first experiments with the polarized internal gas target (pit) at anke/cosy
DESCRIPTION
Ralf Engels for the ANKE-Collaboration Institut für Kernphysik, Forschungszentrum Jülich. First Experiments with the Polarized Internal Gas Target (PIT) at ANKE/COSY. Brookhaven September 14, 2007. Outline. Introduction PIT installation Setup overview - PowerPoint PPT PresentationTRANSCRIPT
First Experiments with the Polarized Internal Gas Target (PIT)
at ANKECOSY
Ralf Engels for the ANKE-Collaboration
Institut fuumlr Kernphysik Forschungszentrum Juumllich
Brookhaven
September 14 2007
September 14 2007 Ralf Engels 2
Outline
Introduction PIT installation
Setup overview Transfer to COSY hall and installation at ANKE
PIT commissioning Stray fields at ANKE Cell tests at ANKE Target commissioning Results
Plans for the future
September 14 2007 Ralf Engels 3
bull internal experiments ndash with the circulating beam bull external experiments ndash with the extracted beam
p p d dwith momenta up to 37 GeVc
COSY ndash COoler SYnchrotron
September 14 2007 Ralf Engels 4
ANKE at COSY
Targetsbull Solid stripbull Cluster jetbull Polarized internal target PIT ( storage cell or jet )
Magnetsbull D2 ndash spectrometer magnetbull D1 D3 ndash beam bending magnets
Detector systemsbull Positive amp Negativebull Forward amp Backwardbull Spectator Detectors
Spectrometer ANKE
September 14 2007 Ralf Engels 5
PIT at ANKE
3D CAD drawing of PIT at ANKE
Storage cellPolarimeter
ABS
Technical constraints
bull Target exchange within a maintenance week
bull New support bridge following the movement of D2 magnet
bull Magnetic shielding of componentsbull of the Atomic Beam Source (ABS)bull (D2 Magnet 16 Tesla)
September 14 2007 Ralf Engels 6
Polarized Internal Gas Target
Main parts of a PITbull Atomic Beam Source
bull Target gas
hydrogen or deuteriumbull H beam intensity (2 hyperfine states)
76 1016 atoms sbull Beam size at the interaction point
σ = 285 plusmn 042 mmbull Polarization for hydrogen atoms
PZ = 089 plusmn 001
PZ = -096 plusmn 001
bull Lamb-Shift Polarimeterbull Target chamber with Storage Cell
ABS and LSP at the laboratory
September 14 2007 Ralf Engels 7
The Lamb-shift Polarimeter
September 14 2007 Ralf Engels 8
The Molecules in the ABS jet
I H 2
+
I H 2
+
+ c middot I p
= 0029 plusmn 0002
Engels et al RSI 76 053305 (2005)
September 14 2007 Ralf Engels 9
ABS and LSP in the COSY hall
December 2004 ndash transfer to COSY hall (outside of the COSY tunnel)
May 2005 ndash tests after reassembling
Setup in the COSY hall
bull Supports representing
D1 and D2
bull New support bridge
bull Platform for all electronic and supply components
bull Heat exchanger with closed cooling-water circuit
June 2005 ndash setup ready
for installation at ANKE
September 14 2007 Ralf Engels 10
PIT installation at ANKE
Platform transportationABS transportation
September 14 2007 Ralf Engels 11
PIT at ANKE
September 14 2007 Ralf Engels 12
Magnetic stray field of D2
PIT setup with shielded components at ANKE
x
y
z
90150135
61530
302555
4026300
200550300
60100300
303355
calculated field strength (G)measured field strength (G)permissible field strength for the device given by the producer (G)
September 14 2007 Ralf Engels 13
Test of the medium-field rf transition unit
0 0 E + 0 0
5 0 E - 0 8
1 0 E - 0 7
1 5 E - 0 7
2 0 E - 0 7
2 5 E - 0 7
3 0 E - 0 7
0 200 400 600 800 1000 1200 1400D2 current A
Pre
ssu
re i
n t
he
targ
et c
ham
ber
e-7
mb
ar
H beam OFF H beam ON states 1 + 2 H beam ON state 1 only
30
25
20
15
10
05
00
field strength in the D2 gap0 T 158 T
0 0 E + 0 0
5 0 E - 0 8
1 0 E - 0 7
1 5 E - 0 7
2 0 E - 0 7
2 5 E - 0 7
3 0 E - 0 7
0 200 400 600 800 1000 1200 1400D2 current A
Pre
ssu
re i
n t
he
targ
et c
ham
ber
e-7
mb
ar
H beam OFF H beam ON states 1 + 2 H beam ON state 1 only
30
25
20
15
10
05
00
field strength in the D2 gap0 T 158 T
no ABS beam
MFT off (HFS 1 and 2)
MFT on (HFS 1 only)
September 14 2007 Ralf Engels 14
Do we have a zero field crossing
Magnetic field scan with ANKE at 53ordm using a 3D Hallprobe (Gatchina)
Bx By By |B|
Magnetic field along ABS axisbullID2=563 A (~ 06 T)
bullID1D3=129484 A
1 Determine the local Larmor precession frequency ωL
2 The angular velocity of the magnetic field ωB
As long as the ratio R=ωLωB is large the spin of the atom follows the field directionrarr no depolarization due to zero crossings
ωL
R=ωLωB
ωB
September 14 2007 Ralf Engels 15
Tuning of the Transition Units
Supporting bridge betweenD1 and D2
Additional shielding fromthe D2 stray fields
Cryopump at the target chamber
Polarimeter ionizer underthe target chamber
September 14 2007 Ralf Engels 16
First Polarization Measurement with the LSP
Problems
- The magnetic stray field of the D2 magnet deflected the produced protons
- The quantization axis was rotated by the stray field and the LSP measures
only the projection on the horizontal beam line
Next time More shielding and a rotatable Wien filter to compensate the
misalignment of the polarization axis
WFT was tuned online at the ANKE target position near the D2 magnet
The measured asymetry was stable during the beam time
September 14 2007 Ralf Engels 17
37middot10-840middot10-9With catcher
30middot10-740middot10-9Without catcher
With
ABS jet
Without
ABS jet
ABS beam catcher
~13cm~13cm
Measured pressures in the target chamber mbar
AB
S-j
et d
ensi
ty c
m-3
integral thickness ~ 15 1011 cm-2
ABS jet
COSY Beam
The ABS jet target
September 14 2007 Ralf Engels 18
Storage cell setup
COSYbeam
XY-table Frame with storage cell and aperture
Target chamber
Feeding tube l = 120 mm Oslash = 10 mm
Extraction tube l = 230 mm Oslash = 10 mm
Beam tube l = 400 mm 20x20 mm2
400mm400mm
September 14 2007 Ralf Engels 19
The COSY beam size
at injection
with an accelerated beam
no target with cluster target(density ~ 1014 atcm2)
9x12 mm 16x15 mm
36x16 mm
15 x 15 mm2
September 14 2007 Ralf Engels 20
Storage cell Final setup for the 1 Experiment
Tools for the experiment New storage cell amp support
(20bull20bull390 mm)
gt high target density gt unpolarized gas feeding system
LSP below the target chamber
gt online measurement of the ABS beam polarization
Silicon Tracking Telescope (STT)
gt measurement of spectator protonsnearby the storage cell center
September 14 2007 Ralf Engels 21
Cooler stacking with the storage cell
28 stacks followed by bull 2s electron cooling bull after 58s acceleration toTp=600 MeV
Cooler Stacking allows for higher polarized beam intensities with cell
Without storage cell 25middot1010 ions were reached
September 14 2007 Ralf Engels 22
Results of the cell tests
single injection 3557empty cell
26no cell80 stacking +
electron cooling
flattop
(600 MeV)after
coolinginjection
empty cell
no cell
target
92ordm
0ordm
ΘANKE
30 stacking + electron cooling
83
number of stored protons 10 9
2030 stacking +
electron cooling
1421single injection
injection type
30 stacking + electron cooling92ordm
cell with H gas from ABS
empty cell
64
6
9
September 14 2007 Ralf Engels 23
Storage cell and stochastically cooled beam
Cooling off
Cooling on
Tp= 831 MeV
September 14 2007 Ralf Engels 24
First Experimental Beam Time
Stacking rarr 120 injection with 10 s e-coolingFlat top rarr 30 min to have about 60 duty time
0 20 50Time min
September 14 2007 Ralf Engels 25
First Experimental Beam Time
Stacking rarr 120 injection with 10 s e-coolingFlat top rarr 30 min to have about 23 duty time
0 20 50Time min
Switching on the gasto feed the storage cell
Acceleration withoutgas in the storage cell
7 109 polarized deuterons in the ring with gas in the target
September 14 2007 Ralf Engels 26
Td=12 GeV target H (N2) gas
dprarrdp
dp rarr rarr
First Double Polarized Experiment dp dp rarr rarr
September 14 2007 Ralf Engels 27
First Double Polarized Experiment dp dp rarr rarr
Td=12 GeV target H (N2) gas
dprarr(dpsp) πo
quasi-free nprarrd
πo
(High amp Low branch)
High branch
Low branch
dp rarr rarr
September 14 2007 Ralf Engels 28
First Polarization Measurement of the Target
ANKE
preliminary
dp Td=12 GeV polarized H gas
quasi-free nprarrd
πo
(High amp Low branch)
ltQygt = 075 plusmn 006
θd=50-150 θd=150-220 θd=220-280 θd=280-400
θd=1550-1650 θd=1650-1700 θd=1700-1770
rarr
quasi-free
np rarr dπ0
(High and low branch)
ltQygt = 079 plusmn 007
September 14 2007 Ralf Engels 29
Summary of commissioning and first experiment
1 Cell-target thickness for H (hyperfine state 1) ~ 2 middot 1013 cm-2
3 ABS jet-target thickness ~ 15 middot 1011 cm-2
bull Tests at ANKE with ABS and storage cell
with stacking injection (Nov 2005) and stochastic cooling (Mar 2006)
2 Average luminosity for the storage-cell test ~ 1 middot 1029 cm-2 s-1
4 Hydrogen polarization in the cell ~ 079 +- 007
bull First experiment dprarrppn - JanFeb 2007rarrrarr
September 14 2007 Ralf Engels 30
Plans for the future
December 07 ndash PIT reinstallation With rotatable Wien filter and
better shielding of the LSP
JanFeb rsquo08 ndash Next beam time d prarr (pp)n at 2435 ndash 37 GeVc
(5 Weeks)
March rsquo08 ndash PIT deinstallation
ABS and LSP can be used for other experiments
- ISTC project 1860 Nuclear Polarization in H2D
2 molecules
- Direct Measurements of the Hyperfine levels
in the 2S12
2P12
state rarr Breit-Rabi diagram
rarr rarr
September 14 2007 Ralf Engels 31
Far Future Polarized Fusion
- First Experiments with the Polarized Internal Gas Target (PIT) at ANKECOSY
-
September 14 2007 Ralf Engels 2
Outline
Introduction PIT installation
Setup overview Transfer to COSY hall and installation at ANKE
PIT commissioning Stray fields at ANKE Cell tests at ANKE Target commissioning Results
Plans for the future
September 14 2007 Ralf Engels 3
bull internal experiments ndash with the circulating beam bull external experiments ndash with the extracted beam
p p d dwith momenta up to 37 GeVc
COSY ndash COoler SYnchrotron
