Operational experience with LHC circulating beams

Size: px
Start display at page:

Download "Operational experience with LHC circulating beams"

Transcription

1 LHC Performance Workshop - Chamonix 2009 Centre de Congrès Le Majestic, Chamonix, France 2 nd -6 th February 2008 Operational experience with LHC circulating beams Stefano Redaelli - BE/OP

2 Acknowledgments Commissioning was possible thanks to the work of MANY people: O. Aberle, I. Agapov, M. Aiba, M. Albert, R. Alemany Fernandez, G. Arduini, R. Assmann, V. Baggiolini, R. Bailey, E. Benedetto, R. Billen, L. Bottura, O. Brüning, A. Butterworth, R. Calaga, E. Carlier, P. Collier, B. Dehning, L. Deniau, S. Fartoukh, F. Follin, D. Forkel- Wirth, K. Fuchsberger, R. Giachino, M. Giovannozzi, B. Goddard, J-J. Gras, E. Hatziangeli, P. Hagen, D. Jacquet, L. Jensen, R. Jones, V. Kain, I. Kozsar, T. Kramer, G. Kruk, M. Lamont, J. Lewis, R. Losito, A. Macpherson, A. Masi, M. Meddahi, V. Mertens, M. Misiowiec, S. Page, L. Ponce, B. Puccio, S. Redaelli, C. Roderick, S. Roesler, F. Roncarolo, M. Sapinski, F. Schmidt, R. Schmidt, W. Sliwinski, R. Steinhagen, M. Strzelczyk, Y. Sun, B. Todd, E. Todesco, R. Tomas Garcia, J. Uythoven, W. Venturini Delsolaro, Heinz Vincke, Helmut Vincke, E. Veyrunes, J. Wenninger, R. Wolf, C. Zamantzas, F. Zimmermann. Acknowledge the excellent performance of the LHC injector complex and the shift crews during the days when we needed LHC beams! Also LHC shift crew! Special acknowledgments: T. Bohl, M. Lamont, R. Steinhagen, R. Tomàs, J. Wenninger Additional fruitful discussions with: G. Arduini, A. Butterworth, E. Ciapala, S. Fartouhk, R. Jones, M. Giovannozzi, W. Venturini 2

3 Milestones of 60 hours of LHC beam First turn! 10:26 TDI-B2 out 13:34 TDI-B1 out 09:35 First turn! 14:59 Beam captured! Circulating>15min Circulating beam: 300+ turns First tune meas. Mountain range Detailed measurements Long. bunch profile Optics response measurements 6 4 Vertical [ mm ] Beta-beat measur. Extracted Beam 2 [1010p] Extracted Beam 1 [1010p] Tune meter YASP: acquisition & threading 10/09 07:00 11/09 00: Longitudinal coordinate [ km ] Fast-BCT 12/09 00:00 Beam profile from Wire Scanner 3

4 Dipole powering history 757 Current in RB circuits [A] Beam current [10 10 p] Injection currents Magnet re-cycling See talk by L. Bottura in this Session 4

5 Outline Introduction Milestones of 60 hours of LHC beam Powering history Operation of accelerator systems Threading: BPM / BLM / screens Multi-turn commissioning, first tune RF capture Additional BI Overall machine performance Orbit, tune, chromaticity, optics Comparisons with design values Conclusions 5

6 First turn (1) - Beam1 on TDI Collimators in all points were used to stop the beam: - optimize beam trajectory before going into next sector; - improve the show! IP2 IP3 IP4 IP5 IP6 IP7 IP8 IP1 Beam losses [ gy/s ] :33:43 TDI.4L Longitudinal position [ km ] 6

7 First turn (2) - Beam1 to IP3 IP2 IP3 IP4 IP5 IP6 IP7 IP8 IP1 Beam losses [ gy/s ] :40:43 TCLA.A5R3.B Longitudinal position [ km ] Horizontal trajectory Vertical trajectory 7

8 First turn (3) - beam to CMS IP2 IP3 IP4 IP5 IP6 IP7 IP8 IP1 Beam losses [ gy/s ] :47:43 TCTH.4L5.B Longitudinal position [ km ] Horizontal trajectory Vertical trajectory 8

9 First turn (3) - beam to CMS IP2 IP3 IP4 IP5 IP6 IP7 IP8 IP1 Beam losses [ gy/s ] :47:43 TCTH.4L5.B Longitudinal position [ km ] Horizontal trajectory Vertical trajectory Courtesy of CMS team 9

10 First turn (4) - Beam 1 to the dump IP2 IP3 IP4 IP5 IP6 IP7 IP8 IP1 Beam losses [ gy/s ] :57:31 TCSG.4R6.B Longitudinal position [ km ] Horizontal trajectory Vertical trajectory 10

11 First turn (5) - Beam1 to IR7 IP2 IP3 IP4 IP5 IP6 IP7 IP8 IP1 Beam losses [ gy/s ] :08:43 TCLA.D6R7.B Longitudinal position [ km ] Horizontal trajectory Vertical trajectory 11

12 First turn (6) - Beam1 to IR8 IP2 IP3 IP4 IP5 IP6 IP7 IP8 IP1 Beam losses [ gy/s ] :12:13 TCTH.4L8.B Longitudinal position [ km ] Horizontal trajectory Vertical trajectory 12

13 First turn (7) - Beam 1 to ATLAS IP2 IP3 IP4 IP5 IP6 IP7 IP8 IP1 Beam losses [ gy/s ] :19:55 TCTH.4L1.B Longitudinal position [ km ] Horizontal trajectory Vertical trajectory 13

14 First turn (7) - Beam 1 to ATLAS IP2 IP3 IP4 IP5 IP6 IP7 IP8 IP1 Beam losses [ gy/s ] :19:55 TCTH.4L1.B Longitudinal position [ km ] Horizontal trajectory Vertical trajectory Courtesy of T. Wengler for the ATLAS team 14

15 Closure of first turn for beam 1 IP2 IP3 IP4 IP5 IP6 IP7 IP8 IP1 Beam losses [ gy/s ] :26: Longitudinal position [ km ] Horizontal trajectory Vertical trajectory 15

16 Screens, first optics checks Al screen Ti screen Screen team + F. Follin Compare H/V beam size with measured beam sizes: β x Nominal optics : = β y 25.5 = 2.7 Beam size meas. : 2 σ x σ y = 2.5 ɛ x ɛ y Amplitude [a.u.] BTV data 1st turn 2nd turn 3rd turn Fitted H size No much more on B1 commissioning x [ mm ] 16

17 Beam loss monitoring Acquisition of all ~4000 monitors available from day-1, all 12 integrations. Used extensively during all sector tests and circulating beam commissioning! Minor list of improvements of application BLM team + F. Follin 17

18 Multi-turns and first tune 300+ turns established in the evening of Sep. 10 th Tune was initially on the 0.5 resonance: crucial commissioned of tune meas. (BBQ) at the same time! Then, tune and chromaticity to improve lifetime Found a wrong tune knob (V) RF team... First tune measurements: R. Steinhagen + BI BBQ team 18

