kw => 5 / W Stor. Ring : 3 M for 750 kw => 4 / W Modularity = You just pay for the Watts you actually need MHz Gain = 52 db Overall Efficiency (PS,..) ~50% No RF trip even if transistor fails 30
31 Storage Ring Vacuum system Vacuum system for one typical cell Together with the Straight Section chambers, ~200 m of NEG coated Al chamber (56% of the ring) SOLEIL = first SR Machine with extensive use of NEG coated AL vessels 31
32 Vacuum Conditioning is well progressing 1,E-08 Non NEG coated stainless steel vacuum vessels 1,E-09 Pav / I (mbar/ma) 1,E-10 NEG coated vacuum vessels y = 2E-10x -0,602 y = 4E-10x -0,6021 Dec. 06 shutdown Crotch change at dipole 1 Beam lifetime : ma 1,E-11 0,10 1,00 10,00 100,00 Integrated Beam Dose (A.h) 32
33 Beam time by the end of 2006 Maximum current: 300 ma in 312/416 buckets Total beam integrated dose: 75 A.h 5% 11% Failures: water, PS, Beam time 84% Start-up, injection, tests, July / December 2006: 1400 hours 33
34 Time structure mode 20 ma in 1 bunch 80 ma in 8 bunches 148ns between 2 successive bunches 34
35 TANGO control system SOLEIL first facility using TANGO at full scale Collaboration ESRF/ELETTRA/SOLEIL/ALBA Easy and efficient tools to control any equipment Control of all equipments from the control room, data archiving Supervision done using GlobalSCREEN applications All hardware installed (Crate with CPCI and boards, PLC s..) Machine commissioning: Matlab applications (Matlab Middle Layer Toolkit, Accelerator Toolbox,...) 35
36 Beamline commissioning TEMPO 09/20/06 ~ 8 mm ODE 10/13/06 ~ 80 mm DIFFABS 09/13/06 SAMBA 12/13/06 DESIRS 12/14/06 36
37 Schedule for the first beamlines in 2007 DESIRS CRISTAL SAMBA TEMPO ODE AILES installation SWING commissioning expert users CASSIOPEE regular users PROXIMA1 installation commissioning expert users regular users DIFFABS SMIS 1/04/07 1/07/07 1/10/07 1/04/07 1/07/07 1/10/07 37
38 Planned Operation in runs of 3 or 4 weeks 3264 h for beamlines h for the machine. janv 2007 févr 2007 mars 2007 avr 2007 mai 2007 juin 2007 juil 2007 août 2007 sept 2007 oct 2007 nov 2007 déc 2007 janv 2008 lun jeu 01 l l l jeu dim mar 01 l l l ven 01 l l l dim 01 mmm mer sam 01 mmm lun jeu 01 l l l sam 01 l l l mar mar ven 02 l l l ven 02 mmm lun mer 02 l l l sam 02 l l l lun 02 mmm jeu dim 02 mmm mar ven 02 l l l dim 02 l l l mer mer sam 03 l l l sam 03 mmm mar jeu 03 l l l dim 03 mmm mar 03 l l l ven lun 03 mmm mer sam 03 l l l lun 03 l l l jeu jeu dim 04 mmm dim 04 mmm mer ven 04 l l l lun 04 mmm mer 04 l l l sam mar 04 l l l jeu dim 04 l l l mar 04 mmm ven ven lun 05 mmm lun 05 mmm jeu sam 05 l l l mar 05 l l l jeu 05 l l l dim mer 05 l l l ven lun 05 l l l mer 05 l l l sam sam mar 06 mmm mar 06 l l l ven dim 06 l l l mer 06 l l l ven 06 l l l lun jeu 06 l l l sam mar 06 mmm jeu 06 l l l dim dim mer 07 l l l mer 07 l l l sam lun 07 mmm jeu 07 l l l sam 07 l l l mar ven 07 l l l dim mer 07 l l l ven 07 l l l lun lun jeu 08 l l l jeu 08 l l l dim mar 08 mmm ven 08 l l l dim 08 mmm mer sam 08 l l l lun jeu 08 l l l sam 08 l l l mar mar ven 09 l l l ven 09 l l l lun mer 09 l l l sam 09 l l l lun 09 mmm jeu dim 09 l l l mar ven 09 l l l dim 09 l l l mer mer sam 10 l l l sam 10 l l l mar jeu 10 l l l dim 10 mmm mar 10 l l l ven lun 10 l l l mer sam 10 l l l lun 10 l l l jeu jeu dim 11 l l l dim 11 mmm mer ven 11 l l l lun 11 mmm mer 11 l l l sam mar 11 mmm jeu dim 11 l l l mar 11 mmm ven ven lun 12 mmm lun 12 mmm jeu sam 12 l l l mar 12 l l l jeu 12 l l l dim mer 12 l l l ven 12 mmm lun mer 12 l l l sam sam mar 13 mmm mar 13 l l l ven dim 13 l l l mer 13 l l l ven 13 l l l lun jeu 13 l l l sam 13 mmm mar jeu 13 l l l dim dim mer mer 14 l l l sam lun jeu 14 l l l sam 14 l l l mar ven 14 l l l dim 14 mmm mer ven 14 l l l lun lun jeu jeu 15 l l l dim mar ven 15 l l l dim 15 mmm mer sam 15 l l l lun 15 mmm jeu sam 15 l l l mar mar ven ven 16 l l l lun mer sam 16 l l l lun 16 mmm jeu dim 16 l l l mar 16 l l l ven dim 16 l l l mer mer