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.

Slides:



Advertisements
Similar presentations
Paul Soler,8 June 2000 RAL and Univ. of Glasgow ALIGNMENT ISSUES FOR RICH 2.
Advertisements

Field measurements of QEA magnets at KEK Mika Masuzawa May 30, 2006.
The MICE Target Lara Howlett University of Sheffield.
Results of the ATLAS Solenoid Magnetic Field Map
TPC status Marian Ivanov. Outlook TPC performance ExB correction Alignment Nonlinearities and edge effects Drift velocity calibration.
Integrating a Short Range Laser Probe with a 6-DOF Vertical Robot Arm and a Rotary Table Theodor Borangiu Anamaria Dogar
CM-18 June The Measurement and Monitoring of the Field from the MICE Magnets Michael A Green Lawrence Berkeley Laboratory, Berkeley, USA Frank Filthaut.
29 June 2004Paul Dauncey1 ECAL Readout Tests Paul Dauncey For the CALICE-UK electronics group A. Baird, D. Bowerman, P. Dauncey, C. Fry, R. Halsall, M.
Zachary Wolf Undulator Tuning June 17, 2008 Undulator Tuning Status Z. Wolf, S. Anderson, R. Colon, S. Jansson, S.Kaplunenko,
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,
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.
Realistic Model of the Solenoid Magnetic Field Paul S Miyagawa, Steve Snow University of Manchester Objectives Closed-loop model Field calculation corrections.
Zachary Wolf LCLS Undulator October 30, LCLS Undulator Tuning And Fiducialization Zack Wolf, Yurii Levashov, Achim.
Update Hardware for conductive cooling of the quench resistors has been fabricated at LBNL. Preparation for installation to start this week. Installation.
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.
Coil Manufacture, Assembly and Magnetic Calibration Facility for Warm and Cold Magnetic Measurements of LHC Superconducting Magnets CERN AT-MTM 1 / 21.
MICE magnetic measurements Sequence of events and MICE hall movements Alain Blondel – 10-April 2012 revision from 13 December 2012.
Page 1 Christian Grefe, DESY FLC Status of PCMAG fieldmapping analysis Annual EUDET Meeting Paris, Status of PCMAG fieldmapping analysis Christian.
ATLAS: SCT detector alignment and B field map. Steve Snow New Year 2005 This title describes work that has been growing from low priority at the start.
A year of ATLAS preparation. Steve Snow New Year 2006 The resolution of tracks reconstructed in ATLAS ID should be: Good enough for some physics from the.
Offline Data Analysis Software Steve Snow, Paul S Miyagawa (University of Manchester) John Hart (Rutherford Appleton Laboratory) Objectives + requirements.
Offline Data Analysis Software Steve Snow, Paul S Miyagawa (University of Manchester) John Hart (Rutherford Appleton Laboratory) Objectives + requirements.
23 July 2012D. Sober1 Some thoughts on Hall D tagger magnet field mapping D. Sober Catholic University of America GlueX Beam/Tagger biweekly meeting 23.
22 July 2008 John Hart Toroid Field Parameterisation 1 Toroid Field Parameterisation An informal report to the RAL ATLAS meeting John Hart 22 July 2008.
14 August Magnetic Field in the ATLAS Muon Spectrometer Masahiro Morii for the ATLAS Group Harvard University Laboratory for Particle Physics and.
ATLAS Inner Detector Magnetic Field I am responsible for providing the magnetic field map for the ATLAS Inner Detector.  6m long x 2m diameter cylindrical.
Lecture 12 Magnetic Force on a Current Torque on a Current Loop Motion of Charged Particle in a Magnetic Field Magnetic Field of a Wire.
Wind Test Plan ●Test individual components, system in different conditions ●Calculate expected power under various conditions Wind block diagram.
Some Thoughts on Magnetic Measurements for MICE Michael A. Green Lawrence Berkeley Laboratory Berkeley CA 94720, USA.
MICE magnetic measurements: AFC considerations Alain Blondel see a previous discussion for reference in CM35 (Feb 2013 slides by V. Blackmore, A. Blondel.