19 RF capture RF OFF RF ON phase RF ON wrong phase and frequency ok: beam captured! RF ON wrong freq. Courtesy of Ed Ciapala for the RF team VERY first beam circulating in the LHC for several minutes (Sep. 11 th ) Beam captured in the night of Sep. 11 th. Right after, we the beam circulated for more than 10 minutes! Commissioning driven by RF team from SR4. From CCC could only watch the longitudinal profile monitor! No particular issues were found. But we need to improve the diagnostic from the CCC. 19

20 Extraction - first emergency dump From the logbook of Thu., Sep. 11 th First captured beam that circulated for more than 10 minutes also experienced the first real emergency dump (Sep. 11 th at 22:45) Initial commissioning of system and relevant operational modes for this phase (Inject&Dump; Circulate&Dump) were achieved. The system performed very well. Dedicated talk in this session by B. Goddard - no further details here. 20

21 Additional BI: First wire scanner profile ! x = 1.67 mm σx = 2.36mm Horizontal profile Signal amplitude [a.u.] X position [ mm ] ! y = 1.68 σy = 2.38mm Vertical profile BI team + E. McCroy (LAFS) Acquisition working on Sep. 12th!! Calculated beam sizes seem compatible with the as-measured the local beta functions! Need more commissioning time... Signal amplitude [a.u.] Y position [ mm ] Data saved by S. Gilardoni 21

22 On-line β-beat measurements R. Tomàs et al. First estimated of β-beat based of 90-turn acquisition by YASP (injection oscillations), available in CCC of Fri. Sep. 12th. Better estimates available from off-line analysis. 22

23 Outline Introduction Milestones of 60 hours of LHC beam Powering history Operation of accelerator systems Threading: BPM / BLM / screens Multi-turn commissioning, first tune RF capture Additional BI Overall machine performance Orbit, tune, chromaticity, optics Comparisons with design values Conclusions 23

24 Machine integer tunes (beam 2) Nominal integer tunes: Qh = 64; Qv = 59 24

25 Tune, coupling and chromaticity Tunes and coupling measured for circulating beam with BBQ (without/with chirp excitation) and turnby-turn analysis of injection oscillations: Qx = / (nom = ) Qy = / (nom = ) Coupling 0.07 / 0.06 (uncorrected) Qx Qy 30 units (preliminary) Coupling compatible with expectations S. Fartouhk (LCC, 2002): 0.06 / 0.04 No corrections implemented yet!! R. Steinhagen et al., LHC-Perf-Note-007 Problem to get the nominal tunes due to coupling. Uncertainty due also to tune reproducibility. See also R. Jones talk. R. Tomàs et al., LHC-Perf-Note

26 Closed-orbit: first day X orbit [mm] Y orbit [mm] IP2 IP3 IP4 IP5 IP6 IP7 IP8 IP1 Horizontal closed-orbit -10 Vertical closed-orbit Longitudinal coordinate [ km ] First closed-orbit (120 turns) in the evening of Sep. 10 th, RF off (while changes of Q and Q where still being made...) Nevertheless, peak orbit errors already close to tolerance! Disclaimer: BPM not yet fully commissioned. A few faulty or strange monitor readings were found RMS = 2.25 mm Horizontal position [ mm ] RMS = 2.14 mm Arc Tol.: ± 4 mm Vertical position [ mm ] 26

27 Best closed-orbit: third day RMS = 1.60 mm Arc Tol.: ± 4 mm Horizontal position [ mm ] J. Wenninger: optimization of closed-orbit with little effort carries out on Sep. 12 th, after RF capture. The RMS calculated excluding bad BPM s (red in plot) is: RMSH = 1.6 mm; RMSV = 1.3 mm Peak-to-peak: only a few monitors outside ±4 mm tolerance. Horizontal orbit: negative offset of -1.2 mm due to energy error RMS = 1.26 mm Vertical position [ mm ] 27

28 RF settings and beam momentum Preliminary estimate of fs (T. Bohl et al): fs 60 Hz from peak detector Schottky spectrum (fs,0 66 Hz for 8 MV) RF frequency for captured beam: Hz (Δ = 229 Hz) Theoretical value: Hz Average energy offset from closed-orbit: -9.4 units (Δp/p ) (consistent with first-turn estimates) 10 units Courtesy of T. Bohl Courtesy of J. Wenninger 28

29 Problem: effect of MSI field on orbit Transverse cross-section of injection septum Perturbation of the beam orbit found by R. Steinhagen and J. Wenninger - RMS: vertical 250 μm; horizontal 100 μm. Period of the SPS cycle (42 second) - Corresponding peak perturbation larger than 500 μm (V)!! - The perturbation is fast and cannot be easily compensated by the orbit feedback Likely source of perturbation: Residual dipole kicks from the injection septa MSI in P2 / P8, pulsed with SPS timing Solution: power the MSI in DC mode - hardware allows that - with static correction! 29

30 Mechanical aperture of the ring Plot by R. Calaga Aperture measurement during sector test done systematically in Sectors 2-3 and 7-8: Example: ARC 1-2 No systematic aperture measurements done for the whole LHC ring Used measurements of response matrices to see the largest oscillations that we could fit... We routinely achieved oscillations of ±10mm without apparent problems with losses. But: no systematic scan of oscillation phases! Cannot draw firm conclusions 30

31 Beta-beat estimates All details discussed by R. Tomàs later in this session - Horizontal beating 30%, isolated peaks 40% - Vertical beating up to % No attempts yet to correct - source likely to be found. 31

32 Conclusions Great success of 10 th Sep. event Remarkable performance of most systems So far, only tested for 450 GeV beam; I<5x10 9 p; only few h of operation! Many crucial accelerator systems deployed Impressive performance of beam instrumentation Impressive list of tools available from day 1 Initial commissioning with beam of controls, injection, RF, beam dump, machine protection, collimators,... Accurate magnetic model; remarkable magnet alignment From beam point of view, the machine looks good Linear optics according to expectations Tolerance of orbit and aperture seem within reach List of problems encountered will be fed back for next run However... a LOT of work is ahead of us!! 32

33 Reserve slides 33

34 Beam losses from collimator in IR Beam on "TCSG-A4R7-B2" "TCSG-B4R7-B2" "TCSG-A5R7-B2" "TCSG-A6R7-B2" "TCSG-A4L7-B2" "TCLA-A6L7-B2" "TCP-C6R7-B2" "TCP-D6R7-B2" "TCP-B6R7-B2" "TCSG-6L7-B2" (03:06:01) (03:13:13) (03:14:01) (03:14:49) (03:05:13) (03:08:25) (03:09:13) (03:10:49) (03:11:37) (03:12:25) 10-3 All collimators around the ring up and running IP7 Could verify of all configurations BLM signal [ Gy/s ] Validate BLM locations that optimize loss response Assess collimator HW response with (small) irradiation Calibrate BLM response simulations Beam 2 (ongoing) Longitudinal position [ km ] BLM + Collimation teams 34