September 14 2007 Ralf Engels 4
ANKE at COSY
Targetsbull Solid stripbull Cluster jetbull Polarized internal target PIT ( storage cell or jet )
Magnetsbull D2 ndash spectrometer magnetbull D1 D3 ndash beam bending magnets
Detector systemsbull Positive amp Negativebull Forward amp Backwardbull Spectator Detectors
Spectrometer ANKE
September 14 2007 Ralf Engels 5
PIT at ANKE
3D CAD drawing of PIT at ANKE
Storage cellPolarimeter
ABS
Technical constraints
bull Target exchange within a maintenance week
bull New support bridge following the movement of D2 magnet
bull Magnetic shielding of componentsbull of the Atomic Beam Source (ABS)bull (D2 Magnet 16 Tesla)
September 14 2007 Ralf Engels 6
Polarized Internal Gas Target
Main parts of a PITbull Atomic Beam Source
bull Target gas
hydrogen or deuteriumbull H beam intensity (2 hyperfine states)
76 1016 atoms sbull Beam size at the interaction point
σ = 285 plusmn 042 mmbull Polarization for hydrogen atoms
PZ = 089 plusmn 001
PZ = -096 plusmn 001
bull Lamb-Shift Polarimeterbull Target chamber with Storage Cell
ABS and LSP at the laboratory
September 14 2007 Ralf Engels 7
The Lamb-shift Polarimeter
September 14 2007 Ralf Engels 8
The Molecules in the ABS jet
I H 2
+
I H 2
+
+ c middot I p
= 0029 plusmn 0002
Engels et al RSI 76 053305 (2005)
September 14 2007 Ralf Engels 9
ABS and LSP in the COSY hall
December 2004 ndash transfer to COSY hall (outside of the COSY tunnel)
May 2005 ndash tests after reassembling
Setup in the COSY hall
bull Supports representing
D1 and D2
bull New support bridge
bull Platform for all electronic and supply components
bull Heat exchanger with closed cooling-water circuit
June 2005 ndash setup ready
for installation at ANKE
September 14 2007 Ralf Engels 10
PIT installation at ANKE
Platform transportationABS transportation
September 14 2007 Ralf Engels 11
PIT at ANKE
September 14 2007 Ralf Engels 12
Magnetic stray field of D2
PIT setup with shielded components at ANKE
x
y
z
90150135
61530
302555
4026300
200550300
60100300
303355
calculated field strength (G)measured field strength (G)permissible field strength for the device given by the producer (G)
September 14 2007 Ralf Engels 13
Test of the medium-field rf transition unit
0 0 E + 0 0
5 0 E - 0 8
1 0 E - 0 7
1 5 E - 0 7
2 0 E - 0 7
2 5 E - 0 7
3 0 E - 0 7
0 200 400 600 800 1000 1200 1400D2 current A
Pre
ssu
re i
n t
he
targ
et c
ham
ber
e-7
mb
ar
H beam OFF H beam ON states 1 + 2 H beam ON state 1 only
30
25
20
15
10
05
00
field strength in the D2 gap0 T 158 T
0 0 E + 0 0
5 0 E - 0 8
1 0 E - 0 7
1 5 E - 0 7
2 0 E - 0 7
2 5 E - 0 7
3 0 E - 0 7
0 200 400 600 800 1000 1200 1400D2 current A
Pre
ssu
re i
n t
he
targ
et c
ham
ber
e-7
mb
ar
H beam OFF H beam ON states 1 + 2 H beam ON state 1 only
30
25
20
15
10
05
00
field strength in the D2 gap0 T 158 T
no ABS beam
MFT off (HFS 1 and 2)
MFT on (HFS 1 only)
September 14 2007 Ralf Engels 14
Do we have a zero field crossing
Magnetic field scan with ANKE at 53ordm using a 3D Hallprobe (Gatchina)
Bx By By |B|
Magnetic field along ABS axisbullID2=563 A (~ 06 T)
bullID1D3=129484 A
1 Determine the local Larmor precession frequency ωL
2 The angular velocity of the magnetic field ωB
As long as the ratio R=ωLωB is large the spin of the atom follows the field directionrarr no depolarization due to zero crossings
ωL
R=ωLωB
ωB
September 14 2007 Ralf Engels 15
Tuning of the Transition Units
Supporting bridge betweenD1 and D2
Additional shielding fromthe D2 stray fields
Cryopump at the target chamber
Polarimeter ionizer underthe target chamber
September 14 2007 Ralf Engels 16
First Polarization Measurement with the LSP
Problems
- The magnetic stray field of the D2 magnet deflected the produced protons
- The quantization axis was rotated by the stray field and the LSP measures
only the projection on the horizontal beam line
Next time More shielding and a rotatable Wien filter to compensate the
misalignment of the polarization axis
WFT was tuned online at the ANKE target position near the D2 magnet
The measured asymetry was stable during the beam time
September 14 2007 Ralf Engels 17
37middot10-840middot10-9With catcher
30middot10-740middot10-9Without catcher
With
ABS jet
Without
ABS jet
ABS beam catcher
~13cm~13cm
Measured pressures in the target chamber mbar
AB
S-j
et d
ensi
ty c
m-3
integral thickness ~ 15 1011 cm-2
ABS jet
COSY Beam
The ABS jet target
September 14 2007 Ralf Engels 18
Storage cell setup
COSYbeam
XY-table Frame with storage cell and aperture
Target chamber
Feeding tube l = 120 mm Oslash = 10 mm
Extraction tube l = 230 mm Oslash = 10 mm
Beam tube l = 400 mm 20x20 mm2
400mm400mm
September 14 2007 Ralf Engels 19
The COSY beam size
at injection
with an accelerated beam
no target with cluster target(density ~ 1014 atcm2)
9x12 mm 16x15 mm
36x16 mm
15 x 15 mm2
September 14 2007 Ralf Engels 20
Storage cell Final setup for the 1 Experiment
Tools for the experiment New storage cell amp support
(20bull20bull390 mm)
gt high target density gt unpolarized gas feeding system
LSP below the target chamber
gt online measurement of the ABS beam polarization
Silicon Tracking Telescope (STT)
gt measurement of spectator protonsnearby the storage cell center
September 14 2007 Ralf Engels 21
Cooler stacking with the storage cell
28 stacks followed by bull 2s electron cooling bull after 58s acceleration toTp=600 MeV
Cooler Stacking allows for higher polarized beam intensities with cell
Without storage cell 25middot1010 ions were reached
September 14 2007 Ralf Engels 22
Results of the cell tests
single injection 3557empty cell
26no cell80 stacking +
electron cooling
flattop
(600 MeV)after
coolinginjection
empty cell
no cell
target
92ordm
0ordm
ΘANKE
30 stacking + electron cooling
83
number of stored protons 10 9
2030 stacking +
electron cooling
1421single injection
injection type
30 stacking + electron cooling92ordm
cell with H gas from ABS
empty cell
64
6
9
September 14 2007 Ralf Engels 23
Storage cell and stochastically cooled beam
Cooling off
Cooling on
Tp= 831 MeV
September 14 2007 Ralf Engels 24
First Experimental Beam Time
Stacking rarr 120 injection with 10 s e-coolingFlat top rarr 30 min to have about 60 duty time
0 20 50Time min
September 14 2007 Ralf Engels 25
First Experimental Beam Time
Stacking rarr 120 injection with 10 s e-coolingFlat top rarr 30 min to have about 23 duty time
0 20 50Time min
Switching on the gasto feed the storage cell
Acceleration withoutgas in the storage cell
7 109 polarized deuterons in the ring with gas in the target
September 14 2007 Ralf Engels 26
Td=12 GeV target H (N2) gas
dprarrdp
dp rarr rarr
First Double Polarized Experiment dp dp rarr rarr
September 14 2007 Ralf Engels 27
First Double Polarized Experiment dp dp rarr rarr
Td=12 GeV target H (N2) gas
dprarr(dpsp) πo
quasi-free nprarrd
πo
(High amp Low branch)
High branch
Low branch
dp rarr rarr
September 14 2007 Ralf Engels 28
First Polarization Measurement of the Target
ANKE
preliminary
dp Td=12 GeV polarized H gas
quasi-free nprarrd
πo
(High amp Low branch)
ltQygt = 075 plusmn 006
θd=50-150 θd=150-220 θd=220-280 θd=280-400
θd=1550-1650 θd=1650-1700 θd=1700-1770
rarr
quasi-free
np rarr dπ0
(High and low branch)
ltQygt = 079 plusmn 007
September 14 2007 Ralf Engels 29
Summary of commissioning and first experiment
1 Cell-target thickness for H (hyperfine state 1) ~ 2 middot 1013 cm-2
3 ABS jet-target thickness ~ 15 middot 1011 cm-2
bull Tests at ANKE with ABS and storage cell
with stacking injection (Nov 2005) and stochastic cooling (Mar 2006)
2 Average luminosity for the storage-cell test ~ 1 middot 1029 cm-2 s-1
4 Hydrogen polarization in the cell ~ 079 +- 007
bull First experiment dprarrppn - JanFeb 2007rarrrarr
September 14 2007 Ralf Engels 30
Plans for the future
December 07 ndash PIT reinstallation With rotatable Wien filter and
better shielding of the LSP
JanFeb rsquo08 ndash Next beam time d prarr (pp)n at 2435 ndash 37 GeVc
(5 Weeks)
March rsquo08 ndash PIT deinstallation
ABS and LSP can be used for other experiments
- ISTC project 1860 Nuclear Polarization in H2D
2 molecules
- Direct Measurements of the Hyperfine levels
in the 2S12
2P12
state rarr Breit-Rabi diagram
rarr rarr
September 14 2007 Ralf Engels 31
Far Future Polarized Fusion
- First Experiments with the Polarized Internal Gas Target (PIT) at ANKECOSY
-
September 14 2007 Ralf Engels 3
bull internal experiments ndash with the circulating beam bull external experiments ndash with the extracted beam
p p d dwith momenta up to 37 GeVc
COSY ndash COoler SYnchrotron
September 14 2007 Ralf Engels 4
ANKE at COSY
Targetsbull Solid stripbull Cluster jetbull Polarized internal target PIT ( storage cell or jet )
Magnetsbull D2 ndash spectrometer magnetbull D1 D3 ndash beam bending magnets
Detector systemsbull Positive amp Negativebull Forward amp Backwardbull Spectator Detectors
Spectrometer ANKE
September 14 2007 Ralf Engels 5
PIT at ANKE
3D CAD drawing of PIT at ANKE
Storage cellPolarimeter
ABS
Technical constraints
bull Target exchange within a maintenance week
bull New support bridge following the movement of D2 magnet
bull Magnetic shielding of componentsbull of the Atomic Beam Source (ABS)bull (D2 Magnet 16 Tesla)
September 14 2007 Ralf Engels 6
Polarized Internal Gas Target
Main parts of a PITbull Atomic Beam Source
bull Target gas
hydrogen or deuteriumbull H beam intensity (2 hyperfine states)
76 1016 atoms sbull Beam size at the interaction point
σ = 285 plusmn 042 mmbull Polarization for hydrogen atoms
PZ = 089 plusmn 001
PZ = -096 plusmn 001
bull Lamb-Shift Polarimeterbull Target chamber with Storage Cell
ABS and LSP at the laboratory
September 14 2007 Ralf Engels 7
The Lamb-shift Polarimeter
September 14 2007 Ralf Engels 8
The Molecules in the ABS jet
I H 2
+
I H 2
+
+ c middot I p