Forum March 2003H.Taureg1 Magnetic Fields in ALICE Mapping and Monitoring.
1 Zero Point Correction. 2 Basic Steps - I For a given site on a given day: 1.Create a magnetic flat field from the east & west calibration images. 2.Using.
COBRA Magnet Status W. Ootani June 27th, 2006 MEG Review W. Ootani June 27th, 2006 MEG Review.
4 th Workshop on ALICE Installation and Commissioning January 16 th & 17 th, CERN Muon Tracking (MUON_TRK, MCH, MTRK) Conclusion of the first ALICE COSMIC.
CHANTI update F. Ambrosino, T. Capussela, D. Di Filippo, P. Massarotti, M. Mirra, M. Napolitano, L. Roscilli, G. Saracino.
EPICS EPICS Collaboration Meeting Argonne National Laboratory drvTS improvements for soft timing EPICS Collaboration Meeting Argonne National Laboratory.
NIKHEF B-field monitors Paul Balm November 11 th, 1999.
H.TauregTechnical Forum June B and T monitoring News on B field mapping B field monitoring Temperature monitoring.
Solenoid map access in athena Paul S Miyagawa, Steve Snow University of Manchester.
Christian Grefe April 15,  Measured Data ◦ Correct for global position and orientation ◦ Correct for 24 hall probe positions and orientations ◦
M. Ellis - MICE Collaboration Meeting - Thursday 28th October Sci-Fi Tracker Performance Software Status –RF background simulation –Beam simulation.
Helical Undulator Status Jim Clarke ASTeC, STFC Daresbury Laboratory.
3.The residual B r on the cylindrical surface is represented by multipole terms The results from the combined geometrical + general Maxwell fit show that.
3.The residual B r on the cylindrical surface is represented by multipole terms The results from the combined geometrical + general Maxwell fit show that.
Force Sensing in SB2’s Wings Anna-Katrina Shedletsky BDML Friday, August 24, 2007.
Mapping the Magnetic Field of the ATLAS Solenoid Paul S Miyagawa University of Manchester ATLAS experiment + solenoid Objectives Field mapping machine.
JRA1 PCMAG field mapping Elements of the work: Hall sensors: improvements and production Calibration of Hall sensor cards Mechanical mapping device Installation.
Spectrometer Solenoid Field Mapping: Thoughts on Mapping Analysis & Results Major caveat: Everything in this talk is highly preliminary Data arrived on.
Status of physics analysis Fabrizio Cei On Behalf of the Physics Analysis Group PSI BVR presentation, February 9, /02/2015Fabrizio Cei1.
PIXEL ladder alignment Hidemitsu ASANO. Photo analysis & survey beam data (with zero magnetic field) ① SVX standalone tracking Global Tracking Strategy.
Beam dynamics simulations with the measured SPARC gun- solenoid field G. Bazzano, P. Musumeci, L. Picardi, M. Preger, M. Quattromini, C. Ronsivalle, J.
CERN –GSI/CEA MM preparation meeting, Magnetic Measurements WP.
X axis y axis Points on a coordinate plane are written like this: (-8, 9) Move the dot.
FIELD MAPPING V. Blackmore CM38 23rd February /70.
Final Results for the Solenoid Magnetic Field Map CERN mapping project team Martin Aleksa, Felix Bergsma, Laurent Chevalier, Pierre-Ange Giudici, Antoine.
Performance of B-sensor types EUDET NIKHEF VS F. Bergsma 12/9/2007.
MAGNET MAPPING J. Cobb V. Blackmore (not responsible for the content of this talk) 27 September 2017.
Re-mapping the Residual B-Field in NA62
Motivation We would like to be able to scale the SHMS Golden Tune we determine this Fall from 2.2 GeV/c to other momenta with linearity errors less than.
Status of the dipole magnetic field analysis
Feng Zhou LCLS-II AP meeting 02/23/2017
Magnetic Measurements For The LCLS Undulator System
Pulser Tests at the A0PI Mark Palmer and Bob Meller Cornell University
Problems with the Run4 Preliminary Phi->KK Analysis
Undulator Tuning Status
LCLS Undulator Tuning And Fiducialization
Presentation transcript:

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 field to 1 in 2000 (10 G in 2 T) “Windmill” measuring machine with 4 arms Driven by pneumatic motors 12 Hall probes on each arm 5 NMR probes, 4 permanent and one on machine Field measured at 4 currents: 5000, 7000, 7730, 7850 A (twice at 7730 A) Analysis at Manchester (Steve Snow and Paul Miyagawa), RAL (JCH) and CERN (Heidi Sandaker)

5 September 2006 John Hart RAL ATLAS physics meeting 2 Field Measuring Machine … undergoing tests in laboratory Carriage Hall probes mounted on 4 windmill arms Rails Driven by pneumatic motors Measurements scheduled for July/August

5 September 2006 John Hart RAL ATLAS physics meeting 3 Notes on the field mapping Mapping originally scheduled for February, but slippage gave time for work on measuring machine and software Accident after machine installed in solenoid necessitated re-survey and replacement of a few probes 2 weeks set aside for measurement but further delays from cryogenics, CERN power failure … Central NMR planned for normalisation failed Normalise to average of Hall probes Probe calibration to ~1 G up to 1.5 T but only ~10 G at higher fields Hysteresis minimal, not more than a few gauss difference in cycling field Solenoid current stable to within less than 0.1 A Some problem with machine jamming near ends of solenoid Aimed for a series of coarse scans rather than a few fine scans

5 September 2006 John Hart RAL ATLAS physics meeting 4 Points measured at 7730 A

5 September 2006 John Hart RAL ATLAS physics meeting 5 Analysis of the mapping data Measuring machine output converted to Bz, Br and Bphi (including temperature correction) using calibration results Need to correct for probe alignment errors (~1 mrad) and normalisation Apply corrections from survey measurements including measuring arm axis directions Further corrections for exact probe positions, skew in carriage positioning, … Check consistency of the measurements Combine data and perform geometrical or Fourier-Bessel fit Generate field map for ATLAS analysis

5 September 2006 John Hart RAL ATLAS physics meeting 6 Plane zero scans Measuring machine positioned so that each arm in turn is at z=0 and measurements made for 16 values of phi. Possible to check agreement between corresponding probes on each arm After corrections, differences are less than 5 G, often less than 2 G Scan data from 2 August but probe alignments from 7 August, so evidence for stability in alignments. Axis alignments from data (relative to field axis) agree with survey measurements (in IWV coordinates), so conclude field is parallel with IWV axis (to within ~0.2 mrad)

5 September 2006 John Hart RAL ATLAS physics meeting 7 Plane zero scans Br for outermost probes (12,24,36 & 48) versus phi

5 September 2006 John Hart RAL ATLAS physics meeting 8 Plane zero scans Bphi for outermost probes (12,24,36 & 48) versus phi

5 September 2006 John Hart RAL ATLAS physics meeting 9 Plane zero scans |B| for outermost probes (12,24,36 & 48) versus phi - structure not expected from “realistic” model

5 September 2006 John Hart RAL ATLAS physics meeting 10 Fine scan in phi Bphi for 3 outermost probes on arm 3 versus phi – after subtraction of return conductor field

5 September 2006 John Hart RAL ATLAS physics meeting 11 Plans Continue checks on consistency of measurements: between measurements (including different probes and different currents) with Maxwell’s equations (using Fourier Bessel fits) with geometrical model Develop software to process measurements on unequally spaced z planes Combine measurements and make a best fit (or fits) to the field Generate a field map for ATLAS physics

5 September 2006 John Hart RAL ATLAS physics meeting 12 Conclusions The field mapping was completed successfully despite various difficulties Preliminary results indicate that a field map accurate to 1 in 2000 is possible Further work is required to understand the measured field and generate the map