sam sam 17 l l l mar jeu dim 17 l l l mar 17 l l l ven lun 17 l l l mer 17 l l l sam lun 17 l l l jeu jeu dim dim 18 mmm mer ven lun mer 18 l l l sam mar 18 mmm jeu 18 l l l dim mar ven ven 19 mmm lun lun 19 mmm jeu sam mar jeu 19 l l l dim mer 19 l l l ven 19 l l l lun mer sam sam 20 mmm mar mar 20 mmm ven 20 mmm dim mer ven 20 l l l lun jeu 20 l l l sam 20 l l l mar jeu dim dim 21 mmm mer mer 21 l l l sam 21 mmm lun jeu sam mar ven 21 l l l dim 21 l l l mer ven lun lun 22 mmm jeu jeu 22 l l l dim 22 mmm mar ven dim mer sam 22 l l l lun 22 l l l jeu sam mar mar 23 mmm ven ven 23 l l l lun 23 mmm mer sam lun jeu dim 23 l l l mar 23 mmm ven 23 mmm dim mer mer 24 l l l sam sam 24 l l l mar 24 l l l jeu dim mar ven lun mer 24 l l l sam 24 mmm lun jeu jeu 25 l l l dim dim 25 l l l mer 25 l l l ven 25 mmm lun mer sam mar jeu 25 l l l dim 25 mmm mar ven ven 26 l l l lun lun 26 mmm jeu 26 l l l sam 26 mmm mar jeu dim mer ven 26 l l l lun 26 mmm mer sam sam 27 l l l mar mar 27 mmm ven 27 l l l dim 27 mmm mer ven lun jeu sam 27 l l l mar 27 l l l jeu dim dim 28 mmm mer mer sam 28 l l l lun 28 mmm jeu sam mar ven dim 28 l l l mer 28 l l l ven lun lun 29 mmm jeu dim 29 mmm mar 29 l l l ven 29 mmm dim mer sam lun 29 l l l jeu 29 l l l sam mar mar 30 l l l ven lun 30 mmm mer 30 l l l sam 30 mmm lun jeu dim mar 30 mmm ven 30 l l l dim mer mer 31 l l l sam jeu 31 l l l mar ven 31 mmm mer 31 l l l lun jeu
39 Milestones in 2007 Beam stability SOFB/ FOFB/ multibunch transverse feedbacks Feedforward for IDs XBPM commissioning IDs Construction of 7 IDs (and installation & commissioning) Preparation for top-up operation Single bunch and 8 bunches operation Beam instabilities and high current operation Instabilities threshold Transverse feedback Nonlinear dynamics characterization Delivery of 2nd cryomodule for 500mA operation 39
40 The first phase of the Machine commissioning has enabled to demonstrate that the expected high performances are or will be met. Acknowledgements Operator team Magnetism and insertion group RF, Linac, Diagnostics groups Vacuum group Alignment group Mechanical and Engineering group Electronics and Computer groups Infrastructure group Safety group Beam Lines 40
SOLEIL Current Performances. And. Futur Developments
SOLEIL Current Performances And Futur Developments Amor Nadji On Behalf of the SOLEIL Team A. Nadji, ESLSXVIII, Trieste, November 25-26 2010 1 Main Parameters Energy (GeV) 2.75 Emittance H (nm.rad) 3.7
Damping Wigglers in PETRA III
Damping Wigglers in PETRA III WIGGLE2005, Frascati 21-22.2.2005 Winni Decking, DESY-MPY Introduction Damping Wiggler Parameters Nonlinear Dynamics with DW Operational Aspects Summary DESY and its Accelerators
Frequency Map Experiments at the Advanced Light Source. David Robin Advanced Light Source
Frequency Map Experiments at the Advanced Light Source David Robin Advanced Light Source work done in collaboration with Christoph Steier (ALS), Ying Wu (Duke), Weishi Wan (ALS), Winfried Decking (DESY),
Status Overview The Australian Synchrotron. Steven Banks Control Systems Group
Status Overview The Australian Synchrotron Steven Banks Control Systems Group Where Are We? Where Are We? Where Are We? The Building Development being managed by Major Projects Victoria (MPV) Budget is
Maintenance & reliability management. H. Rozelot - Workshop Maintenance & Reliability SOLEIL- November 9 & 10
Maintenance & reliability management SYNCHROTRON SOLEIL A light source to explore matter H. Rozelot XFEL November 3rd 2010 Located 25km from Paris 357 permanent people Some dates : Building Construction
Results: Low current (2 10 12 ) Worst case: 800 MHz, 12 50 GeV, 4 turns Energy oscillation amplitude 154 MeV, where
Status Focus has shifted to a neutrino factory Two comprehensive designs of acceleration (liancs, arcs) Jefferson Lab, for Fermilab Study CERN (Keil et al.) Jefferson Lab study Low (2 10 12 ) charge per
Figure 1: Lattice drawing for the APS storage ring.
