Overview installation of Polarized Target 14th Crystal Ball Meeting

Slides:



Advertisements
Similar presentations
Measuring the Neutron and 3 He Spin Structure at Low Q 2 Vincent Sulkosky College of William and Mary, Williamsburg VA Experimental Overview The.
Advertisements

G measurement at Ken Livingston, University of Glasgow, Scotland Slides from: Ken Livingston: Various talks at -
Rory Miskimen University of Massachusetts, Amherst
HIGS Frozen Spin Target System (HIFROST) Pil-Neyo Seo University of Virginia Triangle Universities Nuclear Laboratory (TUNL) PSTP International Workshop,
Spin Filtering Studies at COSY and AD Alexander Nass for the collaboration University of Erlangen-Nürnberg SPIN 2008, Charlottesville,VA,USA, October 8,
A polarized solid state target for photon induced double polarization experiments at ELSA H. Dutz TR16 Bommerholz Hartmut Dutz, S. Goertz, A.
Mauricio Martínez Fabregate Dubrovnik, April 8th 2008 Crystal Ball Meeting 7th -9th April, Dubrovnik Status of the Mainz Frozen Spin Target Institut für.
HD group LEPS RCNP C. Morisaki. ① Development of NMR measurement system for the polarized HD target ② Development of single crystal HD target.
Institut für Kernphysik Bosen th August 2010 Andreas Thomas Polarised Targets for Photoproduction Experiments.
R. D. Foster, C. R. Gould, D. G. Haase, J. H. Kelley, D. M. Markoff, (North Carolina State University and TUNL), W. Tornow (Duke University and TUNL) Supported.
N. Doshita, Yamagata Univ.1 The COMPASS polarized target for Drell-Yan physics Drell-Yan physics Informal International Workshop on Drell-Yan physics.
Status of the Polarized 3He Target
16th Crystal Ball Meeting October, 11-13, 2010, Dubrovnik Grigory Gurevich, Yuri Usov Dubna-Mainz Dilution Cryostat of the New Frozen-Spin Target.
Solid Polarized Target Opportunities at JLab Possibilities for Future Experiments.
Transversal Target Asymmetries in Threshold
Crystal Ball Experiment at MAMI Recent Results W.J. Briscoe for the A2 Collaboration (thanks for the sabbatical support) MESONS 2010 SFB443.
Future activities of the COMPASS polarized target N. Doshita University of Bochum, Germany.
Recoil Polarimetry in Meson Photoproduction at MAMI Mark Sikora, Derek Glazier, Dan Watts School of Physics, University of Edinburgh, UK Introduction The.
WBS1 SBS Basic: Magnet and Infrastructure Robin Wines 11/4/ SBS DOE Review.
Y. Kisselev PST05 conference Nov 05 1 PST05 Conference Microwave cavity for large COMPASS polarized target By: Y. Kisselev, J. Ball, G. Baum, N.
Mitglied der Helmholtz-Gemeinschaft Petersburg Nuclear Physics Institute, Russia Storage cells for internal experiments with Atomic Beam Source at the.
Hall B Cryogenics CLAS and CLAS12 David Kashy Hall B Lead Engineer May 26, 2010.
Motivation Polarized 3 He gas target Solenoid design and test 3 He feasibility test Summary and outlook Johannes Gutenberg-Universit ä t Mainz Institut.
SCU Segmented Cryostat Concept M. Leitner, S. Prestemon, D. Arbelaez, S. Myers September 2 nd, 2014.
HD target.
Thomas Roser Snowmass 2001 June 30 - July 21, 2001 Polarized Proton Acceleration and Collisions Spin dynamics and Siberian Snakes Polarized proton acceleration.
October 4-5, Electron Lens Beam Physics Overview Yun Luo for RHIC e-lens team October 4-5, 2010 Electron Lens.
Forum March 2003H.Taureg1 Magnetic Fields in ALICE Mapping and Monitoring.
KEK Hiroshi Yamaoka Task list for Magnet/Iron yoke Solenoid magnet Iron yoke Experimental hall and other facilities May 11, ’05.
The FROST Experiment Franz Klein for the g9 (FROST) run group CLAS Collaboration Meeting/CLAS12 Workshop Paris 2011.