35 Beam current measurements First calibrated bunch-bybunch measurement Fixed-display of LHC DC-BCT LHC Fast-BCT acquisition Courtesy of M. Ludwig Programs by M. Albert 35

36 Example of response measurement 6 4 Vertical [ mm ] Longitudinal coordinate [ km ] 36

Nominal LHC parameters

Nominal LHC parameters Nominal LHC parameters The nominal LHC peak luminosity L = 10 34 cm 2 s 1 corresponds to a nominal bunch spacing of 25 ns and to β = 0.5 m, full crossing angle θ c = 300 µrad, and bunch population N b

More information

R. Assmann, CERN/AB. for the Collimation Project 7/12/2007 LHC MAC RWA, LHC MAC 12/07

R. Assmann, CERN/AB. for the Collimation Project 7/12/2007 LHC MAC RWA, LHC MAC 12/07 Plan for Collimator Commissioning R. Assmann, CERN/AB 7/12/2007 for the Collimation Project LHC MAC RWA, LHC MAC 12/07 1) Installation Planning and Performance Reach Collimation is an performance-driven

More information

Assessment of BLM Thresholds in Collimation Regions for the LHC startup

Assessment of BLM Thresholds in Collimation Regions for the LHC startup Assessment of BLM Thresholds in Collimation Regions for the LHC startup By Till Böhlen & BLM Team 1/11 Content Introduction to Protection of Collimators Approach & Work so far Experiment @ SPS & Simulations

More information

LHC TRANSVERSE FEEDBACK SYSTEM: FIRST RESULTS OF COMMISSIONING. V.M. Zhabitsky XXI Russian Particle Accelerator Conference

LHC TRANSVERSE FEEDBACK SYSTEM: FIRST RESULTS OF COMMISSIONING. V.M. Zhabitsky XXI Russian Particle Accelerator Conference LHC TRANSVERSE FEEDBACK SYSTEM: FIRST RESULTS OF COMMISSIONING V.M. Zhabitsky XXI Russian Particle Accelerator Conference 28.09-03.10.2008, Zvenigorod LHC Transverse Feedback System: First Results of Commissioning

More information

Betatron tune Measurement

Betatron tune Measurement Betatron tune Measurement Tom UESUGI, Y. Kuriyama, Y. Ishi FFA school, Sep. 8-9, Osaka, 218 CONTENTS Betatron oscillation and tune How to measure tunes KURNS FFAG, Diagnostics BETATRON OSCILLATION AND

More information

MD Amplitude Detuning Studies at 6.5 TeV with Various Configurations of the Crossing Scheme

MD Amplitude Detuning Studies at 6.5 TeV with Various Configurations of the Crossing Scheme CERN-ACC-NOTE-2018-0022 28 February 2018 felix.simon.carlier@cern.ch MD2723 - Amplitude Detuning Studies at 6.5 TeV with Various Configurations of the Crossing Scheme F. Carlier, J. Coello de Portugal,

More information

MD 2485: Active halo control using narrowband and colored noise excitations

MD 2485: Active halo control using narrowband and colored noise excitations CERN-ACC-NOTE-2018-0020 28 February 2018 hector.garcia.morales@cern.ch MD 2485: Active halo control using narrowband and colored noise excitations H.Garcia-Morales, Royal Holloway University of London,

More information

FAST RF KICKER DESIGN

FAST RF KICKER DESIGN FAST RF KICKER DESIGN David Alesini LNF-INFN, Frascati, Rome, Italy ICFA Mini-Workshop on Deflecting/Crabbing Cavity Applications in Accelerators, Shanghai, April 23-25, 2008 FAST STRIPLINE INJECTION KICKERS

More information

Re-commissioning the Recycler Storage Ring at Fermilab

Re-commissioning the Recycler Storage Ring at Fermilab Re-commissioning the Recycler Storage Ring at Fermilab Martin Murphy, Fermilab Presented August 10, 2012 at SLAC National Laboratory for the Workshop on Accelerator Operations The Fermi National Accelerator

More information

TCT - Locations. V. Kain, S. Redaelli, R. Assmann, R. Schmidt. Tertiary collimators (TCTs) for the LHC

TCT - Locations. V. Kain, S. Redaelli, R. Assmann, R. Schmidt. Tertiary collimators (TCTs) for the LHC TCT - Locations V. Kain, S. Redaelli, R. Assmann, R. Schmidt Introduction: Tertiary collimators (TCTs) for the LHC Why alternative locations? General proposal for IRs Proposed Locations for the different

More information

Transverse Wakefields and Alignment of the LCLS-II Kicker and Septum Magnets

Transverse Wakefields and Alignment of the LCLS-II Kicker and Septum Magnets Transverse Wakefields and Alignment of the LCLS-II Kicker and Septum Magnets LCLS-II TN-16-13 12/12/2016 P. Emma, J. Amann,K. Bane, Y. Nosochkov, M. Woodley December 12, 2016 LCLSII-TN-XXXX 1 Introduction

More information

Status of Proton Beam Commissioning at MedAustron Ion Beam Therapy Center

Status of Proton Beam Commissioning at MedAustron Ion Beam Therapy Center Status of Proton Beam Commissioning at MedAustron Ion Beam Therapy Center A. Garonna, A. Wastl, C. Kurfuerst, T. Kulenkampff, C. Schmitzer, L. Penescu, M. Pivi, M. Kronberger, F. Osmic, P. Urschuetz On

More information

Initial Beam Phasing of the SRF Cavities in LCLS-II

Initial Beam Phasing of the SRF Cavities in LCLS-II Introduction Initial Beam Phasing of the SRF Cavities in LCLS-II P. Emma Nov. 28, 2016 One of the more challenging aspects of commissioning the LCLS-II accelerator is in the initial phasing of the SRF

More information

Shintake Monitor Nanometer Beam Size Measurement and Beam Tuning

Shintake Monitor Nanometer Beam Size Measurement and Beam Tuning Shintake Monitor Nanometer Beam Size Measurement and Beam Tuning Technology and Instrumentation in Particle Physics 2011 Chicago, June 11 Jacqueline Yan, M.Oroku, Y. Yamaguchi T. Yamanaka, Y. Kamiya, T.