PERFORMANCE OF THE ADVANCED PHOTON SOURCE Glenn Decker Advanced Photon Source, Argonne National Laboratory 9700 South Cass Avenue, Argonne, Illinois 60439 USA Abstract The Advanced Photon Source (APS)
Status of Radiation Safety System at
Status of Radiation Safety System at Taiwan Photon Source Joseph C. Liu Radiation and Operation Safety Division National Synchrotron Radiation Research Center, Taiwan NSRRC layout 1.5 GeV, 120m, 400 ma
BEPC UPGRADES AND TAU-CHARM FACTORY DESIGN
BEPC UPGRADES AND TAU-CHARM FACTORY DESIGN Abstract BEPC Group, presented by Yingzhi Wu Institute of High Energy Physics, Beijing 100039, P.R. China The luminosity upgrades of the BEPC are briefly reviewed.
Shielding and Radiation Measurements at ESRF
Shielding and Radiation Measurements at ESRF Radiation Safety Meeting SOLEIL Synchrotron, 18 October 26 P. Berkvens European Synchrotron Radiation Facility Radiation protection policy at the ESRF Storage
Tune and Chromaticity Tracking in the Tevatron. C.Y. Tan 09 May 2006
Tune and Chromaticity Tracking in the Tevatron C.Y. Tan 09 May 2006 Overview What is the Tevatron tune tracker? Selected results from some stores. (There are many stores with TT running). Planned chromaticity
THE ALIGNMENT STRATEGY FOR THE SPIRAL2 SUPERCONDUCTING LINAC CRYOMODULES
THE ALIGNMENT STRATEGY FOR THE SPIRAL2 SUPERCONDUCTING LINAC CRYOMODULES R. Beunard, GANIL, BP 55027, 14076 CAEN, CEDEX 5, France Abstract The SPIRAL2* project, located at the GANIL** facility in Caen,
Status of the HOM Damped Cavity for the Willy Wien Ring
Status of the HOM Damped Cavity for the Willy Wien Ring Ernst Weihreter / BESSY Short Review of HOM Damped Cavity Prototype Modifications for the Willy Wien Ring Cavity Results of Low Power Measurements
Towards large dynamic range beam diagnostics and beam dynamics studies. Pavel Evtushenko
Towards large dynamic range beam diagnostics and beam dynamics studies Pavel Evtushenko Motivation Linacs with average current 1-2 ma and energy 1-2.5 GeV are envisioned as drivers for next generation
Development of Virtual Accelerator Environment for Beam Diagnostics *
Development of Virtual Accelerator Environment for Beam Diagnostics * Gu Duan, Zhang Meng, Gu Qiang, Huang Dazhang, Zhao Minghua (Shanghai Institute of Applied Physics, Chinese Academy of Sciences, Shanghai
The BESSY HOM Damped Cavity with Ferrite Absorbers. Review of prototype cavity test results, taperedwaveguidesvshomogenouswaveguides
The BESSY HOM Damped Cavity with Ferrite Absorbers E. Weihreter / BESSY Review of prototype cavity test results, taperedwaveguidesvshomogenouswaveguides Design of a ferrite loaded ridged circular waveguide
HIGH-ENERGY COLLIDER PARAMETERS: e + e Colliders (I)
28. High-energy collider parameters 1 HIGH-ENERGY COLLIDER PARAMETERS: e + e Colliders (I) Updated in early 2012 with numbers received from representatives of the colliders (contact J. Beringer, LBNL).