= 0029 plusmn 0002
Engels et al RSI 76 053305 (2005)
September 14 2007 Ralf Engels 9
ABS and LSP in the COSY hall
December 2004 ndash transfer to COSY hall (outside of the COSY tunnel)
May 2005 ndash tests after reassembling
Setup in the COSY hall
bull Supports representing
D1 and D2
bull New support bridge
bull Platform for all electronic and supply components
bull Heat exchanger with closed cooling-water circuit
June 2005 ndash setup ready
for installation at ANKE
September 14 2007 Ralf Engels 10
PIT installation at ANKE
Platform transportationABS transportation
September 14 2007 Ralf Engels 11
PIT at ANKE
September 14 2007 Ralf Engels 12
Magnetic stray field of D2
PIT setup with shielded components at ANKE
x
y
z
90150135
61530
302555
4026300
200550300
60100300
303355
calculated field strength (G)measured field strength (G)permissible field strength for the device given by the producer (G)
September 14 2007 Ralf Engels 13
Test of the medium-field rf transition unit
0 0 E + 0 0
5 0 E - 0 8
1 0 E - 0 7
1 5 E - 0 7
2 0 E - 0 7
2 5 E - 0 7
3 0 E - 0 7
0 200 400 600 800 1000 1200 1400D2 current A
Pre
ssu
re i
n t
he
targ
et c
ham
ber
e-7
mb
ar
H beam OFF H beam ON states 1 + 2 H beam ON state 1 only
30
25
20
15
10
05
00
field strength in the D2 gap0 T 158 T
0 0 E + 0 0
5 0 E - 0 8
1 0 E - 0 7
1 5 E - 0 7
2 0 E - 0 7
2 5 E - 0 7
3 0 E - 0 7
0 200 400 600 800 1000 1200 1400D2 current A
Pre
ssu
re i
n t
he
targ
et c
ham
ber
e-7
mb
ar
H beam OFF H beam ON states 1 + 2 H beam ON state 1 only
30
25
20
15
10
05
00
field strength in the D2 gap0 T 158 T
no ABS beam
MFT off (HFS 1 and 2)
MFT on (HFS 1 only)
September 14 2007 Ralf Engels 14
Do we have a zero field crossing
Magnetic field scan with ANKE at 53ordm using a 3D Hallprobe (Gatchina)
Bx By By |B|
Magnetic field along ABS axisbullID2=563 A (~ 06 T)
bullID1D3=129484 A
1 Determine the local Larmor precession frequency ωL
2 The angular velocity of the magnetic field ωB
As long as the ratio R=ωLωB is large the spin of the atom follows the field directionrarr no depolarization due to zero crossings
ωL
R=ωLωB
ωB
September 14 2007 Ralf Engels 15
Tuning of the Transition Units
Supporting bridge betweenD1 and D2
Additional shielding fromthe D2 stray fields
Cryopump at the target chamber
Polarimeter ionizer underthe target chamber
September 14 2007 Ralf Engels 16
First Polarization Measurement with the LSP
Problems
- The magnetic stray field of the D2 magnet deflected the produced protons
- The quantization axis was rotated by the stray field and the LSP measures
only the projection on the horizontal beam line
Next time More shielding and a rotatable Wien filter to compensate the
misalignment of the polarization axis
WFT was tuned online at the ANKE target position near the D2 magnet
The measured asymetry was stable during the beam time
September 14 2007 Ralf Engels 17
37middot10-840middot10-9With catcher
30middot10-740middot10-9Without catcher
With
ABS jet
Without
ABS jet
ABS beam catcher
~13cm~13cm
Measured pressures in the target chamber mbar
AB
S-j
et d
ensi
ty c
m-3
integral thickness ~ 15 1011 cm-2
ABS jet
COSY Beam
The ABS jet target
September 14 2007 Ralf Engels 18
Storage cell setup
COSYbeam
XY-table Frame with storage cell and aperture
Target chamber
Feeding tube l = 120 mm Oslash = 10 mm
Extraction tube l = 230 mm Oslash = 10 mm
Beam tube l = 400 mm 20x20 mm2
400mm400mm
September 14 2007 Ralf Engels 19
The COSY beam size
at injection
with an accelerated beam
no target with cluster target(density ~ 1014 atcm2)
9x12 mm 16x15 mm
36x16 mm
15 x 15 mm2
September 14 2007 Ralf Engels 20
Storage cell Final setup for the 1 Experiment
Tools for the experiment New storage cell amp support
(20bull20bull390 mm)
gt high target density gt unpolarized gas feeding system
LSP below the target chamber
gt online measurement of the ABS beam polarization
Silicon Tracking Telescope (STT)
gt measurement of spectator protonsnearby the storage cell center
September 14 2007 Ralf Engels 21
Cooler stacking with the storage cell
28 stacks followed by bull 2s electron cooling bull after 58s acceleration toTp=600 MeV
Cooler Stacking allows for higher polarized beam intensities with cell
Without storage cell 25middot1010 ions were reached
September 14 2007 Ralf Engels 22
Results of the cell tests
single injection 3557empty cell
26no cell80 stacking +
electron cooling
flattop
(600 MeV)after
coolinginjection
empty cell
no cell
target
92ordm
0ordm
ΘANKE
30 stacking + electron cooling
83
number of stored protons 10 9
2030 stacking +
electron cooling
1421single injection
injection type
30 stacking + electron cooling92ordm
cell with H gas from ABS
empty cell
64
6
9
September 14 2007 Ralf Engels 23
Storage cell and stochastically cooled beam
Cooling off
Cooling on
Tp= 831 MeV
September 14 2007 Ralf Engels 24
First Experimental Beam Time
Stacking rarr 120 injection with 10 s e-coolingFlat top rarr 30 min to have about 60 duty time
0 20 50Time min
September 14 2007 Ralf Engels 25
First Experimental Beam Time
Stacking rarr 120 injection with 10 s e-coolingFlat top rarr 30 min to have about 23 duty time
0 20 50Time min
Switching on the gasto feed the storage cell
Acceleration withoutgas in the storage cell
7 109 polarized deuterons in the ring with gas in the target
September 14 2007 Ralf Engels 26
Td=12 GeV target H (N2) gas
dprarrdp
dp rarr rarr
First Double Polarized Experiment dp dp rarr rarr
September 14 2007 Ralf Engels 27
First Double Polarized Experiment dp dp rarr rarr
Td=12 GeV target H (N2) gas
dprarr(dpsp) πo
quasi-free nprarrd
πo
(High amp Low branch)
High branch
Low branch
dp rarr rarr
September 14 2007 Ralf Engels 28
First Polarization Measurement of the Target
ANKE
preliminary
dp Td=12 GeV polarized H gas
quasi-free nprarrd
πo
(High amp Low branch)
ltQygt = 075 plusmn 006
θd=50-150 θd=150-220 θd=220-280 θd=280-400
θd=1550-1650 θd=1650-1700 θd=1700-1770
rarr
quasi-free
np rarr dπ0
(High and low branch)
ltQygt = 079 plusmn 007
September 14 2007 Ralf Engels 29
Summary of commissioning and first experiment
1 Cell-target thickness for H (hyperfine state 1) ~ 2 middot 1013 cm-2
3 ABS jet-target thickness ~ 15 middot 1011 cm-2
bull Tests at ANKE with ABS and storage cell
with stacking injection (Nov 2005) and stochastic cooling (Mar 2006)
2 Average luminosity for the storage-cell test ~ 1 middot 1029 cm-2 s-1
4 Hydrogen polarization in the cell ~ 079 +- 007
bull First experiment dprarrppn - JanFeb 2007rarrrarr
September 14 2007 Ralf Engels 30
Plans for the future
December 07 ndash PIT reinstallation With rotatable Wien filter and
better shielding of the LSP
JanFeb rsquo08 ndash Next beam time d prarr (pp)n at 2435 ndash 37 GeVc
(5 Weeks)
March rsquo08 ndash PIT deinstallation
ABS and LSP can be used for other experiments
- ISTC project 1860 Nuclear Polarization in H2D
2 molecules
- Direct Measurements of the Hyperfine levels
in the 2S12
2P12
state rarr Breit-Rabi diagram
rarr rarr
September 14 2007 Ralf Engels 31
Far Future Polarized Fusion
- First Experiments with the Polarized Internal Gas Target (PIT) at ANKECOSY
-
September 14 2007 Ralf Engels 4
ANKE at COSY
Targetsbull Solid stripbull Cluster jetbull Polarized internal target PIT ( storage cell or jet )
Magnetsbull D2 ndash spectrometer magnetbull D1 D3 ndash beam bending magnets
Detector systemsbull Positive amp Negativebull Forward amp Backwardbull Spectator Detectors
Spectrometer ANKE
September 14 2007 Ralf Engels 5
PIT at ANKE
3D CAD drawing of PIT at ANKE
Storage cellPolarimeter
ABS
Technical constraints
bull Target exchange within a maintenance week
bull New support bridge following the movement of D2 magnet
bull Magnetic shielding of componentsbull of the Atomic Beam Source (ABS)bull (D2 Magnet 16 Tesla)
September 14 2007 Ralf Engels 6
Polarized Internal Gas Target
Main parts of a PITbull Atomic Beam Source
bull Target gas
hydrogen or deuteriumbull H beam intensity (2 hyperfine states)
76 1016 atoms sbull Beam size at the interaction point
σ = 285 plusmn 042 mmbull Polarization for hydrogen atoms
PZ = 089 plusmn 001
PZ = -096 plusmn 001
bull Lamb-Shift Polarimeterbull Target chamber with Storage Cell
ABS and LSP at the laboratory
September 14 2007 Ralf Engels 7
The Lamb-shift Polarimeter
September 14 2007 Ralf Engels 8
The Molecules in the ABS jet
I H 2
+
I H 2
+
+ c middot I p
= 0029 plusmn 0002
Engels et al RSI 76 053305 (2005)
September 14 2007 Ralf Engels 9
ABS and LSP in the COSY hall
December 2004 ndash transfer to COSY hall (outside of the COSY tunnel)
May 2005 ndash tests after reassembling
Setup in the COSY hall
bull Supports representing
D1 and D2
bull New support bridge
bull Platform for all electronic and supply components
bull Heat exchanger with closed cooling-water circuit
June 2005 ndash setup ready
for installation at ANKE
September 14 2007 Ralf Engels 10
PIT installation at ANKE
Platform transportationABS transportation
September 14 2007 Ralf Engels 11
PIT at ANKE
September 14 2007 Ralf Engels 12
Magnetic stray field of D2
PIT setup with shielded components at ANKE
x
y
z
90150135
61530
302555
4026300
200550300
60100300
303355
calculated field strength (G)measured field strength (G)permissible field strength for the device given by the producer (G)
September 14 2007 Ralf Engels 13
Test of the medium-field rf transition unit
0 0 E + 0 0
5 0 E - 0 8
1 0 E - 0 7
1 5 E - 0 7
2 0 E - 0 7
2 5 E - 0 7
3 0 E - 0 7
0 200 400 600 800 1000 1200 1400D2 current A
Pre
ssu
re i
n t
he
targ
et c
ham
ber
e-7
mb
ar
H beam OFF H beam ON states 1 + 2 H beam ON state 1 only
30
25
20
15
10
05
00
field strength in the D2 gap0 T 158 T
0 0 E + 0 0
5 0 E - 0 8
1 0 E - 0 7
1 5 E - 0 7
2 0 E - 0 7
2 5 E - 0 7
3 0 E - 0 7
0 200 400 600 800 1000 1200 1400D2 current A
Pre
ssu
re i
n t
he
targ
et c
ham
ber
e-7
mb
ar
