COBRA Magnet Status W. Ootani June 27th, 2006 MEG Review W. Ootani June 27th, 2006 MEG Review.

Slides:



Advertisements
Similar presentations
Liquid H 2 Absorber Production Contents (1)MICE Absorber Status (2)MICE Absorber Modification (3)Plan/Schedule (4)Summary MICE CM-23 in HARBIN Shigeru.
Advertisements

Field measurements of QEA magnets at KEK Mika Masuzawa May 30, 2006.
SLAC, 5-Dec-2006 Magnets and Magnetic Measurements for Prototype Energy Spectrometer T-474.
COBRA Status W. Ootani MEG Review Meeting Jul. 18th, 2007.
A polarized solid state target for photon induced double polarization experiments at ELSA H. Dutz TR16 Bommerholz Hartmut Dutz, S. Goertz, A.
PXIE: SSR1 Section Focusing Lens 1.Requirements table 2.Developed at FNAL 3.Available from vendors 4.Used at ANL 5.Layout of the SSR1 cryomodule 6.Case.
CM-18 June The Measurement and Monitoring of the Field from the MICE Magnets Michael A Green Lawrence Berkeley Laboratory, Berkeley, USA Frank Filthaut.
IR Magnets for SuperKEKB KEK, Norihito Ohuchi 1.IR Magnets (ES, QCS, QC1) 2.Interference between Magnet-Cryostats and Belle 3.Summary SuperB.WS05.Hawaii.
Zachary Wolf Undulator Tuning June 17, 2008 Undulator Tuning Status Z. Wolf, S. Anderson, R. Colon, S. Jansson, S.Kaplunenko,
Yurii Levashov Undula t or fiducialization test Oct. 14, 2004 Undulator Fiducialization Test Results Fiducialization Tolerances.
Isaac Vasserman Magnetic Measurements and Tuning 10/14/ I. Vasserman LCLS Magnetic Measurements and Tuning.
1 Zachary Wolf 1 Undulator Tuning Status June 9, 2009 Undulator Tuning Status Z. Wolf, S. Anderson, R. Colon, S. Jansson, D. Jensen,
1 Status of infrastructure MICE Video Conference, August 17, 2005 Yury Ivanyushenkov Applied Science Division, Engineering and Instrumentation Department.
Zachary Wolf LCLS Undulator October 30, LCLS Undulator Tuning And Fiducialization Zack Wolf, Yurii Levashov, Achim.
A U.S. Department of Energy Office of Science Laboratory Operated by The University of Chicago Argonne National Laboratory Office of Science U.S. Department.
Zachary Wolf Undulator Oct 12, LCLS Undulator Tuning Zack Wolf, Yurii Levashov, Achim Weidemann, Seva Kaplounenko,
Solenoid Magnetic Field Mapping Paul S Miyagawa University of Manchester Objectives Mapper machine Mapper software Simulation Corrections Fitting Future.
Solenoid Magnetic Field Mapping Paul S Miyagawa University of Manchester Introduction Mapper machine Mapper software - Simulation - Corrections - Fitting.
ILC Main Linac Superconducting Cryogen Free Splittable Quadrupole Progress Report V. Kashikhin for Superconducting Magnet Team.
STAR Collaboration Meeting, Nantes, July2002 SVT Analysis/Status Update Jun Takahashi – University of Sao Paulo.
SLHC-PP – WP7 Critical Components for Injector Upgrade Plasma Generator – CERN, DESY, STFC-RAL Linac4 2MHz RF source Thermal Modeling Gas Measurement and.
Spectrometer Solenoid Update Steve Virostek Lawrence Berkeley National Lab Roy Preece Rutherford Appleton Lab October 28, 2011 MICE Collaboration Meeting.
Malte HildebrandtMEG Review Meeting, 14th February 2007 Report of Run Coordinator Run 2006 Summary Malte Hildebrandt MEG Review Meeting, 14th February.
Alignment and Beam Stability
Status of COBRA Magnet Wataru OOTANI MEG review meeting July 11 th, 2003 PSI Switzerland.
Status of the COBRA Magnet Wataru OOTANI MEG review meeting Feb. 3, 2003 PSI Switzerland.
1 W.Ootani ICEPP, University of Tokyo MEG experiment review meeting Feb , PSI W.Ootani ICEPP, University of Tokyo MEG experiment review meeting.
5 September 2006 John Hart RAL ATLAS physics meeting 1 Preliminary Report on Solenoid Mapping Field mapping completed in first week of August Aim to measure.