Zero Degree Extraction using an Electrostatic Separator
Zero Degree Extraction using an Electrostatic Separator L. Keller Aug. 2005 Take another look at using an electrostatic separator and a weak dipole to allow a zero degree crossing angle a la the TESLA
LHC optics measurement & correction procedures. M. Aiba, R. Calaga, A. Morita, R. Tomás & G. Vanbavinckhove
LHC optics measurement & correction procedures M. Aiba, R. Calaga, A. Morita, R. Tomás & G. Vanbavinckhove Thanks to: I. Agapov, M. Bai, A. Franchi, M. Giovannozzi, V. Kain, G. Kruk, J. Netzel, S. Redaelli,
Libera at ELETTRA: prehistory, history and present state
Libera at ELETTRA: prehistory, history and present state S. Cleva, S. Bassanese, R. De Monte, G. Gaio, M. Lonza, C. Scafuri Elettra - Sincrotrone Trieste 1 ELETTRA and FERMI@Elettra plants ELETTRA (SR):
SIMULATIONS OF ELECTRON CLOUD BUILD-UP AND SATURATION IN THE APS *
SIMULATIONS OF ELECTRON CLOUD BUILD-UP AND SATURATION IN THE APS * K. C. Harkay and R. A. Rosenberg, ANL, Argonne, IL 60439, USA M. A. Furman and M. Pivi, LBNL, Berkeley, CA 94720, USA Abstract In studies
Industrial Involvement in the Construction of Synchrotron Light Sources
Industrial Involvement in the Construction of Synchrotron Light Sources M.S. de Jong, Canadian Light Source Inc. European Particle Accelerator Conference 2004-07-07 Introduction Large demand for synchrotron
Reliability and Availability Aspects of. the IPHI Project
Reliability and Availability Aspects of the IPHI Project Pierre-Yves Beauvais CEA/DSM/DAPNIA for the IPHI Team 18/02/2002 Pierre-Yves Beauvais, CEA Saclay 1 Table of contents Brief description of IPHI
The half cell of the storage ring SESAME looks like: Magnetic length =
6. Magnets 6.1 Introduction SESAME will be perhaps erected in steps. The number of steps depends upon the available money. The cheapest way is to use the quadrupole and sextupoles from BESSY I. In this
Design and development of Configurable BPM readout system for ILSF
Abstract Design and development of Configurable BPM readout system for ILSF M. Shafiee 1,2, J.Rahighi, M.Jafarzadeh, 1 ILSF, Tehran, Iran A.H.Feghhi, 2 Shahid beheshti University, Tehran, Iran A configurable
OVERVIEW OF PROTON DRIVERS FOR NEUTRINO SUPER BEAMS AND NEUTRINO FACTORIES*
FERMILAB-CONF-06-213-AD OVERVIEW OF PROTON DRIVERS FOR NEUTRINO SUPER BEAMS AND NEUTRINO FACTORIES* W. Chou #, Fermilab, Batavia, IL 60510, U.S.A. Abstract There has been a world-wide interest in Proton
THE TAIWAN LIGHT SOURCE AND SUPERCONDUCTING CAVITY
THE TAIWAN LIGHT SOURCE AND SUPERCONDUCTING CAVITY G.H. Luo, Ch. Wang, L.H. Chang, M.C. Lin, T.T. Yang and C.T. Chen SRRC, No. 1 R&D Road VI, HSIP, Hsinchu, Taiwan Abstract The Taiwan Light Source (TLS)
Beam Dynamics Studies and Design Optimisation of New Low Energy Antiproton Facilities arxiv:1606.06697v1 [physics.acc-ph] 21 Jun 2016
Beam Dynamics Studies and Design Optimisation of New Low Energy Antiproton Facilities arxiv:606.06697v [physics.acc-ph] 2 Jun 206 Javier Resta-Lopez, James R. Hunt, Carsten P. Welsch Department of Physics,
Undulators and wigglers for the new generation of synchrotron sources
Undulators and wigglers for the new generation of synchrotron sources P. Elleaume To cite this version: P. Elleaume. Undulators and wigglers for the new generation of synchrotron sources. Journal de Physique
Institute of Accelerator Technologies of Ankara University and TARLA Facility
Institute of Accelerator Technologies of Ankara University and TARLA Facility Avni Aksoy Ankara University [email protected] On behalf of IAT & TARLA Team Contents Brief history of TAC project Institute
10 Project Costs and Schedule
II-367 10 Project Costs and Schedule 10.1 Overview The investment costs given in this chapter include all components necessary for the baseline design of TESLA, as described in chapters 3 to 9. Not included
AUTOMATION OF OPERATIONS ON THE VEPP-4 CONTROL SYSTEM
10th ICALEPCS Int. Conf. on Accelerator & Large Expt. Physics Control Systems. Geneva, 10-14 Oct 2005, PO1.072-7 (2005) AUTOMATION OF OPERATIONS ON THE VEPP-4 CONTROL SYSTEM A. Bogomyagkov, S. Karnaev,
ULTRAFAST LASERS: Free electron lasers thrive from synergy with ultrafast laser systems