H beam OFF H beam ON states 1 + 2 H beam ON state 1 only
30
25
20
15
10
05
00
field strength in the D2 gap0 T 158 T
no ABS beam
MFT off (HFS 1 and 2)
MFT on (HFS 1 only)
September 14 2007 Ralf Engels 14
Do we have a zero field crossing
Magnetic field scan with ANKE at 53ordm using a 3D Hallprobe (Gatchina)
Bx By By |B|
Magnetic field along ABS axisbullID2=563 A (~ 06 T)
bullID1D3=129484 A
1 Determine the local Larmor precession frequency ωL
2 The angular velocity of the magnetic field ωB
As long as the ratio R=ωLωB is large the spin of the atom follows the field directionrarr no depolarization due to zero crossings
ωL
R=ωLωB
ωB
September 14 2007 Ralf Engels 15
Tuning of the Transition Units
Supporting bridge betweenD1 and D2
Additional shielding fromthe D2 stray fields
Cryopump at the target chamber
Polarimeter ionizer underthe target chamber
September 14 2007 Ralf Engels 16
First Polarization Measurement with the LSP
Problems
- The magnetic stray field of the D2 magnet deflected the produced protons
- The quantization axis was rotated by the stray field and the LSP measures
only the projection on the horizontal beam line
Next time More shielding and a rotatable Wien filter to compensate the
misalignment of the polarization axis
WFT was tuned online at the ANKE target position near the D2 magnet
The measured asymetry was stable during the beam time
September 14 2007 Ralf Engels 17
37middot10-840middot10-9With catcher
30middot10-740middot10-9Without catcher
With
ABS jet
Without
ABS jet
ABS beam catcher
~13cm~13cm
Measured pressures in the target chamber mbar
AB
S-j
et d
ensi
ty c
m-3
integral thickness ~ 15 1011 cm-2
ABS jet
COSY Beam
The ABS jet target
September 14 2007 Ralf Engels 18
Storage cell setup
COSYbeam
XY-table Frame with storage cell and aperture
Target chamber
Feeding tube l = 120 mm Oslash = 10 mm
Extraction tube l = 230 mm Oslash = 10 mm
Beam tube l = 400 mm 20x20 mm2
400mm400mm
September 14 2007 Ralf Engels 19
The COSY beam size
at injection
with an accelerated beam
no target with cluster target(density ~ 1014 atcm2)
9x12 mm 16x15 mm
36x16 mm
15 x 15 mm2
September 14 2007 Ralf Engels 20
Storage cell Final setup for the 1 Experiment
Tools for the experiment New storage cell amp support
(20bull20bull390 mm)
gt high target density gt unpolarized gas feeding system
LSP below the target chamber
gt online measurement of the ABS beam polarization
Silicon Tracking Telescope (STT)
gt measurement of spectator protonsnearby the storage cell center
September 14 2007 Ralf Engels 21
Cooler stacking with the storage cell
28 stacks followed by bull 2s electron cooling bull after 58s acceleration toTp=600 MeV
Cooler Stacking allows for higher polarized beam intensities with cell
Without storage cell 25middot1010 ions were reached
September 14 2007 Ralf Engels 22
Results of the cell tests
single injection 3557empty cell
26no cell80 stacking +
electron cooling
flattop
(600 MeV)after
coolinginjection
empty cell
no cell
target
92ordm
0ordm
ΘANKE
30 stacking + electron cooling
83
number of stored protons 10 9
2030 stacking +
electron cooling
1421single injection
injection type
30 stacking + electron cooling92ordm
cell with H gas from ABS
empty cell
64
6
9
September 14 2007 Ralf Engels 23
Storage cell and stochastically cooled beam
Cooling off
Cooling on
Tp= 831 MeV
September 14 2007 Ralf Engels 24
First Experimental Beam Time
Stacking rarr 120 injection with 10 s e-coolingFlat top rarr 30 min to have about 60 duty time
0 20 50Time min
September 14 2007 Ralf Engels 25
First Experimental Beam Time
Stacking rarr 120 injection with 10 s e-coolingFlat top rarr 30 min to have about 23 duty time
0 20 50Time min
Switching on the gasto feed the storage cell
Acceleration withoutgas in the storage cell
7 109 polarized deuterons in the ring with gas in the target
September 14 2007 Ralf Engels 26
Td=12 GeV target H (N2) gas
dprarrdp
dp rarr rarr
First Double Polarized Experiment dp dp rarr rarr
September 14 2007 Ralf Engels 27
First Double Polarized Experiment dp dp rarr rarr
Td=12 GeV target H (N2) gas
dprarr(dpsp) πo
quasi-free nprarrd
πo
(High amp Low branch)
High branch
Low branch
dp rarr rarr
September 14 2007 Ralf Engels 28
First Polarization Measurement of the Target
ANKE
preliminary
dp Td=12 GeV polarized H gas
quasi-free nprarrd
πo
(High amp Low branch)
ltQygt = 075 plusmn 006
θd=50-150 θd=150-220 θd=220-280 θd=280-400
θd=1550-1650 θd=1650-1700 θd=1700-1770
rarr
quasi-free
np rarr dπ0
(High and low branch)
ltQygt = 079 plusmn 007
September 14 2007 Ralf Engels 29
Summary of commissioning and first experiment
1 Cell-target thickness for H (hyperfine state 1) ~ 2 middot 1013 cm-2
3 ABS jet-target thickness ~ 15 middot 1011 cm-2
bull Tests at ANKE with ABS and storage cell
with stacking injection (Nov 2005) and stochastic cooling (Mar 2006)
2 Average luminosity for the storage-cell test ~ 1 middot 1029 cm-2 s-1
4 Hydrogen polarization in the cell ~ 079 +- 007
bull First experiment dprarrppn - JanFeb 2007rarrrarr
September 14 2007 Ralf Engels 30
Plans for the future
December 07 ndash PIT reinstallation With rotatable Wien filter and
better shielding of the LSP
JanFeb rsquo08 ndash Next beam time d prarr (pp)n at 2435 ndash 37 GeVc
(5 Weeks)
March rsquo08 ndash PIT deinstallation
ABS and LSP can be used for other experiments
- ISTC project 1860 Nuclear Polarization in H2D
2 molecules
- Direct Measurements of the Hyperfine levels
in the 2S12
2P12
state rarr Breit-Rabi diagram
rarr rarr
September 14 2007 Ralf Engels 31
Far Future Polarized Fusion
- First Experiments with the Polarized Internal Gas Target (PIT) at ANKECOSY
-
September 14 2007 Ralf Engels 5
PIT at ANKE
3D CAD drawing of PIT at ANKE
Storage cellPolarimeter
ABS
Technical constraints
bull Target exchange within a maintenance week
bull New support bridge following the movement of D2 magnet
bull Magnetic shielding of componentsbull of the Atomic Beam Source (ABS)bull (D2 Magnet 16 Tesla)
September 14 2007 Ralf Engels 6
Polarized Internal Gas Target
Main parts of a PITbull Atomic Beam Source
bull Target gas
hydrogen or deuteriumbull H beam intensity (2 hyperfine states)
76 1016 atoms sbull Beam size at the interaction point
σ = 285 plusmn 042 mmbull Polarization for hydrogen atoms
PZ = 089 plusmn 001
PZ = -096 plusmn 001
bull Lamb-Shift Polarimeterbull Target chamber with Storage Cell
ABS and LSP at the laboratory
September 14 2007 Ralf Engels 7
The Lamb-shift Polarimeter
September 14 2007 Ralf Engels 8
The Molecules in the ABS jet
I H 2
+
I H 2
+
+ c middot I p
= 0029 plusmn 0002
Engels et al RSI 76 053305 (2005)
September 14 2007 Ralf Engels 9
ABS and LSP in the COSY hall
December 2004 ndash transfer to COSY hall (outside of the COSY tunnel)
May 2005 ndash tests after reassembling
Setup in the COSY hall
bull Supports representing
D1 and D2
bull New support bridge
bull Platform for all electronic and supply components
bull Heat exchanger with closed cooling-water circuit
June 2005 ndash setup ready
for installation at ANKE
September 14 2007 Ralf Engels 10
PIT installation at ANKE
Platform transportationABS transportation
September 14 2007 Ralf Engels 11
PIT at ANKE
September 14 2007 Ralf Engels 12
Magnetic stray field of D2
PIT setup with shielded components at ANKE
x
y
z
90150135
61530
302555
4026300
200550300
60100300
303355
calculated field strength (G)measured field strength (G)permissible field strength for the device given by the producer (G)
September 14 2007 Ralf Engels 13
Test of the medium-field rf transition unit
0 0 E + 0 0
5 0 E - 0 8
1 0 E - 0 7
1 5 E - 0 7
2 0 E - 0 7
2 5 E - 0 7
3 0 E - 0 7
0 200 400 600 800 1000 1200 1400D2 current A
Pre
ssu
re i
n t
he
targ
et c
ham
ber
e-7
mb
ar
H beam OFF H beam ON states 1 + 2 H beam ON state 1 only
30
25
20
15
10
05
00
field strength in the D2 gap0 T 158 T
0 0 E + 0 0
5 0 E - 0 8
1 0 E - 0 7
1 5 E - 0 7
2 0 E - 0 7
2 5 E - 0 7
3 0 E - 0 7
0 200 400 600 800 1000 1200 1400D2 current A
Pre
ssu
re i
n t
he
targ
et c
ham
ber
e-7
mb
ar
H beam OFF H beam ON states 1 + 2 H beam ON state 1 only
30
25
20
15
10
05
00
field strength in the D2 gap0 T 158 T
no ABS beam
MFT off (HFS 1 and 2)
MFT on (HFS 1 only)
September 14 2007 Ralf Engels 14
Do we have a zero field crossing
Magnetic field scan with ANKE at 53ordm using a 3D Hallprobe (Gatchina)
Bx By By |B|
Magnetic field along ABS axisbullID2=563 A (~ 06 T)
bullID1D3=129484 A
1 Determine the local Larmor precession frequency ωL
2 The angular velocity of the magnetic field ωB
As long as the ratio R=ωLωB is large the spin of the atom follows the field directionrarr no depolarization due to zero crossings
ωL
R=ωLωB
ωB
September 14 2007 Ralf Engels 15
Tuning of the Transition Units
Supporting bridge betweenD1 and D2
Additional shielding fromthe D2 stray fields
Cryopump at the target chamber
Polarimeter ionizer underthe target chamber
September 14 2007 Ralf Engels 16
First Polarization Measurement with the LSP
Problems
- The magnetic stray field of the D2 magnet deflected the produced protons
- The quantization axis was rotated by the stray field and the LSP measures
only the projection on the horizontal beam line
Next time More shielding and a rotatable Wien filter to compensate the
misalignment of the polarization axis
WFT was tuned online at the ANKE target position near the D2 magnet
The measured asymetry was stable during the beam time
September 14 2007 Ralf Engels 17
37middot10-840middot10-9With catcher
30middot10-740middot10-9Without catcher
With
ABS jet
Without
ABS jet
ABS beam catcher
~13cm~13cm
Measured pressures in the target chamber mbar
AB
S-j
et d
ensi
ty c
m-3
integral thickness ~ 15 1011 cm-2
ABS jet
COSY Beam
The ABS jet target
September 14 2007 Ralf Engels 18
Storage cell setup
COSYbeam
XY-table Frame with storage cell and aperture
Target chamber