More information

Beam Loss Calibration Studies at the LHC Collimator in LSS5

Beam Loss Calibration Studies at the LHC Collimator in LSS5 Beam Loss Calibration Studies at the LHC Collimator in LSS5 Experiment and Simulation BLM Team Till Böhlen 1 Outline Project Introduction Purpose, Aims & Related Work Experiment @ SPS Simulations Measurements,

More information

The impedance budget of the CERN Proton Synchrotron (PS)

The impedance budget of the CERN Proton Synchrotron (PS) The impedance budget of the CERN Proton Synchrotron (PS) Serena Persichelli CERN Hadron Synchrotron Collective effects University of Rome La Sapienza serena.persichelli@cern.ch Why do we study the beam

More information

FLASH 2. FEL seminar. Charge: 0.5 nc. Juliane Rönsch-Schulenburg Overview of FLASH 2 Hamburg,

FLASH 2. FEL seminar. Charge: 0.5 nc. Juliane Rönsch-Schulenburg Overview of FLASH 2 Hamburg, FLASH 2 FEL seminar Juliane Rönsch-Schulenburg Overview of FLASH 2 Hamburg, 2016-03-22 Charge: 0.5 nc Overview 1. FLASH 2 Overview 1.Layout parameters 2. Operation FLASH2. 1.Lasing at wavelengths between

More information

Beam Diagnostics, Low Level RF and Feedback for Room Temperature FELs. Josef Frisch Pohang, March 14, 2011

Beam Diagnostics, Low Level RF and Feedback for Room Temperature FELs. Josef Frisch Pohang, March 14, 2011 Beam Diagnostics, Low Level RF and Feedback for Room Temperature FELs Josef Frisch Pohang, March 14, 2011 Room Temperature / Superconducting Very different pulse structures RT: single bunch or short bursts

More information

Emilia Cruz. September 21, 2015

Emilia Cruz. September 21, 2015 Designing the interaction regions of the upgrades of the LHC Emilia Cruz September 21, 2015 7/7/2016 1 About me Guadalajara, Mexico 7/7/2016 2 About me Bachelors degree: National Autonomous University

More information

MEASUREMENT OF THE BEAM POSITION IN THE LHC MAIN RINGS

MEASUREMENT OF THE BEAM POSITION IN THE LHC MAIN RINGS CERN CH-1211 Geneva 23 Switzerland the Large Hadron Collider project CERN Div./Group or Supplier/Contractor Document No. SL/BI EDMS Document No. 327557 Date: 2002-02-11 Functional Specification MEASUREMENT

More information

Activities on Beam Orbit Stabilization at BESSY II

Activities on Beam Orbit Stabilization at BESSY II Activities on Beam Orbit Stabilization at BESSY II J. Feikes, K. Holldack, P. Kuske, R. Müller BESSY Berlin, Germany IWBS`02 December 2002 Spring 8 BESSY: Synchrotron Radiation User Facility BESSY II:

More information

Modeling and Measurement of Amplitude Dependent Tune Shifts in CESR

Modeling and Measurement of Amplitude Dependent Tune Shifts in CESR Modeling and Measurement of Amplitude Dependent Tune Shifts in CESR Sarah Woodall Lander University David Rubin and Jim Shanks Cornell University Outline Background information about tune and origin of

More information

VIBRATING WIRE SENSORS FOR BEAM INSTRUMENTATION Suren Arutunian

VIBRATING WIRE SENSORS FOR BEAM INSTRUMENTATION Suren Arutunian VIBRATING WIRE SENSORS FOR BEAM INSTRUMENTATION Suren Arutunian Yerevan Physics Institute Yerevan Physics Institute S.Arutunian, VIBRATING WIRE SENSORS FOR BEAM INSTRUMENTATION BIW 2008, Lake Tahoe, USA

More information

ATF2 Project at KEK. T. Tauchi, KEK at Orsay 17 June, 2005

ATF2 Project at KEK. T. Tauchi, KEK at Orsay 17 June, 2005 ATF2 Project at KEK T. Tauchi, KEK at Orsay 17 June, 2005 IP Final Goal Ensure collisions between nanometer beams; i.e. luminosity for ILC experiment Reduction of Risk at ILC FACILITY construction, first

More information

Accelerator Complex U70 of IHEP-Protvino: Status and Upgrade Plans

Accelerator Complex U70 of IHEP-Protvino: Status and Upgrade Plans INSTITUTE FOR HIGH ENERGY PHYSICS () Protvino, Moscow Region, 142281, Russia Accelerator Complex U70 of -Protvino: Status and Upgrade Plans (report 4.1-1) Sergey Ivanov, on behalf of the U70 staff September

More information

C ll l i l m i a m to t rs Słąwomir Wronka O t u l t i l n i e

C ll l i l m i a m to t rs Słąwomir Wronka O t u l t i l n i e Collimators High Power Hadron Machines, CAS Bilbao, 31.05.2011 Słąwomir Wronka Outline Introduction & definitions Types of collimators Typical chalanges & problems Examples 1 Definition A collimator is

More information

A high resolution bunch arrival time monitor system for FLASH / XFEL

A high resolution bunch arrival time monitor system for FLASH / XFEL A high resolution bunch arrival time monitor system for FLASH / XFEL K. Hacker, F. Löhl, F. Ludwig, K.H. Matthiesen, H. Schlarb, B. Schmidt, A. Winter October 24 th Principle of the arrival time detection

More information

SOLEIL Libera Performance

SOLEIL Libera Performance SOLEIL Libera Performance Libera Workshop 24/25 September 2007 on behalf of the SOLEIL BPM team BPM system: MAC2 requirements, Feb. 2002 closed orbit Correction number of BPMs 120 instead of 112 single

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

Acceleration of High-Intensity Protons in the J-PARC Synchrotrons. KEK/J-PARC M. Yoshii

Acceleration of High-Intensity Protons in the J-PARC Synchrotrons. KEK/J-PARC M. Yoshii Acceleration of High-Intensity Protons in the J-PARC Synchrotrons KEK/J-PARC M. Yoshii Introduction 1. J-PARC consists of 400 MeV Linac, 3 GeV Rapid Cycling Synchrotron (RCS) and 50 GeV Main synchrotron

More information

Experiences of the QSBPM System on MAX II

Experiences of the QSBPM System on MAX II Experiences of the QSBPM System on MAX II Peter Röjsel MAX-lab, Lund University, Lund, Sweden Abstract. The MAX II is a third-generation synchrotron radiation source. The first beamline is in operation

More information

Beam Control: Timing, Protection, Database and Application Software

Beam Control: Timing, Protection, Database and Application Software Beam Control: Timing, Protection, Database and Application Software C.M. Chu, J. Tang 储中明 / 唐渊卿 Spallation Neutron Source Oak Ridge National Laboratory Outline Control software overview Timing system Protection

More information

CHAPTER 13 BEAM INSTRUMENTATION

CHAPTER 13 BEAM INSTRUMENTATION CHAPTER 13 BEAM INSTRUMENTATION 13.1 BEAM POSITION MEASUREMENT A complete list of the beam position monitors associated with orbit and trajectory measurements is given in Tab. 13.1. There are three types

More information

The HL-LHC Machine *

The HL-LHC Machine * Chapter 3 The HL-LHC Machine * I. Bejar 1, O. Brüning 1, P. Fessia 2, L. Rossi 1, R. Tomas 3 and M. Zerlauth 2 1 CERN, Accelerator and Technology Sector, Genève 23, CH-1211, Switzerland 2 CERN, TE Department,