Page 1 of 6 ULTRAFAST LASERS: Free electron lasers thrive from synergy with ultrafast laser systems Free electron lasers support unique time-resolved experiments over a wide range of x-ray wavelengths,
Status of the FERMI@Elettra Free Electron Laser
Status of the FERMI@Elettra Free Electron Laser E. Allaria on behalf of the FERMI team Work partially supported by the Italian Ministry of University and Research under grants FIRB-RBAP045JF2 and FIRB-RBAP06AWK3
Status of High Current Ion Sources. Daniela Leitner Lawrence Berkeley National Laboratory
http://ecrgroup.lbl.gov Status of High Current Ion Sources Daniela Leitner Lawrence Berkeley National Laboratory October, 27th, 2003 1 Content Overview of available high current sources Requirements for
Insertion Devices Lecture 4 Permanent Magnet Undulators. Jim Clarke ASTeC Daresbury Laboratory
Insertion Devices Lecture 4 Permanent Magnet Undulators Jim Clarke ASTeC Daresbury Laboratory Introduction to Lecture 4 So far we have discussed at length what the properties of SR are, when it is generated,
A Quick primer on synchrotron radiation: How would an MBA source change my x-ray beam. Jonathan Lang Advanced Photon Source
A Quick primer on synchrotron radiation: How would an MBA source change my x-ray beam Jonathan Lang Advanced Photon Source APS Upgrade - MBA Lattice ε ο = 3100 pm ε ο = 80 pm What is emi7ance? I don t
Activities at the University of Frankfurt (IAP)
Activities at the University of Frankfurt (IAP) Holger Podlech Ulrich Ratzinger Oliver Kester Institut für Angewandte Physik (IAP) Goethe-Universität Frankfurt am Main H. Podlech 1 Development of 325 MHz
Development of High Stability Supports for NSLS-II RF BPMS
BNL-82316-2009-CP Development of High Stability Supports for NSLS-II RF BPMS B. Kosciuk, R. Alforque, B. Bacha, P. Cameron, F. Lincoln, V. Ravindranath, I. Pinayev, S. Sharma, O. Singh Brookhaven National
Status of the Diamond Storage Ring RF Systems. Morten Jensen on behalf of Diamond Storage Ring RF Group
Status of the Diamond Storage Ring RF Systems Morten Jensen on behalf of Diamond Storage Ring RF Group Content 1. General Operational Status 2. Main issues and causes of trips 3. 200 ma + operation Qext
Running in 2011 - Luminosity. Mike Lamont Verena Kain
Running in 2011 - Luminosity Mike Lamont Verena Kain Presentations Many thanks to all the speakers! Experiments expectations Massi Ferro-Luzzi Pushing the limits: beam Elias Métral Pushing the limits:
Beam Instrumentation Group, CERN ACAS, Australian Collaboration for Accelerator Science 3. School of Physics, University of Melbourne 4
Prototype tests of a wide-band Synchrotron-Light based Beam Pattern Monitor for measuring charge-couple bunch instabilities in High-Energy Particle Accelerator Beams Sophie Dawson2,3, Mark Boland2,4, David
K O M A C. Beam Commissioning of 100-MeV KOMAC Linac. Korea Multi-purpose Accelerator Complex 양 성 자 가 속 기 연 구 센 터
LINAC14, Geneva Beam Commissioning of 100-MeV KOMAC Linac Yong-Sub Cho for KOMAC accelerator team September 2, 2014 KOMAC, KAERI 0 Outline KOrea Multi-purpose Accelerator Complex Facility Introduction
Brookhaven Magnet Division - Nuclear Physics Program Support Activities
Brookhaven - Nuclear Physics Program Support Activities Spin Program support E-Cooling R&D RIA RHIC Operations Support Funding AGS Warm Siberian Snake AGS Warm Snake Magnetic element designed and built
Coupling Impedance of SIS18 and SIS100 beampipe CERN-GSI-Webmeeting
Coupling Impedance of SIS18 and SIS100 beampipe CERN-GSI-Webmeeting 23 October 2011 TU Darmstadt Fachbereich 18 Institut Theorie Elektromagnetischer Felder Uwe Niedermayer 1 Contents Motivation / Overview
FACET First Beam Commissioning. Jerry Yocky For the FACET commissioning team 21-May-2012 IPAC 2012, New Orleans, LA
FACET First Beam Commissioning Jerry Yocky For the FACET commissioning team 21-May-2012 IPAC 2012, New Orleans, LA Facility for Advanced accelerator Experimental Tests WHAT IS FACET? The FACET Facility
HIGH CURRENT OPERATION OF THE ACSI TR30 CYCLOTRON
HIGH CURRENT OPERATION OF THE ACSI TR30 CYCLOTRON 18 th International Conference on Cyclotrons and their Applications, Sicily, 2007 Vasile Sabaiduc, Project Manager, RF Senior Engineer Advanced Cyclotron