Experiment beam line installation (9/4/2014) SystemThus FarTo Do Vacuum~ Torr, IP’s on, Vac interlock checkNone Fast valveValve + CCG installed,
BEPCII Prealignment Installation Survey and Alignment Accelerator Center of IHEP Xiaolong Wang
Some Thoughts on Magnetic Measurements for MICE Michael A. Green Lawrence Berkeley Laboratory Berkeley CA 94720, USA.
Forum March 2003H.Taureg1 Magnetic Fields in ALICE Mapping and Monitoring.
Improvement on vertex reconstruction Motivations Many peaks in vertex distributions Further study for the
NIKHEF B-field monitors Paul Balm November 11 th, 1999.
Americas Cavity Specification C.M. Ginsburg (Fermilab) On behalf of the Fermilab cavity crew October 20, 2010.
ATF2 Magnets etc. 1. Magnets 2. Power supplies 3. Magnetic field measurement 4. Movers and supports R. Sugahara May 30, 2005.
Hall D infrastructure and integration Elton Smith Hall D Collaboration Meeting September 9-11, 2004.
X LCLS SCU NbTi Prototype Schedule Version: February 12, 2015 Update 23JUN2015 X X System complete and ready for test X System complete & tested w/Hall.
1 COBRA Magnet Status W.Ootani MEG Experiment Review Meeting, Jul W.Ootani MEG Experiment Review Meeting, Jul
NUMI Update on Steel, Coils, Fixtures, and Prototyping J.K. Nelson 12/98 MINOS Meeting.
A. Baldini PSI July 05 Overview of the experiment MEG is being built (Beam line, Magnet, LXe, DC, TC, Elect., Software) Delays in some items: O(months)
Preliminary result of the target polarization 2004 Kaori Kondo COMPASS target team.
Simulation of heat load at JHF decay pipe and beam dump KEK Yoshinari Hayato.
1 W.Ootani ICEPP, University of Tokyo MEG experiment review meeting Feb , PSI W.Ootani ICEPP, University of Tokyo MEG experiment review meeting.
Haixin Huang AGS Cold Snake: Status and Plans.
26 Aug 2008PC Shield walls – extend the length of channel – will ‘pull’ field x y Coil Centred coil + 2 walls  X – Y asymmetry Off-centre coil +
Physics Requirements Sensitivity to Manufacturing Imperfections Strategy  where to map field  measure deviation from ideal model  fit to error tables.
Status of physics analysis Fabrizio Cei On Behalf of the Physics Analysis Group PSI BVR presentation, February 9, /02/2015Fabrizio Cei1.
CERN –GSI/CEA MM preparation meeting, Magnetic Measurements WP.
201 MHz Cavity Plans Derun Li Center for Beam Physics Lawrence Berkeley National Laboratory February 11, 2011 MAP Friday Video Conference Meeting.
1 Implementation at RAL Iouri Ivaniouchenkov on behalf of Elwyn Baynham, Tom Bradshaw, Tony Jones, Jim Rochford Engineering Department, RAL MICE Collaboration.
24 June 2013 GSI, Darmstadt Helmholtz Institut Mainz Bertalan Feher, PANDA EMP First Measurements for a Superconducting Shield for the PANDA Polarized.
FC Status CM39 1/20 June 2014 OXFORDRALDARESBURY V. BlackmoreV. BaylissT. Hartnett J. CobbT. BradshawS. Griffiths W. LauM. CourtholdI. Mullacrane R. PreeceA.
704 MHz cavity design based on 704MHZ_v7.stp C. Pai
Magnetic Field Mapping
Status of the CLIC DR wiggler design and production at BINP
AEGIS Magnet System.
Beam-beam effects in eRHIC and MeRHIC
Vertex Detector Mechanical R&D Design Questions and Issues
Magnetic Measurements For The LCLS Undulator System
Spectrometer Solenoid Fabrication Status and Schedule
HRS at small angles for e+/ e- pair for APEX
Alignment of the first two magnet system modules of Wendelstein 7-X
Bubble Chamber – Beam Requirements
PERMANENT MAGNET QUADRUPOLE FOR THE LINAC 4 CCDTL
Undulator Tuning Status
Heinz-Dieter Nuhn – LCLS Undulator Group Leader May 14, 2009
LCLS Undulator Tuning And Fiducialization
8-T Solenoid Package and Local Magnetic Shielding in FRIB Cryomodules
SR Update for JLEIC June 8, 2017
Presentation transcript:

COBRA Magnet Status W. Ootani June 27th, 2006 MEG Review W. Ootani June 27th, 2006 MEG Review

Field Measurement Final field measurement was done in February as scheduled. Measurement summary COBRA field I SC =360A I NC =320A |z|<110cm Δz=2cm, -4cm<R<+29cm ΔR=2cm, 0°<φ<+330° Δφ=30° points BTS fringe field I BTS =200A (unlike polarity) -110cm<z<0cm Δz=2cm, -4cm<R<+29cm ΔR=2cm, 0°<φ<+330° Δφ=30° points Field stability measurement with NMR 2

COBRA Field Stability Stability of the COBRA field was measured over a week with NMR at the magic point. COBRA field is stable within <20ppm. 3 Homegeneity (calculation) ~20ppm Hall probe

COBRA Field Map We are finishing the analysis. Measured data Correction for Hall-sensor readout Absolute calibration Temperature compensation Planar Hall effect Correction with the measured position of measuring machine center. Interpolation bw/ measuring points by means of bspline surface fitting. Calculation Detailed coil modeling Thermal expansion at low temperature (~-0.4%) 4

COBRA Field Map, cont’d Comparison with calculation to check the validity of the measurement The measured field is in agreement with the calculation within 0.22%(σ) all over the volume. Center of field difference distribution ~ 0 Not a random deviation Difficult to judge which is right. Possible usage Measured data for |z|<1100mm R<290mm and calculation for the other regions. Measured field map at φ=0 after surface fitting R Z B 5

Grounding scheme of COBRA system Quench Problem There were frequent quenches in the COBRA magnet. We found that it is caused by the external noise on the input signal line of the quench detector. It seems that they happen mostly at the beg. and the end of the working time. Modified shielding and grounding scheme are being tried. No quench for the past three weeks, but with zero coil current. Looking for the noise source in parallel. No irregularity found in primary power. Noise Quench detector signal 6

Fringe Field Problem A dramatic reduction of beam rate was found in πM3 beam line last month when the COBRA ON. Reduction: GPS, LTF Transverse component causes diffraction of the beam. There is an effect also at πE3 beam line, but it’s not serious once the field is stabilized. Possible πM3 Shielding on beam pipe with high-μ material Installation of Parmalloy sheet ( t 0.5mm, μ =180000) was done last week. Shielding factor ~400 is expected. Retune the beam line Add horizontal steering magnet Soft iron wall bw/ πM3 and πE5 The effect is being calculated. 7

Shielding with high permeability material (Permalloy μ=180000) was done in the πM3 beam line last week. The effect was measured on Jun. 26th. No shieldingShielding Shielding+quic k tuning GPS70%~100% LTF5%50%75-80% Fringe Field Problem, Cont’d 8 Roll of Permalloy sheet πM3 beam line with Permalloy sheet Some more room to improve by further tuning. Final tuning will be done in our next beam time. (~end. Aug.)