More information

Totem Experiment Status Report

Totem Experiment Status Report Totem Experiment Status Report Edoardo Bossini (on behalf of the TOTEM collaboration) 131 st LHCC meeting 1 Outline CT-PPS layout and acceptance Running operation Detector commissioning CT-PPS analysis

More information

CTPPS Detector Performance

CTPPS Detector Performance CTPPS Detector Performance Run 2016 Data summary SiStrips Performance Data Quality Radiation Damage Alignment Optics Validation Acceptance Diamond Performance Data Quality Data consistency checks Run 2017

More information

Physics Requirements Document Document Title: SCRF 1.3 GHz Cryomodule Document Number: LCLSII-4.1-PR-0146-R0 Page 1 of 7

Physics Requirements Document Document Title: SCRF 1.3 GHz Cryomodule Document Number: LCLSII-4.1-PR-0146-R0 Page 1 of 7 Document Number: LCLSII-4.1-PR-0146-R0 Page 1 of 7 Document Approval: Originator: Tor Raubenheimer, Physics Support Lead Date Approved Approver: Marc Ross, Cryogenic System Manager Approver: Jose Chan,

More information

FLASH at DESY. FLASH. Free-Electron Laser in Hamburg. The first soft X-ray FEL operating two undulator beamlines simultaneously

FLASH at DESY. FLASH. Free-Electron Laser in Hamburg. The first soft X-ray FEL operating two undulator beamlines simultaneously FLASH at DESY The first soft X-ray FEL operating two undulator beamlines simultaneously Katja Honkavaara, DESY for the FLASH team FEL Conference 2014, Basel 25-29 August, 2014 First Lasing FLASH2 > First

More information

Vision for the Future: BESSY VSR A Variable Bunch Length Storage Ring

Vision for the Future: BESSY VSR A Variable Bunch Length Storage Ring Vision for the Future: BESSY VSR A Variable Bunch Length Storage Ring Gode Wüstefeld, HZB ESLS, Aarhus, Nov. 23-24, 211 presented by P. Kuske Outline BESSY VSR - Motivation - Limits of short bunches: measurements

More information

AC Dispersion Measurement. David Rubin Cornell Laboratory for Accelerator-Based Sciences and Education

AC Dispersion Measurement. David Rubin Cornell Laboratory for Accelerator-Based Sciences and Education AC Dispersion Measurement David Rubin Cornell Laboratory for Accelerator-Based Sciences and Education AC dispersion measurement Traditional dispersion measurement - Measure orbit - Change ring energy (δe/e

More information

ANALYSIS OF 3RD OCTAVE BAND GROUND MOTIONS TRANSMISSION IN SYNCHROTRON RADIATION FACILITY SOLARIS Daniel Ziemianski, Marek Kozien

ANALYSIS OF 3RD OCTAVE BAND GROUND MOTIONS TRANSMISSION IN SYNCHROTRON RADIATION FACILITY SOLARIS Daniel Ziemianski, Marek Kozien ANALYSIS OF 3RD OCTAVE BAND GROUND MOTIONS TRANSMISSION IN SYNCHROTRON RADIATION FACILITY SOLARIS Daniel Ziemianski, Marek Kozien Cracow University of Technology, Institute of Applied Mechanics, al. Jana

More information

PINGER MAGNET SYSTEM FOR THE ALBA SYNCHROTRON LIGHT SOURCE

PINGER MAGNET SYSTEM FOR THE ALBA SYNCHROTRON LIGHT SOURCE ACDIV-2015-03 May, 2015 PINGER MAGNET SYSTEM FOR THE ALBA SYNCHROTRON LIGHT SOURCE M.Pont, N.Ayala, G.Benedetti, M.Carla, Z.Marti, R.Nuñez ALBA Synchrotron, Barcelona, Spain Abstract A pinger magnet system

More information

Magnet Powering with zero downtime a dream?

Magnet Powering with zero downtime a dream? Magnet Powering with zero downtime a dream? M. Zerlauth LHC Performance Workshop February 2012 Thanks to : HWC team, H.Thiesen, V.Montabonnet, J.P.Burnet, S.Claudet, E.Blanco, R.Denz, R.Schmidt, E.Blanco,

More information

Coherent Synchrotron Radiation in the ANKA Storage Ring

Coherent Synchrotron Radiation in the ANKA Storage Ring Coherent Synchrotron Radiation in the ANKA Storage Ring Marcel Schuh On behalf of the ANKA THz-Group Laboratory for Applications of Synchrotron Radiation (LAS) / Institute of Synchrotron Radiation (ISS)

More information

Attosecond Diagnostics of Muti GeV Electron Beams Using W Band Deflectors

Attosecond Diagnostics of Muti GeV Electron Beams Using W Band Deflectors Attosecond Diagnostics of Muti GeV Electron Beams Using W Band Deflectors V.A. Dolgashev, P. Emma, M. Dal Forno, A. Novokhatski, S. Weathersby SLAC National Accelerator Laboratory FEIS 2: Femtosecond Electron

More information

Bunch-by-Bunch Broadband Feedback for the ESRF

Bunch-by-Bunch Broadband Feedback for the ESRF Bunch-by-Bunch Broadband Feedback for the ESRF ESLS RF meeting / Aarhus 21-09-2005 J. Jacob, E. Plouviez, J.-M. Koch, G. Naylor, V. Serrière Goal: Active damping of longitudinal and transverse multibunch

More information

Recent studies of the electron cloud-induced beam instability at the Los Alamos PSR

Recent studies of the electron cloud-induced beam instability at the Los Alamos PSR Recent studies of the electron cloud-induced beam instability at the Los Alamos PSR R. Macek 10/7/10 Other Participants: L. Rybarcyk, R. McCrady, T Zaugg Results since ECLOUD 07 workshop Slide 1 Slide

More information

Integration of the Beam Position Monitoring System into the Controls & Operation Environment

Integration of the Beam Position Monitoring System into the Controls & Operation Environment 2017-09-06 FC2WG Meeting #30 Common Specification F-CS-B-0005e: Integration of the Beam Position Monitoring System into the Controls & Operation Environment https://edms.cern.ch/document/1823368/ J. Fitzek,

More information

LHC. LHC Crab-cavity Aspects & Strategy. LHC Upgrade & Crab Crossing. New Road Map. SPS, a first validation step

LHC. LHC Crab-cavity Aspects & Strategy. LHC Upgrade & Crab Crossing. New Road Map. SPS, a first validation step LHC Crab-cavity Aspects & Strategy Rama Calaga (for the LHC-CC collaboration) IPAC10, Kyoto, May 25, 2010 LHC LHC Upgrade & Crab Crossing New Road Map SPS, a first validation step Special thanks: R. Assmann,

More information

Tutorial on Design of RF system for Indus Accelerator. Maherdra Lad Head, Radio Frequency Systems Division RRCAT, Indore