Tom Wilson Product Marketing Manager Delivery Systems Varian Medical Systems International AG. CERN Accelerator School, May 2015
INDUSTRIAL DESIGN Tom Wilson Product Marketing Manager Delivery Systems Varian Medical Systems International AG VARIAN ONCOLOGY SYSTEMS 1 VARIAN ONCOLOGY SYSTEMS CERN Accelerator, May 2015 Industrial Design
RF SYSTEM FOR VEPP-5 DAMPING RING
Ó³ Ÿ. 2006.. 3, º 7(136).. 60Ä64 Š 621.384.634.14 RF SYSTEM FOR VEPP-5 DAMPING RING Ye. Gusev, N. Kot, S. Krutikhin, I. Kuptsov, G. Kurkin, I. Makarov, N. Matyash, L. Mironenko, S. Motygin, V. Osipov,
Correlation between OATS, Fully Anechoic Room and GTEM Radiated Emissions
Correlation between OATS, Fully Anechoic Room and GTEM Radiated Emissions Stephen Clay Introduction: Just a few words about myself. My name is Steve Clay and I work for Nokia Mobile Phones, and it is my
Solutions Manufacturing Performance
Solutions Manufacturing Performance Let s partner up for your project At RI Research Instruments we develop, design, manufacture and test high performance components and systems to the needs of our customers
TS321 Low Power Single Operational Amplifier
SOT-25 Pin Definition: 1. Input + 2. Ground 3. Input - 4. Output 5. Vcc General Description The TS321 brings performance and economy to low power systems. With high unity gain frequency and a guaranteed
MEMS mirror for low cost laser scanners. Ulrich Hofmann
MEMS mirror for low cost laser scanners Ulrich Hofmann Outline Introduction Optical concept of the LIDAR laser scanner MEMS mirror requirements MEMS mirror concept, simulation and design fabrication process
LLRF. Digital RF Stabilization System
LLRF Digital RF Stabilization System Many instruments. Many people. Working together. Stability means knowing your machine has innovative solutions. For users, stability means a machine achieving its full
Short overview of TEUFEL-project
Short overview of TEUFEL-project ELAN-meeting may 2004 Frascati (I) Contents Overview of TEUFEL project at Twente Photo cathode research Recent experience Outlook Overview FEL Drive laser Photo cathode
Slice Emittance Measurements at the SLAC Gun Test Facility*
SLAC-PUB-954 September Slice Emittance Measurements at the SLAC Gun Test Facility* D. H. Dowell, P. R. Bolton, J.E. Clendenin, P. Emma, S.M. Gierman, C.G. Limborg, B.F. Murphy, J.F. Schmerge Stanford Linear
Information about the T9 beam line and experimental facilities
Information about the T9 beam line and experimental facilities The incoming proton beam from the PS accelerator impinges on the North target and thus produces the particles for the T9 beam line. The collisions
The design and performance of Static Var Compensators for particle accelerators
CERN-ACC-2015-0104 [email protected] The design and performance of Static Var Compensators for particle accelerators Karsten Kahle, Francisco R. Blánquez, Charles-Mathieu Genton CERN, Geneva, Switzerland,
NUCLEAR MAGNETIC RESONANCE. Advanced Laboratory, Physics 407, University of Wisconsin Madison, Wisconsin 53706
(revised 4/21/03) NUCLEAR MAGNETIC RESONANCE Advanced Laboratory, Physics 407, University of Wisconsin Madison, Wisconsin 53706 Abstract This experiment studies the Nuclear Magnetic Resonance of protons
LHC MACHINE PROTECTION
LHC MACHINE PROTECTION Rossano Giachino, CERN, Geneva, Switzerland Abstract The energy stored in LHC magnets presents a considerable challenge for commissioning even before any beam is injected. Furthermore,
MASW-000823-12770T. HMIC TM PIN Diode SP2T 13 Watt Switch for TD-SCDMA Applications. Features. Functional Diagram (TOP VIEW)
Features Exceptional Loss = 0.35 db Avg @ 2025 MHz, 20mA Exceptional Loss = 0.50 db Avg @ 2025 MHz, 20mA Higher - Isolation = 31dB Avg @ 2025 MHz, 20mA Higher RF C.W. Input Power =13 W C.W.(-Ant Port)
Relativistic kinematics basic energy, mass and momentum units, Lorents force, track bending, sagitta. First accelerator: cathode ray tube
Accelerators Relativistic kinematics basic energy, mass and momentum units, Lorents force, track bending, sagitta Basic static acceleration: First accelerator: cathode ray tube Cathode C consist of a filament,
