AB/BI J. Koopman New WS design - Brain storm session 18/06/2007 1/16 New WS design - Brain storm session.

Slides:



Advertisements
Similar presentations
Lyon 2005 DIPAC Lyon th DIPAC Lyon June 2005Ulrich Raich CERN AB/BDI Instrumentation in small, low energy machines Ulrich Raich CERN AB-BDI.
Advertisements

Measurements of adiabatic dual rf capture in the SIS 18 O. Chorniy.
PIP and the Booster Notch Bob Zwaska October 12, 2011 PIP Meeting.
The performance of Strip-Fiber EM Calorimeter response uniformity, spatial resolution The 7th ACFA Workshop on Physics and Detector at Future Linear Collider.
Low energy electron beam as a nondestructive diagnostic tool for high power beams. P. Logachev, D. Malutin, A. Starostenko, BINP, RUPAC’2006, Novosibirsk.
Bunch shape monitor for Linac-4 A.V.Feschenko Institute For Nuclear Research (INR), Moscow , Russia.
ECFA-DESY workshop, NIKEF 1 st April, 2003Nick Walker, DESY Energy Spread Measurement in the TESLA Extraction Line Nick Walker - DESY.
PS wirescanner calibration Student Meeting 10/03/2014 Carolina Bianchini BE-BI-BL.
Applied Sensor Technology. Outline Introduction Examples of Sensors Basic readout electronics Semiconductor detectors.
INFN of Genova, Pavia and Roma Flavio Gatti, PSI, February 9 th, Timing Counter status Timing Counter status.
Beam Loss Analysis Tool for the CTF3 PETS Tank M. Velasco, T. Lefevre, R. Scheidegger, M. Wood, J. Hebden, G. Simpson Northwestern University, Evanston,
PSB magnetic cycle 160 MeV to 2 GeV with 2.5E13 protons per ring A. Blas 2 GeV magnetic cycle 29/04/ Requirements 1.Present performance: 1E13p from.
Design and test of a high-speed beam monitor for hardon therapy H. Pernegger on behalf of Erich Griesmayer Fachhochschule Wr. Neustadt/Fotec Austria (H.
DORIS - 2 GeV Experiences in 2011 Olympus Collaboration Meeting April 27th, 2011 F.Brinker.
Genova/Pavia/Roma Flavio Gatti, PSI, July 1st, Timing Counter july 2004.
SPS New Wire Scanner Mechanics Review
Matching and Synchrotron Light Diagnostics F.Roncarolo, E.Bravin, S.Burger, A.Goldblatt, G.Trad.
The LHC: an Accelerated Overview Jonathan Walsh May 2, 2006.
1 Performance of multi-anode PMT employing an ultra bi-alkali photo-cathode and rugged dynodes Takahiro Toizumi Tokyo Institute of Technology S. Inagwa.
IPBSM status and plan ATF project meeting M.Oroku.
1 BeamBeam3D: Code Improvements and Applications Ji Qiang Center of Beam Physics Lawrence Berkeley National Laboratory SciDAC II, COMPASS collaboration.
Fermilab, April 8 th, 2003F.Roncarolo 1 CERN SPS Emittance Measurements F. Roncarolo, CERN AB/BDI University of Lausanne Acknowledgments: B.Dehning, R.Jung,
INTRODUCTION  RECYCLER BPM – Original system not adequate to measure beam position precisely. It is being upgraded to meet the required physics precision.
AAC February 4-6, 2003 Protons on Target Ioanis Kourbanis MI/Beams.
Energy calibration at LHC J. Wenninger. Motivation In general there is not much interest for accurate knowledge of the momentum in hadron machines. 
1 C. Simon CLIC Instrumentation workshop BPM C. Simon on behalf of the Saclay’s group CLIC Instrumentation workshop 2 nd - 3 rd June.
Travelling Wave Tube For Broadband amplifier helix TWTs (proposed by Pierce and others in 1946 ) are widely used For High average power purposes the.
RHIC Status: Startup Run 12 V. Schoefer RHIC Spin Collaboration Meeting 1/13/12.
C. Fischer – LHC Instrumentation Review – 19-20/11/2001 Gas Monitors for Transverse Distribution Studies in the LHC LHC Instrumentation Review Workshop.
Development of a Gamma-Ray Beam Profile Monitor for the High-Intensity Gamma-Ray Source Thomas Regier, Department of Physics and Engineering Physics University.