Tutorial on Design of RF system for Indus Accelerator. Maherdra Lad Head, Radio Frequency Systems Division RRCAT, Indore Tutorial on Design of RF system for Indus Accelerator Maherdra Lad Head, Radio Frequency Systems Division RRCAT, Indore Basic principle of RF Acceleration RF Power Amplifier The RF source supplies power

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

BEPCII-THE SECOND PHASE CONSTRUCTION OF BEIJING ELECTRON POSITRON COLLIDER

BEPCII-THE SECOND PHASE CONSTRUCTION OF BEIJING ELECTRON POSITRON COLLIDER BEPCII-THE SECOND PHASE CONSTRUCTION OF BEIJING ELECTRON POSITRON COLLIDER C. Zhang, G.X. Pei for BEPCII Team IHEP, CAS, P.O. Box 918, Beijing 100039, P.R. China Abstract BEPCII, the second phase construction

More information

Short-Pulse X-ray at the Advanced Photon Source Overview

Short-Pulse X-ray at the Advanced Photon Source Overview Short-Pulse X-ray at the Advanced Photon Source Overview Vadim Sajaev and Louis Emery Accelerator Operations and Physics Group Accelerator Systems Division Mini-workshop on Methods of Data Analysis in

More information

THz Pump Beam for LCLS. Henrik Loos. LCLS Hard X-Ray Upgrade Workshop July 29-31, 2009

THz Pump Beam for LCLS. Henrik Loos. LCLS Hard X-Ray Upgrade Workshop July 29-31, 2009 Beam for LCLS Henrik Loos Workshop July 29-31, 29 1 1 Henrik Loos Overview Coherent Radiation Sources Timing THz Source Performance 2 2 Henrik Loos LCLS Layout 6 MeV 135 MeV 25 MeV 4.3 GeV 13.6 GeV σ z.83

More information

Spin Manipulation with an RF Wien-Filter at COSY PSTP Workshop 2015

Spin Manipulation with an RF Wien-Filter at COSY PSTP Workshop 2015 Spin Manipulation with an RF Wien-Filter at COSY PSTP Workshop 2015 Bochum, September 15, 2015 Forschungszentrum Jülich Sebastian Mey and Ralf Gebel for the JEDI Collaboration Content EDM Measurements

More information

Low-Level RF. S. Simrock, DESY. MAC mtg, May 05 Stefan Simrock DESY

Low-Level RF. S. Simrock, DESY. MAC mtg, May 05 Stefan Simrock DESY Low-Level RF S. Simrock, DESY Outline Scope of LLRF System Work Breakdown for XFEL LLRF Design for the VUV-FEL Cost, Personpower and Schedule RF Systems for XFEL RF Gun Injector 3rd harmonic cavity Main

More information

Using Higher Order Modes in the Superconducting TESLA Cavities for Diagnostics at DESY

Using Higher Order Modes in the Superconducting TESLA Cavities for Diagnostics at DESY Using Higher Order Modes in the Superconducting TESLA Cavities for Diagnostics at FLASH @ DESY N. Baboi, DESY, Hamburg for the HOM team : S. Molloy 1, N. Baboi 2, N. Eddy 3, J. Frisch 1, L. Hendrickson

More information

The Commissioning of the ATLAS Pixel Detector

The Commissioning of the ATLAS Pixel Detector The Commissioning of the ATLAS Pixel Detector XCIV National Congress Italian Physical Society Genova, 22-27 Settembre 2008 Nicoletta Garelli Large Hadronic Collider MOTIVATION: Find Higgs Boson and New

More information

INSTALLATION AND FIRST COMMISSIONING OF THE LLRF SYSTEM

INSTALLATION AND FIRST COMMISSIONING OF THE LLRF SYSTEM INSTALLATION AND FIRST COMMISSIONING OF THE LLRF SYSTEM FOR THE EUROPEAN XFEL Julien Branlard, for the LLRF team TALK OVERVIEW 2 Introduction Brief reminder about the XFEL LLRF system Commissioning goals

More information

ONLINE COUPLING MEASUREMENT AND CORRECTION THROUGHOUT THE LHC CYCLE

ONLINE COUPLING MEASUREMENT AND CORRECTION THROUGHOUT THE LHC CYCLE Content from this work may be used under the terms of the CC BY 3.0 licence ( 2017). Any distribution of this work must maintain attribution to the author(s), title of the work, publisher, and DOI. 16th

More information

Proceedings of Chamonix 2010 workshop on LHC Performance CRAB CAVITIES

Proceedings of Chamonix 2010 workshop on LHC Performance CRAB CAVITIES CRAB CAVITIES R. Calaga, R. De-Maria (BNL), E. Metral, Y. Sun, R. Tomás, F. Zimmermann (CERN) Abstract With lower betas at collision points or longer bunches, luminosity loss due to the crossing angle

More information

Towards an RF Wien-Filter for EDM Searches in Storage Rings

Towards an RF Wien-Filter for EDM Searches in Storage Rings Towards an RF Wien-Filter for EDM Searches in Storage Rings DPG Annual Spring Meeting 2015 Wuppertal, March 10, 2015 Sebastian Mey and Ralf Gebel for the JEDI Collaboration Forschungszentrum Jülich Content

More information

Detection of Beam Induced Dipole-Mode Signals in the SLC S-Band Structures* Abstract

Detection of Beam Induced Dipole-Mode Signals in the SLC S-Band Structures* Abstract -. SLAC-PUB-79 June 1997 Detection of Beam nduced Dipole-Mode Signals in the SLC S-Band Structures* M. Seidel, C. Adolphsen, R. Assmann, D.H. Whittum Stanford Linear Accelerator Center, Stanford University,

More information

Nonintercepting Diagnostics for Transverse Beam Properties: from Rings to ERLs

Nonintercepting Diagnostics for Transverse Beam Properties: from Rings to ERLs Nonintercepting Diagnostics for Transverse Beam Properties: from Rings to ERLs Alex H. Lumpkin Accelerator Operations Division Advanced Photon Source Presented at Jefferson National Accelerator Laboratory

More information

O. Napoly LC02, SLAC, Feb. 5, Higher Order Modes Measurements

O. Napoly LC02, SLAC, Feb. 5, Higher Order Modes Measurements O. Napoly LC02, SLAC, Feb. 5, 2002 Higher Order Modes Measurements with Beam at the TTF Linac TTF Measurements A collective effort including most of Saclay, Orsay and DESY TTF physicists : S. Fartoukh,

More information

Precision RF Beam Position Monitors for Measuring Beam Position and Tilt Progress Report

Precision RF Beam Position Monitors for Measuring Beam Position and Tilt Progress Report Precision RF Beam Position Monitors for Measuring Beam Position and Tilt Progress Report UC Berkeley Senior Personnel Yury G. Kolomensky Collaborating Institutions Stanford Linear Accelerator Center: Marc

More information

Non-invasive Beam Profile Measurements using an Electron-Beam Scanner

Non-invasive Beam Profile Measurements using an Electron-Beam Scanner Non-invasive Beam Profile Measurements using an Electron-Beam Scanner W. Blokland and S. Cousineau Willem Blokland for the Spallation Neutron Source Managed by UT-Battelle Overview SNS Accelerator Electron