SpectraTec II. Polarized Multi-Laser Source BLUE SKY RESEARCH WAVELENGTHS. The SpectraTec II
BLUE SKY RESEARCH The SpectraTec II, two wavelength laser module is a highly integrated system comprised of two lasers, individual driving and temperature control electronics, wavelength combining, and
Spin Tracking with COSY INFINITY and its Benchmarking
Spin Tracking with COSY INFINITY and its Benchmarking 2015-05-05 Marcel Rosenthal for the JEDI collaboration Outline Methods Simulation toolbox New extension: Transfer maps for time-varying fields Application
MYRRHA Injector Design
MYRRHA Injector Design Horst Klein Dominik Mäder, Holger Podlech, Ulrich Ratzinger, Alwin Schempp, Rudolf Tiede, Markus Vossberg, Chuan Zhang Institute for Applied Physics, Goethe-University Frankfurt
Systems, Inc. Energy Advanced
Systems, Inc. nergy Advanced ADVAND NRGY SYSTMS, IN Our Mission To be the supplier of choice for advanced radiation sources, high brightness commercial accelerator applications, government accelerator
DEVELOPMENT OF THE SWISSFEL UNDULATOR BPM SYSTEM
Proceedings of BC2014, Monterey, CA, USA DEVELOPMENT OF THE SWSSFEL UNDULATOR BPM SYSTEM M. Stadler #, R. Baldinger, R. Ditter, B. Keil, F. Marcellini, G. Marinkovic, M. Roggli, M. Rohrer PS, Villigen,
A new extraction system for the upgraded AIC-144 cyclotron
NUKLEONIKA 2001;46(2):51 57 ORIGINAL PAPER A new extraction system for the upgraded AIC-144 cyclotron Edmund Bakewicz, Krzysztof Daniel, Henryk Doruch, Jacek Sulikowski, Ryszard Taraszkiewicz, Nikolaj
CLS Naming and Numbering Convention
CLS Naming and Numbering Convention 0.2.1.1 Rev. 6 Date: 2015-Dec-03 Copyright 2015, Canadian Light Source Inc. This document is the property of Canadian Light Source Inc. (CLSI). No exploitation or transfer
14.5GHZ 2.2KW CW GENERATOR. GKP 22KP 14.5GHz WR62 3x400V
14.5GHZ 2.2KW CW GENERATOR GKP 22KP 14.5GHz WR62 3x400V UTILIZATION OF GKP 22KP GENERATOR With its characteristics of power stability whatever the load, very fast response time at a pulse, low ripple,
PowerAmp Design. PowerAmp Design PAD135 COMPACT HIGH VOLATGE OP AMP
PowerAmp Design COMPACT HIGH VOLTAGE OP AMP Rev G KEY FEATURES LOW COST SMALL SIZE 40mm SQUARE HIGH VOLTAGE 200 VOLTS HIGH OUTPUT CURRENT 10A PEAK 40 WATT DISSIPATION CAPABILITY 200V/µS SLEW RATE APPLICATIONS
BEAM OPERATION OF THE PAL-XFEL INJECTOR TEST FACILITY
Proceedings of FEL2014, Basel, Switzerland WEB02 BEAM OPERATION OF THE PAL-XFEL INJECTOR TEST FACILITY J.-H. Han, J. Hong, J. H. Lee, M. S. Chae, S. Y. Baek, H. J. Choi, T. Ha, J. Hu, W. H. Hwang, S. H.
The accurate calibration of all detectors is crucial for the subsequent data
Chapter 4 Calibration The accurate calibration of all detectors is crucial for the subsequent data analysis. The stability of the gain and offset for energy and time calibration of all detectors involved
Solar Energy. Outline. Solar radiation. What is light?-- Electromagnetic Radiation. Light - Electromagnetic wave spectrum. Electromagnetic Radiation
Outline MAE 493R/593V- Renewable Energy Devices Solar Energy Electromagnetic wave Solar spectrum Solar global radiation Solar thermal energy Solar thermal collectors Solar thermal power plants Photovoltaics
Energy Deposition in MICE Absorbers and Coils
in MICE Absorbers and Coils November 2, 2003 Video Conference Page 1 An Application for G4Mice We would like to estimate how much energy is deposited in magnet coils and the hydrogen absorber. Most of
THE TESLA TEST FACILITY AS A PROTOTYPE FOR THE GLOBAL ACCELERATOR NETWORK
THE TESLA TEST FACILITY AS A PROTOTYPE FOR THE GLOBAL ACCELERATOR NETWORK K. Rehlich, DESY, Hamburg, Germany Abstract The next generation of large accelerators facilities will be produced and operated
Mission: Cure, Research and Teaching. Marco Pullia Cnao design and commissioning
CNAO design and commissioning Marco Pullia, CNAO Foundation What is the CNAO Foundation No profit organisation (Foundation) created with the financial law 2001 to build the national center for hadrontherapy
C.-K. Ng. Stanford Linear Accelerator Center. and. T. Weiland. University oftechnology. FB18, Schlossgartenstr. 8. D64289, Darmstadt, Germany.