Feeding tube l = 120 mm Oslash = 10 mm
Extraction tube l = 230 mm Oslash = 10 mm
Beam tube l = 400 mm 20x20 mm2
400mm400mm
September 14 2007 Ralf Engels 19
The COSY beam size
at injection
with an accelerated beam
no target with cluster target(density ~ 1014 atcm2)
9x12 mm 16x15 mm
36x16 mm
15 x 15 mm2
September 14 2007 Ralf Engels 20
Storage cell Final setup for the 1 Experiment
Tools for the experiment New storage cell amp support
(20bull20bull390 mm)
gt high target density gt unpolarized gas feeding system
LSP below the target chamber
gt online measurement of the ABS beam polarization
Silicon Tracking Telescope (STT)
gt measurement of spectator protonsnearby the storage cell center
September 14 2007 Ralf Engels 21
Cooler stacking with the storage cell
28 stacks followed by bull 2s electron cooling bull after 58s acceleration toTp=600 MeV
Cooler Stacking allows for higher polarized beam intensities with cell
Without storage cell 25middot1010 ions were reached
September 14 2007 Ralf Engels 22
Results of the cell tests
single injection 3557empty cell
26no cell80 stacking +
electron cooling
flattop
(600 MeV)after
coolinginjection
empty cell
no cell
target
92ordm
0ordm
ΘANKE
30 stacking + electron cooling
83
number of stored protons 10 9
2030 stacking +
electron cooling
1421single injection
injection type
30 stacking + electron cooling92ordm
cell with H gas from ABS
empty cell
64
6
9
September 14 2007 Ralf Engels 23
Storage cell and stochastically cooled beam
Cooling off
Cooling on
Tp= 831 MeV
September 14 2007 Ralf Engels 24
First Experimental Beam Time
Stacking rarr 120 injection with 10 s e-coolingFlat top rarr 30 min to have about 60 duty time
0 20 50Time min
September 14 2007 Ralf Engels 25
First Experimental Beam Time
Stacking rarr 120 injection with 10 s e-coolingFlat top rarr 30 min to have about 23 duty time
0 20 50Time min
Switching on the gasto feed the storage cell
Acceleration withoutgas in the storage cell
7 109 polarized deuterons in the ring with gas in the target
September 14 2007 Ralf Engels 26
Td=12 GeV target H (N2) gas
dprarrdp
dp rarr rarr
First Double Polarized Experiment dp dp rarr rarr
September 14 2007 Ralf Engels 27
First Double Polarized Experiment dp dp rarr rarr
Td=12 GeV target H (N2) gas
dprarr(dpsp) πo
quasi-free nprarrd
πo
(High amp Low branch)
High branch
Low branch
dp rarr rarr
September 14 2007 Ralf Engels 28
First Polarization Measurement of the Target
ANKE
preliminary
dp Td=12 GeV polarized H gas
quasi-free nprarrd
πo
(High amp Low branch)
ltQygt = 075 plusmn 006
θd=50-150 θd=150-220 θd=220-280 θd=280-400
θd=1550-1650 θd=1650-1700 θd=1700-1770
rarr
quasi-free
np rarr dπ0
(High and low branch)
ltQygt = 079 plusmn 007
September 14 2007 Ralf Engels 29
Summary of commissioning and first experiment
1 Cell-target thickness for H (hyperfine state 1) ~ 2 middot 1013 cm-2
3 ABS jet-target thickness ~ 15 middot 1011 cm-2
bull Tests at ANKE with ABS and storage cell
with stacking injection (Nov 2005) and stochastic cooling (Mar 2006)
2 Average luminosity for the storage-cell test ~ 1 middot 1029 cm-2 s-1
4 Hydrogen polarization in the cell ~ 079 +- 007
bull First experiment dprarrppn - JanFeb 2007rarrrarr
September 14 2007 Ralf Engels 30
Plans for the future
December 07 ndash PIT reinstallation With rotatable Wien filter and
better shielding of the LSP
JanFeb rsquo08 ndash Next beam time d prarr (pp)n at 2435 ndash 37 GeVc
(5 Weeks)
March rsquo08 ndash PIT deinstallation
ABS and LSP can be used for other experiments
- ISTC project 1860 Nuclear Polarization in H2D
2 molecules
- Direct Measurements of the Hyperfine levels
in the 2S12
2P12
state rarr Breit-Rabi diagram
rarr rarr
September 14 2007 Ralf Engels 31
Far Future Polarized Fusion
- First Experiments with the Polarized Internal Gas Target (PIT) at ANKECOSY
-
September 14 2007 Ralf Engels 6
Polarized Internal Gas Target
Main parts of a PITbull Atomic Beam Source
bull Target gas
hydrogen or deuteriumbull H beam intensity (2 hyperfine states)
76 1016 atoms sbull Beam size at the interaction point
σ = 285 plusmn 042 mmbull Polarization for hydrogen atoms
PZ = 089 plusmn 001
PZ = -096 plusmn 001
bull Lamb-Shift Polarimeterbull Target chamber with Storage Cell
ABS and LSP at the laboratory
September 14 2007 Ralf Engels 7
The Lamb-shift Polarimeter
September 14 2007 Ralf Engels 8
The Molecules in the ABS jet
I H 2
+
I H 2
+
+ c middot I p
= 0029 plusmn 0002
Engels et al RSI 76 053305 (2005)
September 14 2007 Ralf Engels 9
ABS and LSP in the COSY hall
December 2004 ndash transfer to COSY hall (outside of the COSY tunnel)
May 2005 ndash tests after reassembling
Setup in the COSY hall
bull Supports representing
D1 and D2
bull New support bridge
bull Platform for all electronic and supply components
bull Heat exchanger with closed cooling-water circuit
June 2005 ndash setup ready
for installation at ANKE
September 14 2007 Ralf Engels 10
PIT installation at ANKE
Platform transportationABS transportation
September 14 2007 Ralf Engels 11
PIT at ANKE
September 14 2007 Ralf Engels 12
Magnetic stray field of D2
PIT setup with shielded components at ANKE
x
y
z
90150135
61530
302555
4026300
200550300
60100300
303355
calculated field strength (G)measured field strength (G)permissible field strength for the device given by the producer (G)
September 14 2007 Ralf Engels 13
Test of the medium-field rf transition unit
0 0 E + 0 0
5 0 E - 0 8
1 0 E - 0 7
1 5 E - 0 7
2 0 E - 0 7
2 5 E - 0 7
3 0 E - 0 7
0 200 400 600 800 1000 1200 1400D2 current A
Pre
ssu
re i
n t
he
targ
et c
ham
ber
e-7
mb
ar
H beam OFF H beam ON states 1 + 2 H beam ON state 1 only
30
25
20
15
10
05
00
field strength in the D2 gap0 T 158 T
0 0 E + 0 0
5 0 E - 0 8
1 0 E - 0 7
1 5 E - 0 7
2 0 E - 0 7
2 5 E - 0 7
3 0 E - 0 7
0 200 400 600 800 1000 1200 1400D2 current A
Pre
ssu
re i
n t
he
targ
et c
ham
ber
e-7
mb
ar
H beam OFF H beam ON states 1 + 2 H beam ON state 1 only
30
25
20
15
10
05
00
field strength in the D2 gap0 T 158 T
no ABS beam
MFT off (HFS 1 and 2)
MFT on (HFS 1 only)
September 14 2007 Ralf Engels 14
Do we have a zero field crossing
Magnetic field scan with ANKE at 53ordm using a 3D Hallprobe (Gatchina)
Bx By By |B|
Magnetic field along ABS axisbullID2=563 A (~ 06 T)
bullID1D3=129484 A
1 Determine the local Larmor precession frequency ωL
2 The angular velocity of the magnetic field ωB
As long as the ratio R=ωLωB is large the spin of the atom follows the field directionrarr no depolarization due to zero crossings
ωL
R=ωLωB
ωB
September 14 2007 Ralf Engels 15
Tuning of the Transition Units
Supporting bridge betweenD1 and D2
Additional shielding fromthe D2 stray fields
Cryopump at the target chamber
Polarimeter ionizer underthe target chamber
September 14 2007 Ralf Engels 16
First Polarization Measurement with the LSP
Problems
- The magnetic stray field of the D2 magnet deflected the produced protons
- The quantization axis was rotated by the stray field and the LSP measures
only the projection on the horizontal beam line
Next time More shielding and a rotatable Wien filter to compensate the
misalignment of the polarization axis
WFT was tuned online at the ANKE target position near the D2 magnet
The measured asymetry was stable during the beam time
September 14 2007 Ralf Engels 17
37middot10-840middot10-9With catcher
30middot10-740middot10-9Without catcher
With
ABS jet
Without
ABS jet
ABS beam catcher
~13cm~13cm
Measured pressures in the target chamber mbar
AB
S-j
et d
ensi
ty c
m-3
integral thickness ~ 15 1011 cm-2
ABS jet
COSY Beam
The ABS jet target
September 14 2007 Ralf Engels 18
Storage cell setup
COSYbeam
XY-table Frame with storage cell and aperture
Target chamber
Feeding tube l = 120 mm Oslash = 10 mm
Extraction tube l = 230 mm Oslash = 10 mm
Beam tube l = 400 mm 20x20 mm2
400mm400mm
September 14 2007 Ralf Engels 19
The COSY beam size
at injection
with an accelerated beam
no target with cluster target(density ~ 1014 atcm2)
9x12 mm 16x15 mm
36x16 mm
15 x 15 mm2
September 14 2007 Ralf Engels 20
Storage cell Final setup for the 1 Experiment
Tools for the experiment New storage cell amp support
(20bull20bull390 mm)
gt high target density gt unpolarized gas feeding system
LSP below the target chamber
gt online measurement of the ABS beam polarization
Silicon Tracking Telescope (STT)
gt measurement of spectator protonsnearby the storage cell center
September 14 2007 Ralf Engels 21
Cooler stacking with the storage cell
28 stacks followed by bull 2s electron cooling bull after 58s acceleration toTp=600 MeV
Cooler Stacking allows for higher polarized beam intensities with cell
Without storage cell 25middot1010 ions were reached
September 14 2007 Ralf Engels 22
Results of the cell tests
single injection 3557empty cell
26no cell80 stacking +
electron cooling
flattop
(600 MeV)after
coolinginjection
empty cell
no cell
target
92ordm
0ordm
ΘANKE
30 stacking + electron cooling
83
number of stored protons 10 9
2030 stacking +
electron cooling
1421single injection
injection type
30 stacking + electron cooling92ordm
cell with H gas from ABS
empty cell
64
6
9
September 14 2007 Ralf Engels 23
Storage cell and stochastically cooled beam
Cooling off
Cooling on
Tp= 831 MeV
September 14 2007 Ralf Engels 24
First Experimental Beam Time
Stacking rarr 120 injection with 10 s e-coolingFlat top rarr 30 min to have about 60 duty time
0 20 50Time min
September 14 2007 Ralf Engels 25
First Experimental Beam Time
Stacking rarr 120 injection with 10 s e-coolingFlat top rarr 30 min to have about 23 duty time
0 20 50Time min
Switching on the gasto feed the storage cell
Acceleration withoutgas in the storage cell
7 109 polarized deuterons in the ring with gas in the target
September 14 2007 Ralf Engels 26
Td=12 GeV target H (N2) gas
dprarrdp
dp rarr rarr
First Double Polarized Experiment dp dp rarr rarr