The Stripping Foil Test Stand in the Linac4 Transfer Line
The Quadrupole Pick-up in the CPS -intro and progress report PPC 3 Dec 1999 A. Jansson.
BSRT CALIBRATION MD SUMMARY LSWG #6-15/09/2015 BSRT TEAM.
Multibunch beam stability in damping ring (Proposal of multibunch operation week in October) K. Kubo.
ICFA-HB 2004 Commissioning Experience for the SNS Linac A. Aleksandrov, S. Assadi, I. Campisi, P. Chu, S. Cousineau, V. Danilov, G. Dodson, J. Galambos,
G. Ferioli, R. Jung - LHC-BI Review Workshop November 19&20 LHC Screen Profile Monitors G. Ferioli, R. Jung Introduction BTV LHC layout Monitor set-up.
Beam stability in damping ring - for stable extracted beam for ATF K. Kubo.
LHC Beam Loss Monitors, B.Dehning 1/15 LHC Beam loss Monitors Loss monitor specifications Radiation tolerant Electronics Ionisation chamber development.
FSC Status and Plans Pavel Semenov IHEP, Protvino on behalf of the IHEP PANDA group PANDA Russia workshop, ITEP 27 April 2010.
Linearity Tests The laser induced high noise pulses on the APD rendering it useless. We tried several methods to shield and filter the noise. With a stabilized.
PROBLEM 1 Show that the (beam size ^2) varies quadratically with distance in a drift section with no quadrupoles.
Eduardo Nebot del Busto (1) CERN, Geneva, Switzerland (2) The University of Liverpool, Department of physics, Liverpool, U. K (3) The Cockcroft Institute,
Prepared by M. Jimenez AT Dept / Vacuum Group, ECloud’04 Future Needs and Future Directions Maximizing the LHC Performances J.M. Jimenez …when Nature persists.
SPS proton beam for AWAKE E. Shaposhnikova 13 th AWAKE PEB Meeting With contributions from T. Argyropoulos, T. Bohl, H. Bartosik, S. Cettour.
ATF2 beam operation status Toshiyuki OKUGI, KEK The 9 th TB&SGC meeting KEK, 3-gokan Seminar Hall 2009/ 12/ 16.
Electron Spectrometer: Status July 14 Simon Jolly, Lawrence Deacon 1 st July 2014.
DRAFT: What have been done and what to do in ILC-LET beam dynamics Beam dynamics/Simulations Group Beijing.
IoP HEPP/APP annual meeting 2010 Feedback on Nanosecond Timescales: maintaining luminosity at future linear colliders Ben Constance John Adams Institute,
1 RTML Emittance Measurement Station Yuri Kubyshin (1), Robert Apsimon (2), Hector García (1,2) (1) Technical University of Catalonia (UPC) (2) CERN CLIC.
RHIC Status April 8, 2011 RSC Meeting Haixin Huang.
Experience with Novosibirsk FEL Getmanov Yaroslav Budker INP, Russia Dec. 2012, Berlin, Germany Unwanted Beam Workshop.
ESS wire scanner Benjamin Cheymol
Summary of ions measurements in 2015 and priorities for 2016 studies E. Shaposhnikova 3/02/2016 Based on input from H. Bartosik, T. Bohl, B. Goddard, V.
Beam Instrumentation of CEPC Yue Junhui (岳军会) for the BI Group Accelerator Center, IHEP HF2014.
Requirements from BI and new instruments after LS1 LHC Optics Measurement and Correction Review; B.Dehning 1 Bernd Dehning CERN BE/BI
Beam Gas Imaging Kick-off meeting 30-Oct-2012
Power and control electronics for the new fast wire scanners
Show that the (beam size ^2) varies quadratically with distance in a drift section with no quadrupoles.
PSB rf manipulations PSB cavities
BC2 Commissioning Parameters
Deng Ziyan Jan 10-12, 2006 BESIII Collaboration Meeting
Profile measurements at CTF
ERL accelerator review. Parameters for a Compton source
Sensitivity tests of BLM_S chamber in PSB dump
Beam-Based Alignment Results
PSB magnetic cycle 900 ms MeV to 2 GeV
Another Immortal Fill….
Breakout Session SC3 – Undulator
Computed Tomography (C.T)
Measurement of the beam (transverse) emittances
Presentation transcript:

AB/BI J. Koopman New WS design - Brain storm session 18/06/2007 1/16 New WS design - Brain storm session

AB/BI J. Koopman New WS design - Brain storm session 18/06/2007 2/16 Introduction First rotational WS in SPS in Later WS in PS, LEP, PSB and finally in LHC. LHCSPSPSPSB TypeLinearLinear (DESY) Rotating Speed [m/s] Servo typePosition Speed Servo devicePotentio- meter Tachometer Position read- out device Potentio- meter Optical Ruler Potentio- meter Resolver Amplitude read- out dev. Scint./ PMT Scint./ PMT Scint./ PMT Scint./PMT & SEM

AB/BI J. Koopman New WS design - Brain storm session 18/06/2007 3/16 Encountered problems Breaking wires due to: –Beam interaction. –Induced RF power. Instabilities of position and profile measurements due to: –Inaccuracy of position measurements. –Flexibility, vibrations in mechanics and wire (in some cases). Aging bellows in PS (broke after ~13000 scans). Outgassing bellows in LHC during bake-out. Timing jitter in PS. Magnet quenching in LHC (simulations GEANT4). Fixation wires in fork. Wire drift into beam due to offset in speed feedback loop (PS).

AB/BI J. Koopman New WS design - Brain storm session 18/06/2007 4/16 Different WS types

AB/BI J. Koopman New WS design - Brain storm session 18/06/2007 5/16 Profile examples LHC beam, σ = 1mm LHC beam, σ = 320µm

AB/BI J. Koopman New WS design - Brain storm session 18/06/2007 6/16 Graphs Federico: (every point in the graphs is the result of 500 fit calculations.) –1. Systematic error on beam size due to position resolution limitation. –2. Statistical error on beam size due to limitation in number of primary events. –3. Statistical error on beam size due to presence of noise on amplitude measurement. –4. Statistical error on beam size due to presence of noise on position measurement © F.Roncarolo

AB/BI J. Koopman New WS design - Brain storm session 18/06/2007 7/16 PMT signal LHC quantityunitsaccum. q.units pilot bunch intensity (σ y 450GeV)5.00E+09p p center portion interacting with wire (d=30μm)4% 2.00E+08p interaction/detection efficiency (GEANT)2.50E E+03p average energy deposition (GEANT)10MeV/p5.00E+04MeV BC408 scintillator conversion efficiency8.00E+03photons/MeV4.00E+08ph transmission efficiency scintillator to PMT10%4.00E+07ph quantum efficiency S20 photocathode PMT20%electrons/photon8.00E+06el gain 6-stage XP2243B PMT1.00E E+10el output charge PMT1.60E-19C/el1.28E-08C RMS bunch 450GeV (l=11.12 cm)3.75E-10s PMT pulse duration FWHM (~scintillator p.d.)2.60E-9s theoretical output current PMT FWHM 4.92E+00A

AB/BI J. Koopman New WS design - Brain storm session 18/06/2007 8/16 Thermionic Em. Current 1 st Batch Injection 2 nd Batch Injection Beam Energy Ramp Voltage ~ Heating LHC cycle with 2 injections in the SPS Thermiomic Em.Current

AB/BI J. Koopman New WS design - Brain storm session 18/06/2007 9/16 Ferrite Effects

AB/BI J. Koopman New WS design - Brain storm session 18/06/ /16 Hot wire radiation profile Digitized video recording of an 8 mm carbon wire scanning a 0.8 mA electron beam (LEP). The wire is parallel to the horizontal axis, and the light intensity is plotted along the vertical axis (arbitrary units). Successive profiles are separated by 20 ms. The central spot corresponds to the passage of the wire through the beam.

AB/BI J. Koopman New WS design - Brain storm session 18/06/ /16 Ferrites in SPS

AB/BI J. Koopman New WS design - Brain storm session 18/06/ /16 LHC WS tank

AB/BI J. Koopman New WS design - Brain storm session 18/06/ /16 Requirements 1/2 Wire speed (actual range from 0.1 to 20 m/s): –High: Wire damage. Magnet quench. –Low: PMT signal statistics. Position measurement statistics. Wire diameter (actual range 8-30 µm): –Large: Scintillator signal statistics. Ease of handling. –Small: Magnet quench. Wire material (tried C, SiO 2, SiC, Be, W): –Conducting: Continuity monitoring. Temperature monitoring. –Resisting to high beam intensities and RF power coupling.

AB/BI J. Koopman New WS design - Brain storm session 18/06/ /16 Requirements 2/2 Mechanics: –Rigid: Vibrations, deformations. Position measurement. –Linear: Straight forward position measurement w/o conversion factor errors. Fork: –Opening ranging from 28 (LEP) to 200 mm (SPS). –No Al for LHC. Scan timing inaccuracy < 1ms. Position measurement inaccuracy ~ 1µm.

AB/BI J. Koopman New WS design - Brain storm session 18/06/ /16 Suggestions for a new design 1/2 A wire of 100mm long and 30um of diameter only weights ~160 µg! –Design a light weight wire transport system for high speed (=acceleration). –Need lower force to move this at high speed. –Lower force induces less vibrations. Try to avoid bellows. –Fragile. –Need high forces. Position measurement as close as possible to wire fixation. Design small (RF friendly) wire cavity. Use position instead of speed feedback.

AB/BI J. Koopman New WS design - Brain storm session 18/06/ /16 Suggestions for a new design 2/2