SLAC-PUB-95-7005 September, 1995 Impedance of the PEP-II DIP Screen C.-K. Ng Stanford Linear Accelerator Center Stanford University, Stanford, CA 94309, USA and T. Weiland University oftechnology FB18,
Calorimetry in particle physics experiments
Calorimetry in particle physics experiments Unit n. 8 Calibration techniques Roberta Arcidiacono Lecture overview Introduction Hardware Calibration Test Beam Calibration In-situ Calibration (EM calorimeters)
The IR FEL at the Fritz Haber Institute Berlin: A Tool for IR Spectroscopy of Molecules, Clusters, and Solids
The IR FEL at the Fritz Haber Institute Berlin: A Tool for IR Spectroscopy of Molecules, Clusters, and Solids Wieland Schöllkopf Fritz-Haber-Institut der Max-Planck-Gesellschaft, Berlin Outline 1. Design
Study of electron cloud at MI and slip stacking process simulation
Study of electron cloud at MI and slip stacking process simulation Alexandr S. Valkovich Purpose 1.Understand the slip stacking process which happens in the Main Injector. 2. Calculation of bunch distortion
Development and Experimental Performance Evaluation of a Dose-Rate meter for Pulsed Beam.
5 th International Workshop on Radiation Safety at Synchrotron Radiation Sources Development and Experimental Performance Evaluation of a Dose-Rate meter for Pulsed Beam. A. Vascotto 1, K. Casarin 1, S.
Introduction. Magnet Coordinate System
283 Fiducialization Procedures for the ALS Ring Magnets and the Booster Synchrotron Girders Jack Tanabe, Roderich Keller and Ted Lauritzen Lawrence Berkeley Laboratory, Berkeley, CA 94720, U. S. A. Introduction
Self-Mixing Laser Diode Vibrometer with Wide Dynamic Range
Self-Mixing Laser Diode Vibrometer with Wide Dynamic Range G. Giuliani,, S. Donati, L. Monti -, Italy Outline Conventional Laser vibrometry (LDV) Self-mixing interferometry Self-mixing vibrometer Principle:
9000 Series Accelerometers Specifications
Technical Data 9000 Series Accelerometers Specifications Catalog Numbers EK-43781I, EK-43782I, EK-46255I, EK-45890I, EK-43784I, EK-47086I, EK-43792I, EK-47090I, EK-43799I, EK-43794I, EK-43795I, EK-43797I,
Lecture VI Magnetic Design
Lecture VI Magnetic Design Field Quality Adjustment After Construction (or After the Start of Production Run) Ramesh Gupta Superconducting Brookhaven National Laboratory US Particle Accelerator School
Investigations on Critical Higher Order Modes in CEBAF Upgrade Cavities
Investigations on Critical Higher Order Modes in CEBAF Upgrade Cavities F. Marhauser Thanks also to H. Wang and K. Tian 27. August 2009 How HOMs are excited and why they are important - Wakefields- some
Undulators at PETRA: Experience and Perspectives
Undulators at PETRA: Experience and Perspectives Markus Tischer for the Insertion Devices Group at DESY 3-Way Meeting, Argonne, Aug 1 st - 2 nd 2013 Outline > PETRA III IDs > Commissioning experience >
3 Main Linac. 3.1 Introduction. 3.2 Beam Dynamics II-63
II-63 3 Main Linac 3.1 Introduction In this chapter, we describe the layout and the properties of the main linacs, in which the electron and positron beams are accelerated from 5 to 250 GeV at a gradient
FCC 1309180800 JGU WBS_v0034.xlsm
1 Accelerators 1.1 Hadron injectors 1.1.1 Overall design parameters 1.1.1.1 Performance and gap of existing injector chain 1.1.1.2 Performance and gap of existing injector chain 1.1.1.3 Baseline parameters
A Guide to Acousto-Optic Modulators
A Guide to Acousto-Optic Modulators D. J. McCarron December 7, 2007 1 Introduction Acousto-optic modulators (AOMs) are useful devices which allow the frequency, intensity and direction of a laser beam