Analysis of the Ammonia Target Polarization Kangkang L. Kovacs, Physics Department, University of Virginia, Charlottesville, VA
9 th Crystal Ball Meeting Basel October Andreas Thomas Transversely Polarized Target 1.-Possible Physics Experiments 2.-Frozen Spin Target 3.-Technical.
1 G9a -FROST. 2 Experiments FROST New generation of CLAS photoproduction experiments with FROzen Spin Polarized Target (FROST) E02-112: γp→KY (K + Λ,
Status of the Crystal Ball A.Starostin UCLA. Tasks in preparation for the polarized target experiments CB and the “cube” will be movable on rails – all.
CONSTRUCTION AND TEST OF A TRANSVERSE SUPERCONDUCTING HOLDING MAGNET 15th CB Meeting Mainz March 8th, 2010 Henry G. Ortega Spina.
Transversity Readiness and Timeline Xiaodong Jiang, March 17th, This document specifies the overall readiness for Hall A experiments E06-010/E
Recent Developments in Polarized Solid Targets H. Dutz, S. Goertz Physics Institute, University Bonn J. Heckmann, C. Hess, W. Meyer, E. Radke, G. Reicherz.
COMPASS polarized target for Drell-Yan Michael Pesek Charles University in Prague On behalf of COMPASS PT group PSPT, Charlottesville, Virginia
A First Analysis of the 3 He Test Beamtime CB Meeting Mainz, March 9, 2010 Patricia Aguar Bartolomé Alexander Mushkarenkov.
The Polarized Internal Target at ANKE: First Results Kirill Grigoryev Institut für Kernphysik, Forschungszentrum Jülich PhD student from Petersburg Nuclear.
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.
17th Crystal Ball Meeting
The Polarized Internal Gas Target of ANKE at COSY
Mapping the Magnetic Field of the ATLAS Solenoid Paul S Miyagawa University of Manchester ATLAS experiment + solenoid Objectives Field mapping machine.
Preliminary result of the target polarization 2004 Kaori Kondo COMPASS target team.
Future Perspectives of the Bonn Polarized Target Since the mid 1980‘s: Bonn is a place of excellence in the field of polarized solid targets ! Still valid.
Analysis of    production ► Data taking ► Reaction identification ► Results for double polarization observable F ► Summary Based on data taken in the.
24 June 2013 GSI, Darmstadt Helmholtz Institut Mainz Bertalan Feher, PANDA EMP First Measurements for a Superconducting Shield for the PANDA Polarized.
CLAS12 Longitudinally Polarized Target R&D Update CLAS Collaboration, October 20, 2015 Chris Keith.
Study of a Superconducting Shield for a Transverse Polarized Target for PANDA 2012 Paris Helmholtz Institut Mainz Bertalan Feher, PANDA EMP Session Status.
Status of Polarimeters and Polarized Targets: what are the plans for development of polarized targets to meet the needs of the Day 1 and future experimental.
Initial Tests of the JLab Frozen Spin Target Chris Keith Target Group Jefferson Lab September 13, 2007 Brookhaven National Lab.
Dipole Magnetic Field Effect on the Antiproton Beam
Yingshun Zhu Design progress of QD0 in CEPC Interaction Region
Future Physics at HERMES
AEGIS Magnet System.
The CMS magnet superconducting coil
Polarized Target Activity at the University of Virginia
Test of Optical Stochastic Cooling in CESR
Status of the AGATA installation at GANIL
Polarized solid Targets for AFTER
INFN-Sezione di Pavia, Italy
NMR system for the frozen spin target to measure the polarisation
OT Survey & Adjustment Outline: Survey technique at present
I Alexander Nass for the JEDI collaboration
ACCELERATORS AND DETECTORS
Hall D Cryogenic requirements
as a prototype for Super c-tau factory
Main Design Parameters RHIC Magnets for MEIC Ion Collider Ring
Polarized 3He target installation
Presentation transcript:

Overview installation of Polarized Target 14th Crystal Ball Meeting 0.- Hydrogen Target Length 1.- Polarized target tests 2.- Rail System for ‘Frozen Spin’ mode 3.- CB Frame / Electronics 4.- Schedule 14th Crystal Ball Meeting Edinburgh September 13.-15. 2009 Andreas Thomas

Note: Hydrogen Target Length New Xray picture of 30mm cell at 9.9.09 [R.Kondratiev, O.Kostikov, A.Thomas] Results: 3 cm cell 30.2 +- 0.3 mm h - Bump 5 cm cell 47.2 +- 0.5 mm standard 10 cm cell 100.0 +- 1.0 mm High luminosity

Components of the polarized target for the Crystal Ball detector He3/He4 Roots 4000m3/h Vacuum system Components of the polarized target for the Crystal Ball detector Targetmaterial H-Butanol D-Butanol Mikrowaves 70GHz Dynamic Nuclear Polarization Superconducting Polarization magnet 5Tesla NMR-Apparatus 106MHz Polarisation meas. Horizontal He3/He4 Dilutionrefrigerator (20mKelvin) with internal Holding coil

Internal Holding coil · Current leads (46A): Copper T=300K  70 K HTc Supracond. T= 70K  4 K NbTi 200mm T= 4K  1.5K Internal Holding coil 1.3Kelvin ??? Tesla at 46A L=136mm, d=48mm, 4 layers Support Copper-tube d=0.3mm

Full test with new insert and butanol target in June – July 2009

Polarizing magnet He4(liq)

Start

Stop

Calibration of the Holding coil field B0=2.5Tesla F= 106MHz Observe shift of NMR-Signal depending on holding coil current

B0=2.5Tesla F= 106MHz 46A ~ 0.895Tesla

Internal transverse Holding coil Coil tested at 4.2K Henry Ortega Started PhD in Mainz Different layers are used to optimize the homogeniety.

Simulation Ideal case for dipole magnet: “Racetrack” coil: magnetic field highly non-uniform and not appropriate for a cylinder. “Saddle” coil: winding must fit to the so-called overlapping ellipse or “cosine” shape of current distribution (Wilson 2002 & Ašner 1999).

4-layer dipole: N1=N2=138 N3=N4=78 150mm

High Field Solenoid or Transverse Field

The degree of polarization PT of the target protons (run in May ´98) : Measurement of the degree of proton polarization with online NMR during GDH data taking New NMR  [N.Frömmgen]

Polarization method Crystal Ball Cryostat Polarizing magnet Polarizing Rail system needed Microwaves + NMR Microwaves Polarizing magnet Polarizing magnet External magnet 2.5 T Polarize with microwaves Internal holding coil 0.7 T Remove external magnet Move CB detector in. Data taking. Repolarization

Rail system to Move the CBall, TAPS and Magnet ACAD rails J.Rosche Chassis J.Ahrens Electronics A.Starostin P.Pedroni Move magnet transverse A.Thomas

Rails are beeing aligned and fixed: R.Kondratiev O.Kostikov

Heavy load cars will be mounted by J.Ahrens next week

Electronics has to be mounted partially on CB frame: A.Starostin A.Lapik M. Korolija

Schedule 1.- Polarized Target - tests in dilution mode reproduced successfully - transverse coil tested at 4K - DNP measured - Colleagues from Dubna in Mainz Nov.-Dec. 2.- Rail system for CBall - Cables dismounted, Rails beeing aligned now - First move of CB next week - DAPHNE in storage hall, TOF detectors? - Installation of part of electronics in CB-Frame? 3.- Installation of PT in CBall - Start in October - Test beam in December for intensity dependent relaxation time etc. - Transverse or Longitudinal coil.