September 14 2007 Ralf Engels 27
First Double Polarized Experiment dp dp rarr rarr
Td=12 GeV target H (N2) gas
dprarr(dpsp) πo
quasi-free nprarrd
πo
(High amp Low branch)
High branch
Low branch
dp rarr rarr
September 14 2007 Ralf Engels 28
First Polarization Measurement of the Target
ANKE
preliminary
dp Td=12 GeV polarized H gas
quasi-free nprarrd
πo
(High amp Low branch)
ltQygt = 075 plusmn 006
θd=50-150 θd=150-220 θd=220-280 θd=280-400
θd=1550-1650 θd=1650-1700 θd=1700-1770
rarr
quasi-free
np rarr dπ0
(High and low branch)
ltQygt = 079 plusmn 007
September 14 2007 Ralf Engels 29
Summary of commissioning and first experiment
1 Cell-target thickness for H (hyperfine state 1) ~ 2 middot 1013 cm-2
3 ABS jet-target thickness ~ 15 middot 1011 cm-2
bull Tests at ANKE with ABS and storage cell
with stacking injection (Nov 2005) and stochastic cooling (Mar 2006)
2 Average luminosity for the storage-cell test ~ 1 middot 1029 cm-2 s-1
4 Hydrogen polarization in the cell ~ 079 +- 007
bull First experiment dprarrppn - JanFeb 2007rarrrarr
September 14 2007 Ralf Engels 30
Plans for the future
December 07 ndash PIT reinstallation With rotatable Wien filter and
better shielding of the LSP
JanFeb rsquo08 ndash Next beam time d prarr (pp)n at 2435 ndash 37 GeVc
(5 Weeks)
March rsquo08 ndash PIT deinstallation
ABS and LSP can be used for other experiments
- ISTC project 1860 Nuclear Polarization in H2D
2 molecules
- Direct Measurements of the Hyperfine levels
in the 2S12
2P12
state rarr Breit-Rabi diagram
rarr rarr
September 14 2007 Ralf Engels 31
Far Future Polarized Fusion
- First Experiments with the Polarized Internal Gas Target (PIT) at ANKECOSY
-
September 14 2007 Ralf Engels 7
The Lamb-shift Polarimeter
September 14 2007 Ralf Engels 8
The Molecules in the ABS jet
I H 2
+
I H 2
+
+ c middot I p
= 0029 plusmn 0002
Engels et al RSI 76 053305 (2005)
September 14 2007 Ralf Engels 9
ABS and LSP in the COSY hall
December 2004 ndash transfer to COSY hall (outside of the COSY tunnel)
May 2005 ndash tests after reassembling
Setup in the COSY hall
bull Supports representing
D1 and D2
bull New support bridge
bull Platform for all electronic and supply components
bull Heat exchanger with closed cooling-water circuit
June 2005 ndash setup ready
for installation at ANKE
September 14 2007 Ralf Engels 10
PIT installation at ANKE
Platform transportationABS transportation
September 14 2007 Ralf Engels 11
PIT at ANKE
September 14 2007 Ralf Engels 12
Magnetic stray field of D2
PIT setup with shielded components at ANKE
x
y
z
90150135
61530
302555
4026300
200550300
60100300
303355
calculated field strength (G)measured field strength (G)permissible field strength for the device given by the producer (G)
September 14 2007 Ralf Engels 13
Test of the medium-field rf transition unit
0 0 E + 0 0
5 0 E - 0 8
1 0 E - 0 7
1 5 E - 0 7
2 0 E - 0 7
2 5 E - 0 7
3 0 E - 0 7
0 200 400 600 800 1000 1200 1400D2 current A
Pre
ssu
re i
n t
he
targ
et c
ham
ber
e-7
mb
ar
H beam OFF H beam ON states 1 + 2 H beam ON state 1 only
30
25
20
15
10
05
00
field strength in the D2 gap0 T 158 T
0 0 E + 0 0
5 0 E - 0 8
1 0 E - 0 7
1 5 E - 0 7
2 0 E - 0 7
2 5 E - 0 7
3 0 E - 0 7
0 200 400 600 800 1000 1200 1400D2 current A
Pre
ssu
re i
n t
he
targ
et c
ham
ber
e-7
mb
ar
H beam OFF H beam ON states 1 + 2 H beam ON state 1 only
30
25
20
15
10
05
00
field strength in the D2 gap0 T 158 T
no ABS beam
MFT off (HFS 1 and 2)
MFT on (HFS 1 only)
September 14 2007 Ralf Engels 14
Do we have a zero field crossing
Magnetic field scan with ANKE at 53ordm using a 3D Hallprobe (Gatchina)
Bx By By |B|
Magnetic field along ABS axisbullID2=563 A (~ 06 T)
bullID1D3=129484 A
1 Determine the local Larmor precession frequency ωL
2 The angular velocity of the magnetic field ωB
As long as the ratio R=ωLωB is large the spin of the atom follows the field directionrarr no depolarization due to zero crossings
ωL
R=ωLωB
ωB
September 14 2007 Ralf Engels 15
Tuning of the Transition Units
Supporting bridge betweenD1 and D2
Additional shielding fromthe D2 stray fields
Cryopump at the target chamber
Polarimeter ionizer underthe target chamber
September 14 2007 Ralf Engels 16
First Polarization Measurement with the LSP
Problems
- The magnetic stray field of the D2 magnet deflected the produced protons
- The quantization axis was rotated by the stray field and the LSP measures
only the projection on the horizontal beam line
Next time More shielding and a rotatable Wien filter to compensate the
misalignment of the polarization axis
WFT was tuned online at the ANKE target position near the D2 magnet
The measured asymetry was stable during the beam time
September 14 2007 Ralf Engels 17
37middot10-840middot10-9With catcher
30middot10-740middot10-9Without catcher
With
ABS jet
Without
ABS jet
ABS beam catcher
~13cm~13cm
Measured pressures in the target chamber mbar
AB
S-j
et d
ensi
ty c
m-3
integral thickness ~ 15 1011 cm-2
ABS jet
COSY Beam
The ABS jet target
September 14 2007 Ralf Engels 18
Storage cell setup
COSYbeam
XY-table Frame with storage cell and aperture
Target chamber
Feeding tube l = 120 mm Oslash = 10 mm
Extraction tube l = 230 mm Oslash = 10 mm
Beam tube l = 400 mm 20x20 mm2
400mm400mm
September 14 2007 Ralf Engels 19
The COSY beam size
at injection
with an accelerated beam
no target with cluster target(density ~ 1014 atcm2)
9x12 mm 16x15 mm
36x16 mm
15 x 15 mm2
September 14 2007 Ralf Engels 20
Storage cell Final setup for the 1 Experiment
Tools for the experiment New storage cell amp support
(20bull20bull390 mm)
gt high target density gt unpolarized gas feeding system
LSP below the target chamber
gt online measurement of the ABS beam polarization
Silicon Tracking Telescope (STT)
gt measurement of spectator protonsnearby the storage cell center
September 14 2007 Ralf Engels 21
Cooler stacking with the storage cell
28 stacks followed by bull 2s electron cooling bull after 58s acceleration toTp=600 MeV
Cooler Stacking allows for higher polarized beam intensities with cell
Without storage cell 25middot1010 ions were reached
September 14 2007 Ralf Engels 22
Results of the cell tests
single injection 3557empty cell
26no cell80 stacking +
electron cooling
flattop
(600 MeV)after
coolinginjection
empty cell
no cell
target
92ordm
0ordm
ΘANKE
30 stacking + electron cooling
83
number of stored protons 10 9
2030 stacking +
electron cooling
1421single injection
injection type
30 stacking + electron cooling92ordm
cell with H gas from ABS
empty cell
64
6
9
September 14 2007 Ralf Engels 23
Storage cell and stochastically cooled beam
Cooling off
Cooling on
Tp= 831 MeV
September 14 2007 Ralf Engels 24
First Experimental Beam Time
Stacking rarr 120 injection with 10 s e-coolingFlat top rarr 30 min to have about 60 duty time
0 20 50Time min
September 14 2007 Ralf Engels 25
First Experimental Beam Time
Stacking rarr 120 injection with 10 s e-coolingFlat top rarr 30 min to have about 23 duty time
0 20 50Time min
Switching on the gasto feed the storage cell
Acceleration withoutgas in the storage cell
7 109 polarized deuterons in the ring with gas in the target
September 14 2007 Ralf Engels 26
Td=12 GeV target H (N2) gas
dprarrdp
dp rarr rarr
First Double Polarized Experiment dp dp rarr rarr
September 14 2007 Ralf Engels 27
First Double Polarized Experiment dp dp rarr rarr
Td=12 GeV target H (N2) gas
dprarr(dpsp) πo
quasi-free nprarrd
πo
(High amp Low branch)
High branch
Low branch
dp rarr rarr
September 14 2007 Ralf Engels 28
First Polarization Measurement of the Target
ANKE
preliminary
dp Td=12 GeV polarized H gas
quasi-free nprarrd
πo
(High amp Low branch)
ltQygt = 075 plusmn 006
θd=50-150 θd=150-220 θd=220-280 θd=280-400
θd=1550-1650 θd=1650-1700 θd=1700-1770
rarr
quasi-free
np rarr dπ0
(High and low branch)
ltQygt = 079 plusmn 007
September 14 2007 Ralf Engels 29
Summary of commissioning and first experiment
1 Cell-target thickness for H (hyperfine state 1) ~ 2 middot 1013 cm-2
3 ABS jet-target thickness ~ 15 middot 1011 cm-2
bull Tests at ANKE with ABS and storage cell
with stacking injection (Nov 2005) and stochastic cooling (Mar 2006)
2 Average luminosity for the storage-cell test ~ 1 middot 1029 cm-2 s-1
4 Hydrogen polarization in the cell ~ 079 +- 007
bull First experiment dprarrppn - JanFeb 2007rarrrarr
September 14 2007 Ralf Engels 30
Plans for the future
December 07 ndash PIT reinstallation With rotatable Wien filter and
better shielding of the LSP
JanFeb rsquo08 ndash Next beam time d prarr (pp)n at 2435 ndash 37 GeVc
(5 Weeks)
March rsquo08 ndash PIT deinstallation
ABS and LSP can be used for other experiments
- ISTC project 1860 Nuclear Polarization in H2D
2 molecules
- Direct Measurements of the Hyperfine levels
in the 2S12
2P12
state rarr Breit-Rabi diagram
rarr rarr
September 14 2007 Ralf Engels 31
Far Future Polarized Fusion
- First Experiments with the Polarized Internal Gas Target (PIT) at ANKECOSY
-
September 14 2007 Ralf Engels 8
The Molecules in the ABS jet
I H 2
+
I H 2
+
+ c middot I p
= 0029 plusmn 0002
Engels et al RSI 76 053305 (2005)
September 14 2007 Ralf Engels 9
ABS and LSP in the COSY hall
December 2004 ndash transfer to COSY hall (outside of the COSY tunnel)
May 2005 ndash tests after reassembling
Setup in the COSY hall
bull Supports representing
D1 and D2
bull New support bridge
bull Platform for all electronic and supply components
bull Heat exchanger with closed cooling-water circuit
June 2005 ndash setup ready
for installation at ANKE
September 14 2007 Ralf Engels 10
PIT installation at ANKE
Platform transportationABS transportation
September 14 2007 Ralf Engels 11
PIT at ANKE
September 14 2007 Ralf Engels 12
Magnetic stray field of D2
PIT setup with shielded components at ANKE
x
y
z
90150135
61530
302555
4026300
200550300
60100300
303355