More information

Lattice Design for PRISM-FFAG. A. Sato Osaka University for the PRISM working group

Lattice Design for PRISM-FFAG. A. Sato Osaka University for the PRISM working group Lattice Design for PRISM-FFAG A. Sato Osaka University for the PRISM working group contents PRISM overview PRISM-FFAG dynamics study & its method PRISM Phase Rotated Intense Slow Muon source Anticipated

More information

Diamond sensors as beam conditions monitors in CMS and LHC

Diamond sensors as beam conditions monitors in CMS and LHC Diamond sensors as beam conditions monitors in CMS and LHC Maria Hempel DESY Zeuthen & BTU Cottbus on behalf of the BRM-CMS and CMS-DESY groups GSI Darmstadt, 11th - 13th December 2011 Outline 1. Description

More information

How did the LHC access system perform in 2009

How did the LHC access system perform in 2009 How did the LHC access system perform in 2009 L. Ponce On behalf of the OP team And a special thanks to all the volunteers who helped giving access Outline Some preliminary remarks Status and major issues

More information

Position of the LHC luminous region

Position of the LHC luminous region Position of the LHC luminous region SL/HRF reported by Philippe Baudrenghien Philippe Baudrenghien SL-HRF 1 RF low-level during physics (tentative...) Good lifetime -> One phase loop per beam... - Goal

More information

Operation of a Single Pass, Bunch-by-bunch x-ray Beam Size Monitor for the CESR Test Accelerator Research Program. October 3, 2012

Operation of a Single Pass, Bunch-by-bunch x-ray Beam Size Monitor for the CESR Test Accelerator Research Program. October 3, 2012 Operation of a Single Pass, Bunch-by-bunch x-ray Beam Size Monitor for the CESR Test Accelerator Research Program October 3, 2012 Goals Goals For This Presentation: 1.Provide an overview of the efforts

More information

JEDI. Status of the commissioning of the waveguide RF Wien Filter

JEDI. Status of the commissioning of the waveguide RF Wien Filter COSY Beam Time Request For Lab. use Exp. No.: Session No. E 005.4 7 Collaboration: JEDI Status of the commissioning of the waveguide RF Wien Filter Spokespersons for the beam time: Ralf Gebel (Jülich)

More information

FAST KICKERS LNF-INFN

FAST KICKERS LNF-INFN ILC Damping Rings R&D Workshop - ILCDR06 September 26-28, 2006 at Cornell University FAST KICKERS R&D @ LNF-INFN Fabio Marcellini for the LNF fast kickers study group* * D. Alesini, F. Marcellini P. Raimondi,

More information

LHC COMMISSIONING AT HIGHER ENERGY

LHC COMMISSIONING AT HIGHER ENERGY LHC COMMISSIONING AT HIGHER ENERGY P. Collier, F. Bordry, J. Wenninger, CERN, Geneva, Switzerland Abstract The LHC has just come to the end of its first Long Shutdown (LS1) and preparations are underway

More information

EMMA the World's First Non-Scaling FFAG Accelerator

EMMA the World's First Non-Scaling FFAG Accelerator EMMA the World's First Non-Scaling FFAG Accelerator Susan Smith STFC Daresbury Laboratory CONTENTS Introduction Contents What are ns-ffags? and Why EMMA? The international collaboration EMMA goals and

More information

BESSY VSR: SRF challenges and developments for a variable pulse-length next generation light source

BESSY VSR: SRF challenges and developments for a variable pulse-length next generation light source BESSY VSR: SRF challenges and developments for a variable pulse-length next generation light source Institut SRF - Wissenschaft und Technologie (FG-ISRF) Adolfo Vélez et al. SRF17 Lanzhou, 17-21/7/2017

More information

STPA FOR LINAC4 AVAILABILITY REQUIREMENTS. A. Apollonio, R. Schmidt 4 th European STAMP Workshop, Zurich, 2016

STPA FOR LINAC4 AVAILABILITY REQUIREMENTS. A. Apollonio, R. Schmidt 4 th European STAMP Workshop, Zurich, 2016 STPA FOR LINAC4 AVAILABILITY REQUIREMENTS A. Apollonio, R. Schmidt 4 th European STAMP Workshop, Zurich, 2016 LHC colliding particle beams at very high energy 26.8 km Circumference LHC Accelerator (100

More information

MEASUREMENT OF BEAM LOSSES USING OPTICAL FIBRES AT THE AUSTRALIAN SYNCHROTRON

MEASUREMENT OF BEAM LOSSES USING OPTICAL FIBRES AT THE AUSTRALIAN SYNCHROTRON MEASUREMENT OF BEAM LOSSES USING OPTICAL FIBRES AT THE AUSTRALIAN SYNCHROTRON E. Nebot del Busto (1,2), M. J. Boland (3,4), E. B. Holzer (1), P. D. Jackson (5), M. Kastriotou (1,2), R. P. Rasool (4), J.

More information

Digital Signal processing in Beam Diagnostics Lecture 2

Digital Signal processing in Beam Diagnostics Lecture 2 Digital Signal processing in Beam Diagnostics Lecture 2 Ulrich Raich CERN AB - BI (Beam Instrumentation) 1 Overview Lecture 2 Left-over from yesterday: Trajectory measurements Synchronisation to BPM signals

More information

Proposal of test setup

Proposal of test setup Proposal of test setup Status of the study The Compact Linear collider (CLIC) study is a site independent feasibility study aiming at the development of a realistic technology at an affordable cost for

More information

LCLS Injector Diagnostics. Henrik Loos. Diagnostics overview Transverse Beam Properties Longitudinal Beam Properties

LCLS Injector Diagnostics. Henrik Loos. Diagnostics overview Transverse Beam Properties Longitudinal Beam Properties Diagnostics overview Transverse Beam Properties Longitudinal Beam Properties LCLS Diagnostics Tasks Charge Toroids (Gun, Inj, BC, Und) Faraday cups (Gun & Inj) Trajectory & energy Stripline BPMs (Gun,

More information

Hall C Polarimetry at 12 GeV Dave Gaskell Hall C Users Meeting January 14, 2012

Hall C Polarimetry at 12 GeV Dave Gaskell Hall C Users Meeting January 14, 2012 Hall C Polarimetry at 12 GeV Dave Gaskell Hall C Users Meeting January 14, 2012 1. Møller Polarimeter 2. Compton Polarimeter Hall C 12 GeV Polarimetry Møller Polarimeter 6 GeV operation: uses 2 quads to

More information

A Study of undulator magnets characterization using the Vibrating Wire technique

A Study of undulator magnets characterization using the Vibrating Wire technique A Study of undulator magnets characterization using the Vibrating Wire technique Alexander. Temnykh a, Yurii Levashov b and Zachary Wolf b a Cornell University, Laboratory for Elem-Particle Physics, Ithaca,

