Handbook OPTIFLEX 1300 C - Max-Planck-Institut für Kernphysik
Institut für Kernphysik
-
Upload
rafael-craig -
Category
Documents
-
view
27 -
download
5
description
Transcript of Institut für Kernphysik
Institut für Kernphysik
17th Crystal Ball MeetingMainz, February 28th, 2011
Andreas Thomas
Frozen Spin Target
1.- Polarised Target Operation
2.- Short Term Plans
3.- Modifications
4.- Long term plans
Operation
MovableCrystal Ball
4-Photon
Detector
Cryostat
Movable5Tesla
PolarisingMagnet
First Beam with Transverse Polarisation started 15th December 2009.In 2010 we had more than 2000 hours beam on this target.
Cryostat Performance
Temperature stability: T ~ +- 0.2mKelvin (one day) (typical one week measurement period).
T=24mK
T=27mK
T=29mK
t=40h
Frozen Spin Target Relaxationtime
....),,,( eTemperaturFieldBRadicalMaterial
0,2 0,3 0,4 0,5 0,6 0,7 0,8
0
200
400
600
800
1000
1200
1400
1600
rela
xatio
n tim
e [h
]
holding field [T]
Relaxation time of butanol at 60 mK depending on the applied magnetic field
t
ePP
0
26 mK, 0.44T
410#
# protons
radicals
Free electrons Radicals in material by chemical or radiative doping
Saturated electrons of target material not polarized (Pauli principle)
Butanol
HHHH
HOCCCCH
HHHH
N
O
CH3
CH3CH3
CH3
Tempo
Target material
Dilution factor (fButanol=10/74)determines quality of target material.
We have 9*1022 pol. Protons per cm2 in our2cm long target cell.
2cm
Filling factor ~ 60% H. Ortega Spina
Vacuum
C4H10O – 60%30mm
3He/4He – 6%
X-ray picture withBeamspot andNMR coil fromlast week.
Soldering of the NMR coil (target material has to be keptunder liq. Nitrogen) and installation into the cryostat.
Degree of Polarisation
B=0T B=2.5T
NMR System for Polarisation measurement
MHzp 106
Typical NMR Signals
Thermal Equilibrium-Signal0.5% Polarisation2.5Tesla,1Kelvin
Enhanced Signal at 70% Polarisationafter spin rotation
TE
dynTEdyn AU
AUPP
Temperature measurement
AVS Picowatt Resistance Bridge
kT
BP
tanh
! Systematic error for all asymmetries!
[Gerhard Reicherz, PT Ruhr-Universität Bochum,Next talk]
D-Butanol
Target materialDensity and species of the radicals
are very important for:•maximum degree of polarization
•polarization build up times•relaxation timesTrityl-Radikal
Highest Deuteron polarisation due to new doping material with narrow ESR from Bochum.
Deuteron NMR Signals
Proposal:
•Beam for 3 weeks in April (proton target optimized for and )
•Beam for 2 weeks in May (deuteron target broad band at 1557MeV)
•Dismounting Cryostat after final test (TE-calibration, filling factor…)
•Mounting of EPTagger.
•Mounting of liquid hydrogen target (cell length 3cm or 5cm or 10cm?).
•Test beamtime end of summer/fall.
Short term plans
Transverse (Saddle coil)
and
Longitudinal (Solenoid)
Internal
Holding Field (1.2K, 0.6T)
Modifications: Magnet TechnologyDNP at 200mK and 2.5T with 70GHz microwaves.Frozen spin target (25mKelvin, 0.6T).Secondary particles punch through holding coil.All directions of polarization.
High Field 1T
Threshold Production
Transverse Field
Modifications: Internal Polarising Coil
DNP at 200mK and 2.5T with 70GHz microwaves.10Layer coil at 50A.Secondary particles punch through holding coil.Higher momentum threshold.
Problem is the required field homogenietyof 10-E4. Notched solenoid.3d finite element calculation, optimisationand precise production needed.
New Coil with 10 layer (2.5Tesla) inMainz mechanical workshop.
Talk S.Schrauf
Vacuum 3He/4He – 6%
Modifications: Active Polarised Target
•Change from transverse to longitudinal polarisation.
•Internal polarising coil for high luminosity and precission experiments.
•Active polarised target for treshhold experiments.
Long term plans