calculated field strength (G)measured field strength (G)permissible field strength for the device given by the producer (G)
September 14 2007 Ralf Engels 13
Test of the medium-field rf transition unit
0 0 E + 0 0
5 0 E - 0 8
1 0 E - 0 7
1 5 E - 0 7
2 0 E - 0 7
2 5 E - 0 7
3 0 E - 0 7
0 200 400 600 800 1000 1200 1400D2 current A
Pre
ssu
re i
n t
he
targ
et c
ham
ber
e-7
mb
ar
H beam OFF H beam ON states 1 + 2 H beam ON state 1 only
30
25
20
15
10
05
00
field strength in the D2 gap0 T 158 T
0 0 E + 0 0
5 0 E - 0 8
1 0 E - 0 7
1 5 E - 0 7
2 0 E - 0 7
2 5 E - 0 7
3 0 E - 0 7
0 200 400 600 800 1000 1200 1400D2 current A
Pre
ssu
re i
n t
he
targ
et c
ham
ber
e-7
mb
ar
H beam OFF H beam ON states 1 + 2 H beam ON state 1 only
30
25
20
15
10
05
00
field strength in the D2 gap0 T 158 T
no ABS beam
MFT off (HFS 1 and 2)
MFT on (HFS 1 only)
September 14 2007 Ralf Engels 14
Do we have a zero field crossing
Magnetic field scan with ANKE at 53ordm using a 3D Hallprobe (Gatchina)
Bx By By |B|
Magnetic field along ABS axisbullID2=563 A (~ 06 T)
bullID1D3=129484 A
1 Determine the local Larmor precession frequency ωL
2 The angular velocity of the magnetic field ωB
As long as the ratio R=ωLωB is large the spin of the atom follows the field directionrarr no depolarization due to zero crossings
ωL
R=ωLωB
ωB
September 14 2007 Ralf Engels 15
Tuning of the Transition Units
Supporting bridge betweenD1 and D2
Additional shielding fromthe D2 stray fields
Cryopump at the target chamber
Polarimeter ionizer underthe target chamber
September 14 2007 Ralf Engels 16
First Polarization Measurement with the LSP
Problems
- The magnetic stray field of the D2 magnet deflected the produced protons
- The quantization axis was rotated by the stray field and the LSP measures
only the projection on the horizontal beam line
Next time More shielding and a rotatable Wien filter to compensate the
misalignment of the polarization axis
WFT was tuned online at the ANKE target position near the D2 magnet
The measured asymetry was stable during the beam time
September 14 2007 Ralf Engels 17
37middot10-840middot10-9With catcher
30middot10-740middot10-9Without catcher
With
ABS jet
Without
ABS jet
ABS beam catcher
~13cm~13cm
Measured pressures in the target chamber mbar
AB
S-j
et d
ensi
ty c
m-3
integral thickness ~ 15 1011 cm-2
ABS jet
COSY Beam
The ABS jet target
September 14 2007 Ralf Engels 18
Storage cell setup
COSYbeam
XY-table Frame with storage cell and aperture
Target chamber
Feeding tube l = 120 mm Oslash = 10 mm
Extraction tube l = 230 mm Oslash = 10 mm
Beam tube l = 400 mm 20x20 mm2
400mm400mm
September 14 2007 Ralf Engels 19
The COSY beam size
at injection
with an accelerated beam
no target with cluster target(density ~ 1014 atcm2)
9x12 mm 16x15 mm
36x16 mm
15 x 15 mm2
September 14 2007 Ralf Engels 20
Storage cell Final setup for the 1 Experiment
Tools for the experiment New storage cell amp support
(20bull20bull390 mm)
gt high target density gt unpolarized gas feeding system
LSP below the target chamber
gt online measurement of the ABS beam polarization
Silicon Tracking Telescope (STT)
gt measurement of spectator protonsnearby the storage cell center
September 14 2007 Ralf Engels 21
Cooler stacking with the storage cell
28 stacks followed by bull 2s electron cooling bull after 58s acceleration toTp=600 MeV
Cooler Stacking allows for higher polarized beam intensities with cell
Without storage cell 25middot1010 ions were reached
September 14 2007 Ralf Engels 22
Results of the cell tests
single injection 3557empty cell
26no cell80 stacking +
electron cooling
flattop
(600 MeV)after
coolinginjection
empty cell
no cell
target
92ordm
0ordm
ΘANKE
30 stacking + electron cooling
83
number of stored protons 10 9
2030 stacking +
electron cooling
1421single injection
injection type
30 stacking + electron cooling92ordm
cell with H gas from ABS
empty cell
64
6
9
September 14 2007 Ralf Engels 23
Storage cell and stochastically cooled beam
Cooling off
Cooling on
Tp= 831 MeV
September 14 2007 Ralf Engels 24
First Experimental Beam Time
Stacking rarr 120 injection with 10 s e-coolingFlat top rarr 30 min to have about 60 duty time
0 20 50Time min
September 14 2007 Ralf Engels 25
First Experimental Beam Time
Stacking rarr 120 injection with 10 s e-coolingFlat top rarr 30 min to have about 23 duty time
0 20 50Time min
Switching on the gasto feed the storage cell
Acceleration withoutgas in the storage cell
7 109 polarized deuterons in the ring with gas in the target
September 14 2007 Ralf Engels 26
Td=12 GeV target H (N2) gas
dprarrdp
dp rarr rarr
First Double Polarized Experiment dp dp rarr rarr
September 14 2007 Ralf Engels 27
First Double Polarized Experiment dp dp rarr rarr
Td=12 GeV target H (N2) gas
dprarr(dpsp) πo
quasi-free nprarrd
πo
(High amp Low branch)
High branch
Low branch
dp rarr rarr
September 14 2007 Ralf Engels 28
First Polarization Measurement of the Target
ANKE
preliminary
dp Td=12 GeV polarized H gas
quasi-free nprarrd
πo
(High amp Low branch)
ltQygt = 075 plusmn 006
θd=50-150 θd=150-220 θd=220-280 θd=280-400
θd=1550-1650 θd=1650-1700 θd=1700-1770
rarr
quasi-free
np rarr dπ0
(High and low branch)
ltQygt = 079 plusmn 007
September 14 2007 Ralf Engels 29
Summary of commissioning and first experiment
1 Cell-target thickness for H (hyperfine state 1) ~ 2 middot 1013 cm-2
3 ABS jet-target thickness ~ 15 middot 1011 cm-2
bull Tests at ANKE with ABS and storage cell
with stacking injection (Nov 2005) and stochastic cooling (Mar 2006)
2 Average luminosity for the storage-cell test ~ 1 middot 1029 cm-2 s-1
4 Hydrogen polarization in the cell ~ 079 +- 007
bull First experiment dprarrppn - JanFeb 2007rarrrarr
September 14 2007 Ralf Engels 30
Plans for the future
December 07 ndash PIT reinstallation With rotatable Wien filter and
better shielding of the LSP
JanFeb rsquo08 ndash Next beam time d prarr (pp)n at 2435 ndash 37 GeVc
(5 Weeks)
March rsquo08 ndash PIT deinstallation
ABS and LSP can be used for other experiments
- ISTC project 1860 Nuclear Polarization in H2D
2 molecules
- Direct Measurements of the Hyperfine levels
in the 2S12
2P12
state rarr Breit-Rabi diagram
rarr rarr
September 14 2007 Ralf Engels 31
Far Future Polarized Fusion
- First Experiments with the Polarized Internal Gas Target (PIT) at ANKECOSY
-
September 14 2007 Ralf Engels 9
ABS and LSP in the COSY hall
December 2004 ndash transfer to COSY hall (outside of the COSY tunnel)
May 2005 ndash tests after reassembling
Setup in the COSY hall
bull Supports representing
D1 and D2
bull New support bridge
bull Platform for all electronic and supply components
bull Heat exchanger with closed cooling-water circuit
June 2005 ndash setup ready
for installation at ANKE
September 14 2007 Ralf Engels 10
PIT installation at ANKE
Platform transportationABS transportation
September 14 2007 Ralf Engels 11
PIT at ANKE
September 14 2007 Ralf Engels 12
Magnetic stray field of D2
PIT setup with shielded components at ANKE
x
y
z
90150135
61530
302555
4026300
200550300
60100300
303355
calculated field strength (G)measured field strength (G)permissible field strength for the device given by the producer (G)
September 14 2007 Ralf Engels 13
Test of the medium-field rf transition unit
0 0 E + 0 0
5 0 E - 0 8
1 0 E - 0 7
1 5 E - 0 7
2 0 E - 0 7
2 5 E - 0 7
3 0 E - 0 7
0 200 400 600 800 1000 1200 1400D2 current A
Pre
ssu
re i
n t
he
targ
et c
ham
ber
e-7
mb
ar
H beam OFF H beam ON states 1 + 2 H beam ON state 1 only
30
25
20
15
10
05
00
field strength in the D2 gap0 T 158 T
0 0 E + 0 0
5 0 E - 0 8
1 0 E - 0 7
1 5 E - 0 7
2 0 E - 0 7
2 5 E - 0 7
3 0 E - 0 7
0 200 400 600 800 1000 1200 1400D2 current A
Pre
ssu
re i
n t
he
targ
et c
ham
ber
e-7
mb
ar
H beam OFF H beam ON states 1 + 2 H beam ON state 1 only
30
25
20
15
10
05
00
field strength in the D2 gap0 T 158 T
no ABS beam
MFT off (HFS 1 and 2)
MFT on (HFS 1 only)
September 14 2007 Ralf Engels 14
Do we have a zero field crossing
Magnetic field scan with ANKE at 53ordm using a 3D Hallprobe (Gatchina)
Bx By By |B|
Magnetic field along ABS axisbullID2=563 A (~ 06 T)
bullID1D3=129484 A
1 Determine the local Larmor precession frequency ωL
2 The angular velocity of the magnetic field ωB
As long as the ratio R=ωLωB is large the spin of the atom follows the field directionrarr no depolarization due to zero crossings
ωL
R=ωLωB
ωB
September 14 2007 Ralf Engels 15
Tuning of the Transition Units
Supporting bridge betweenD1 and D2
Additional shielding fromthe D2 stray fields
Cryopump at the target chamber
Polarimeter ionizer underthe target chamber
September 14 2007 Ralf Engels 16
First Polarization Measurement with the LSP
Problems
- The magnetic stray field of the D2 magnet deflected the produced protons
- The quantization axis was rotated by the stray field and the LSP measures
only the projection on the horizontal beam line
Next time More shielding and a rotatable Wien filter to compensate the
misalignment of the polarization axis
WFT was tuned online at the ANKE target position near the D2 magnet
The measured asymetry was stable during the beam time
September 14 2007 Ralf Engels 17
37middot10-840middot10-9With catcher
30middot10-740middot10-9Without catcher
With
ABS jet
Without
ABS jet
ABS beam catcher
~13cm~13cm
Measured pressures in the target chamber mbar
AB
S-j
et d
ensi
ty c
m-3
integral thickness ~ 15 1011 cm-2
ABS jet
COSY Beam
The ABS jet target
September 14 2007 Ralf Engels 18
Storage cell setup
COSYbeam
XY-table Frame with storage cell and aperture
Target chamber
Feeding tube l = 120 mm Oslash = 10 mm
Extraction tube l = 230 mm Oslash = 10 mm
Beam tube l = 400 mm 20x20 mm2
400mm400mm
September 14 2007 Ralf Engels 19
The COSY beam size
at injection
with an accelerated beam
no target with cluster target(density ~ 1014 atcm2)
9x12 mm 16x15 mm
36x16 mm