More information

taccor Optional features Overview Turn-key GHz femtosecond laser

taccor Optional features Overview Turn-key GHz femtosecond laser taccor Turn-key GHz femtosecond laser Self-locking and maintaining Stable and robust True hands off turn-key system Wavelength tunable Integrated pump laser Overview The taccor is a unique turn-key femtosecond

More information

Advanced Beam Instrumentation and Diagnostics for FELs

Advanced Beam Instrumentation and Diagnostics for FELs Advanced Beam Instrumentation and Diagnostics for FELs P. Evtushenko, Jefferson Lab with help and insights from many others: S. Benson, D. Douglas, Jefferson Lab T. Maxwell, P. Krejcik, SLAC S. Wesch,

More information

Undulator K-Parameter Measurements at LCLS

Undulator K-Parameter Measurements at LCLS Undulator K-Parameter Measurements at LCLS J. Welch, A. Brachmann, F-J. Decker, Y. Ding, P. Emma, A. Fisher, J. Frisch, Z. Huang, R. Iverson, H. Loos, H-D. Nuhn, P. Stefan, D. Ratner, J. Turner, J. Wu,

More information

Dark Current Kicker Studies at FLASH

Dark Current Kicker Studies at FLASH Dark Current Kicker Studies at FLASH F. Obier, J. Wortmann, S. Schreiber, W. Decking, K. Flöttmann FLASH Seminar, DESY, 02 Feb 2010 History of the dark current kicker 2005 Vertical kicker was installed

More information

Feedback Requirements for SASE FELS. Henrik Loos, SLAC IPAC 2010, Kyoto, Japan

Feedback Requirements for SASE FELS. Henrik Loos, SLAC IPAC 2010, Kyoto, Japan Feedback Requirements for SASE FELS Henrik Loos, SLAC, Kyoto, Japan 1 1 Henrik Loos Outline Stability requirements for SASE FELs Diagnostics for beam parameters Transverse: Beam position monitors Longitudinal:

More information

LHC Electronics irradiation tests in the CNGS side gallery September 2009

LHC Electronics irradiation tests in the CNGS side gallery September 2009 LHC Electronics irradiation tests in the CNGS side gallery September 2009 D.Kramer for the RADWG Thanks to B.Todd, E.Gousiou, E.Calvo, E.Effinger, R.Denz, K.Roeed, J.Lendaro, M.Brugger, EN/MEF, DG/SCR,

More information

New apparatus for precise synchronous phase shift measurements in storage rings 1

New apparatus for precise synchronous phase shift measurements in storage rings 1 New apparatus for precise synchronous phase shift measurements in storage rings 1 Boris Podobedov and Robert Siemann Stanford Linear Accelerator Center, Stanford University, Stanford, CA 94309 Measuring

More information

Commissioning of National Synchrotron Light Source-II (NSLS-II) Fast Orbit Feedback System

Commissioning of National Synchrotron Light Source-II (NSLS-II) Fast Orbit Feedback System Commissioning of National Synchrotron Light Source-II (NSLS-II) Fast Orbit Feedback System 15 th ICALEPCS 2015, Melbourne, Australia K. Ha, Y. Tian, L. Yu, W. Cheng, L. Dalesio W. Levine, University of

More information

Slide Title. Bulleted Text

Slide Title. Bulleted Text Slide Title 1 Slide Outline Title Brief view of the C-AD Complex Review of the RHIC LLRF Upgrade Platform Generic Implementation of a Feedback Loop RHIC Bunch by Bunch Longitudinal Damper Cavity Controller

More information

Joachim Tückmantel CERN, Geneva

Joachim Tückmantel CERN, Geneva Joachim Tückmantel CERN, Geneva Split up the problem : Linac made of different sections Section made of equivalent families Joachim Tückmantel, CERN Family: One transmitter supplies several (or 1) cavities

More information

e+/e- Vertical Beam Dynamics during CESR-C Operation

e+/e- Vertical Beam Dynamics during CESR-C Operation e+/e- Vertical Beam Dynamics during CESR-C Operation I. Introduction II. e+ turn-by-turn vertical dynamics III. e- turn-by-turn vertical dynamics IV. Summary R. Holtzapple, J. Kern, and E.Tanke January

More information

CERN EUROPEAN ORGANIZATION FOR NUCLEAR RESEARCH INVESTIGATION OF A RIDGE-LOADED WAVEGUIDE STRUCTURE FOR CLIC X-BAND CRAB CAVITY

CERN EUROPEAN ORGANIZATION FOR NUCLEAR RESEARCH INVESTIGATION OF A RIDGE-LOADED WAVEGUIDE STRUCTURE FOR CLIC X-BAND CRAB CAVITY CERN EUROPEAN ORGANIZATION FOR NUCLEAR RESEARCH CLIC Note 1003 INVESTIGATION OF A RIDGE-LOADED WAVEGUIDE STRUCTURE FOR CLIC X-BAND CRAB CAVITY V.F. Khan, R. Calaga and A. Grudiev CERN, Geneva, Switzerland.

More information

LUCX - THZ PROGRAM: OVERVIEW AND PROSPECTS

LUCX - THZ PROGRAM: OVERVIEW AND PROSPECTS LUCX - THZ PROGRAM: OVERVIEW AND PROSPECTS A. Aryshev On behalf of QB group and THz collaboration 14 Outline THz project overview LUCX activity LUCX Projects Overview THz program LUCX Laser system LUCX

More information

Plan for Accelerator Beam Study Towards J-PARC Muon Project. Koji YOSHIMURA (KEK) for KEK Muon Working Group at NuFACT08 July 2nd, 2008

Plan for Accelerator Beam Study Towards J-PARC Muon Project. Koji YOSHIMURA (KEK) for KEK Muon Working Group at NuFACT08 July 2nd, 2008 Plan for Accelerator Beam Study Towards J-PARC Muon Project Koji YOSHIMURA (KEK) for KEK Muon Working Group at NuFACT08 July 2nd, 2008 Contents Introduction Muon Project at J-PARC Beam Requirements R&D

More information

Design of beam optics for FCC-ee

Design of beam optics for FCC-ee Design of beam optics for FCC-ee KEK Accelerator Seminar 4 Aug. 2015 K. Oide (KEK) Many thanks to M. Benedikt, A. Bogomyagkov. H. Burkhardt, B. Holzer, J. Jowett, I. Koop, E. Levitchev, P. Piminov, D.

More information

EuroTeV High Bandwidth Wall Current Monitor. Alessandro D Elia AB-BI-PI 1-1 -

EuroTeV High Bandwidth Wall Current Monitor. Alessandro D Elia AB-BI-PI 1-1 - EU contract number RII3-CT-2003-506395 CARE/ELAN Document-2007-012 EuroTeV High Bandwidth Wall Current Monitor Alessandro D Elia AB-BI-PI 1-1 - EU contract number RII3-CT-2003-506395 CARE/ELAN Document-2007-012

More information