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Overview installation of Polarized Target . 0.- Hydrogen Target Length 1 .- Polarized target tests 2.- Rail System for ‘Frozen Spin’ mode 3.- CB Frame / Electronics 4.- Schedule. 14 th Crystal Ball Meeting Edinburgh September 13.-15. 2009 Andreas Thomas. - PowerPoint PPT Presentation
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14th Crystal Ball MeetingEdinburgh
September 13.-15. 2009Andreas Thomas
Overview installation of Polarized Target
0.- Hydrogen Target Length
1.- Polarized target tests
2.- Rail System for ‘Frozen Spin’ mode
3.- CB Frame / Electronics
4.- Schedule
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 standard10 cm cell 100.0 +- 1.0 mm High luminosity
He3/He4 Roots4000m3/h
Vacuum system
Mikrowaves70GHz
Dynamic Nuclear
Polarization
NMR-Apparatus
106MHz
Polarisation meas.
Components of the polarized target
for the Crystal Ball detector
Horizontal He3/He4 Dilutionrefrigerator
(20mKelvin)with internalHolding coil
SuperconductingPolarization magnet
5Tesla
TargetmaterialH-ButanolD-Butanol
· Current leads (46A): Copper T=300K 70 KHTc Supracond. T= 70K 4 KNbTi 200mm T= 4K 1.5K
Internal
Holding coil
1.3Kelvin
??? Tesla at 46AL=136mm, d=48mm, 4 layersSupport Copper-tube d=0.3mm
Full test with new insert and butanol target in June – July 2009
Polarizingmagnet
He4(liq)
Start
Stop
Calibration of the Holding coil field
B0=2.5Tesla
F= 106MHz
Observe shift of NMR-Signal depending onholding coil current
46A ~ 0.895Tesla
B0=2.5Tesla
F= 106MHz
Internal transverse Holding coil
Coil tested at 4.2KHenry OrtegaStarted PhD in Mainz
Different layers areused tooptimize thehomogeniety.
Simulation
• “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).
Ideal case for dipole magnet:
cos)(J
150mm
4-layer dipole:N1=N2=138N3=N4=78
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 polarizationwith online NMR during GDH data taking
New NMR [N.Frömmgen]
physETPBP
aNpNaNpN
measE
h
Rail system needed
Cryostat
Polarizingmagnet
Crystal BallPolarization method
1. External magnet 2.5 T2. Polarize with microwaves3. Internal holding coil 0.7 T4. Remove external magnet5. Move CB detector in. 6. Data taking.7. Repolarization
Polarizingmagnet
MicrowavesMicrowaves + NMR
Rail system to Move the CBall, TAPS and Magnet
ACAD railsJ.Rosche
ChassisJ.Ahrens
ElectronicsA.StarostinP.Pedroni
Move magnettransverseA.Thomas
Rails are beeing alignedand fixed:R.KondratievO.Kostikov
Heavy load cars will be mountedby J.Ahrens next week
Electronics has to be mountedpartially on CB frame:A.StarostinA.LapikM. 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.