15 x 15 mm2
September 14 2007 Ralf Engels 20
Storage cell Final setup for the 1 Experiment
Tools for the experiment New storage cell amp support
(20bull20bull390 mm)
gt high target density gt unpolarized gas feeding system
LSP below the target chamber
gt online measurement of the ABS beam polarization
Silicon Tracking Telescope (STT)
gt measurement of spectator protonsnearby the storage cell center
September 14 2007 Ralf Engels 21
Cooler stacking with the storage cell
28 stacks followed by bull 2s electron cooling bull after 58s acceleration toTp=600 MeV
Cooler Stacking allows for higher polarized beam intensities with cell
Without storage cell 25middot1010 ions were reached
September 14 2007 Ralf Engels 22
Results of the cell tests
single injection 3557empty cell
26no cell80 stacking +
electron cooling
flattop
(600 MeV)after
coolinginjection
empty cell
no cell
target
92ordm
0ordm
ΘANKE
30 stacking + electron cooling
83
number of stored protons 10 9
2030 stacking +
electron cooling
1421single injection
injection type
30 stacking + electron cooling92ordm
cell with H gas from ABS
empty cell
64
6
9
September 14 2007 Ralf Engels 23
Storage cell and stochastically cooled beam
Cooling off
Cooling on
Tp= 831 MeV
September 14 2007 Ralf Engels 24
First Experimental Beam Time
Stacking rarr 120 injection with 10 s e-coolingFlat top rarr 30 min to have about 60 duty time
0 20 50Time min
September 14 2007 Ralf Engels 25
First Experimental Beam Time
Stacking rarr 120 injection with 10 s e-coolingFlat top rarr 30 min to have about 23 duty time
0 20 50Time min
Switching on the gasto feed the storage cell
Acceleration withoutgas in the storage cell
7 109 polarized deuterons in the ring with gas in the target
September 14 2007 Ralf Engels 26
Td=12 GeV target H (N2) gas
dprarrdp
dp rarr rarr
First Double Polarized Experiment dp dp rarr rarr
September 14 2007 Ralf Engels 27
First Double Polarized Experiment dp dp rarr rarr
Td=12 GeV target H (N2) gas
dprarr(dpsp) πo
quasi-free nprarrd
πo
(High amp Low branch)
High branch
Low branch
dp rarr rarr
September 14 2007 Ralf Engels 28
First Polarization Measurement of the Target
ANKE
preliminary
dp Td=12 GeV polarized H gas
quasi-free nprarrd
πo
(High amp Low branch)
ltQygt = 075 plusmn 006
θd=50-150 θd=150-220 θd=220-280 θd=280-400
θd=1550-1650 θd=1650-1700 θd=1700-1770
rarr
quasi-free
np rarr dπ0
(High and low branch)
ltQygt = 079 plusmn 007
September 14 2007 Ralf Engels 29
Summary of commissioning and first experiment
1 Cell-target thickness for H (hyperfine state 1) ~ 2 middot 1013 cm-2
3 ABS jet-target thickness ~ 15 middot 1011 cm-2
bull Tests at ANKE with ABS and storage cell
with stacking injection (Nov 2005) and stochastic cooling (Mar 2006)
2 Average luminosity for the storage-cell test ~ 1 middot 1029 cm-2 s-1
4 Hydrogen polarization in the cell ~ 079 +- 007
bull First experiment dprarrppn - JanFeb 2007rarrrarr
September 14 2007 Ralf Engels 30
Plans for the future
December 07 ndash PIT reinstallation With rotatable Wien filter and
better shielding of the LSP
JanFeb rsquo08 ndash Next beam time d prarr (pp)n at 2435 ndash 37 GeVc
(5 Weeks)
March rsquo08 ndash PIT deinstallation
ABS and LSP can be used for other experiments
- ISTC project 1860 Nuclear Polarization in H2D
2 molecules
- Direct Measurements of the Hyperfine levels
in the 2S12
2P12
state rarr Breit-Rabi diagram
rarr rarr
September 14 2007 Ralf Engels 31
Far Future Polarized Fusion
- First Experiments with the Polarized Internal Gas Target (PIT) at ANKECOSY
-
September 14 2007 Ralf Engels 10
PIT installation at ANKE
Platform transportationABS transportation
September 14 2007 Ralf Engels 11
PIT at ANKE
September 14 2007 Ralf Engels 12
Magnetic stray field of D2
PIT setup with shielded components at ANKE
x
y
z
90150135
61530
302555
4026300
200550300
60100300
303355
calculated field strength (G)measured field strength (G)permissible field strength for the device given by the producer (G)
September 14 2007 Ralf Engels 13
Test of the medium-field rf transition unit
0 0 E + 0 0
5 0 E - 0 8
1 0 E - 0 7
1 5 E - 0 7
2 0 E - 0 7
2 5 E - 0 7
3 0 E - 0 7
0 200 400 600 800 1000 1200 1400D2 current A
Pre
ssu
re i
n t
he
targ
et c
ham
ber
e-7
mb
ar
H beam OFF H beam ON states 1 + 2 H beam ON state 1 only
30
25
20
15
10
05
00
field strength in the D2 gap0 T 158 T
0 0 E + 0 0
5 0 E - 0 8
1 0 E - 0 7
1 5 E - 0 7
2 0 E - 0 7
2 5 E - 0 7
3 0 E - 0 7
0 200 400 600 800 1000 1200 1400D2 current A
Pre
ssu
re i
n t
he
targ
et c
ham
ber
e-7
mb
ar
H beam OFF H beam ON states 1 + 2 H beam ON state 1 only
30
25
20
15
10
05
00
field strength in the D2 gap0 T 158 T
no ABS beam
MFT off (HFS 1 and 2)
MFT on (HFS 1 only)
September 14 2007 Ralf Engels 14
Do we have a zero field crossing
Magnetic field scan with ANKE at 53ordm using a 3D Hallprobe (Gatchina)
Bx By By |B|
Magnetic field along ABS axisbullID2=563 A (~ 06 T)
bullID1D3=129484 A
1 Determine the local Larmor precession frequency ωL
2 The angular velocity of the magnetic field ωB
As long as the ratio R=ωLωB is large the spin of the atom follows the field directionrarr no depolarization due to zero crossings
ωL
R=ωLωB
ωB
September 14 2007 Ralf Engels 15
Tuning of the Transition Units
Supporting bridge betweenD1 and D2
Additional shielding fromthe D2 stray fields
Cryopump at the target chamber
Polarimeter ionizer underthe target chamber
September 14 2007 Ralf Engels 16
First Polarization Measurement with the LSP
Problems
- The magnetic stray field of the D2 magnet deflected the produced protons
- The quantization axis was rotated by the stray field and the LSP measures
only the projection on the horizontal beam line
Next time More shielding and a rotatable Wien filter to compensate the
misalignment of the polarization axis
WFT was tuned online at the ANKE target position near the D2 magnet
The measured asymetry was stable during the beam time
September 14 2007 Ralf Engels 17
37middot10-840middot10-9With catcher
30middot10-740middot10-9Without catcher
With
ABS jet
Without
ABS jet
ABS beam catcher
~13cm~13cm
Measured pressures in the target chamber mbar
AB
S-j
et d
ensi
ty c
m-3
integral thickness ~ 15 1011 cm-2
ABS jet
COSY Beam
The ABS jet target
September 14 2007 Ralf Engels 18
Storage cell setup
COSYbeam
XY-table Frame with storage cell and aperture
Target chamber
Feeding tube l = 120 mm Oslash = 10 mm
Extraction tube l = 230 mm Oslash = 10 mm
Beam tube l = 400 mm 20x20 mm2
400mm400mm
September 14 2007 Ralf Engels 19
The COSY beam size
at injection
with an accelerated beam
no target with cluster target(density ~ 1014 atcm2)
9x12 mm 16x15 mm
36x16 mm
15 x 15 mm2
September 14 2007 Ralf Engels 20
Storage cell Final setup for the 1 Experiment
Tools for the experiment New storage cell amp support
(20bull20bull390 mm)
gt high target density gt unpolarized gas feeding system
LSP below the target chamber
gt online measurement of the ABS beam polarization
Silicon Tracking Telescope (STT)
gt measurement of spectator protonsnearby the storage cell center
September 14 2007 Ralf Engels 21
Cooler stacking with the storage cell
28 stacks followed by bull 2s electron cooling bull after 58s acceleration toTp=600 MeV
Cooler Stacking allows for higher polarized beam intensities with cell
Without storage cell 25middot1010 ions were reached
September 14 2007 Ralf Engels 22
Results of the cell tests
single injection 3557empty cell
26no cell80 stacking +
electron cooling
flattop
(600 MeV)after
coolinginjection
empty cell
no cell
target
92ordm
0ordm
ΘANKE
30 stacking + electron cooling
83
number of stored protons 10 9
2030 stacking +
electron cooling
1421single injection
injection type
30 stacking + electron cooling92ordm
cell with H gas from ABS
empty cell
64
6
9
September 14 2007 Ralf Engels 23
Storage cell and stochastically cooled beam
Cooling off
Cooling on
Tp= 831 MeV
September 14 2007 Ralf Engels 24
First Experimental Beam Time
Stacking rarr 120 injection with 10 s e-coolingFlat top rarr 30 min to have about 60 duty time
0 20 50Time min
September 14 2007 Ralf Engels 25
First Experimental Beam Time
Stacking rarr 120 injection with 10 s e-coolingFlat top rarr 30 min to have about 23 duty time
0 20 50Time min
Switching on the gasto feed the storage cell
Acceleration withoutgas in the storage cell
7 109 polarized deuterons in the ring with gas in the target
September 14 2007 Ralf Engels 26
Td=12 GeV target H (N2) gas
dprarrdp
dp rarr rarr
First Double Polarized Experiment dp dp rarr rarr
September 14 2007 Ralf Engels 27
First Double Polarized Experiment dp dp rarr rarr
Td=12 GeV target H (N2) gas
dprarr(dpsp) πo
quasi-free nprarrd
πo
(High amp Low branch)
High branch
Low branch
dp rarr rarr
September 14 2007 Ralf Engels 28
First Polarization Measurement of the Target
ANKE
preliminary
dp Td=12 GeV polarized H gas
quasi-free nprarrd
πo
(High amp Low branch)
ltQygt = 075 plusmn 006
θd=50-150 θd=150-220 θd=220-280 θd=280-400
θd=1550-1650 θd=1650-1700 θd=1700-1770
rarr
quasi-free
np rarr dπ0
(High and low branch)
ltQygt = 079 plusmn 007
September 14 2007 Ralf Engels 29
Summary of commissioning and first experiment
1 Cell-target thickness for H (hyperfine state 1) ~ 2 middot 1013 cm-2
3 ABS jet-target thickness ~ 15 middot 1011 cm-2
bull Tests at ANKE with ABS and storage cell
with stacking injection (Nov 2005) and stochastic cooling (Mar 2006)
2 Average luminosity for the storage-cell test ~ 1 middot 1029 cm-2 s-1
4 Hydrogen polarization in the cell ~ 079 +- 007
bull First experiment dprarrppn - JanFeb 2007rarrrarr
September 14 2007 Ralf Engels 30
Plans for the future
December 07 ndash PIT reinstallation With rotatable Wien filter and
better shielding of the LSP
JanFeb rsquo08 ndash Next beam time d prarr (pp)n at 2435 ndash 37 GeVc
(5 Weeks)
March rsquo08 ndash PIT deinstallation
ABS and LSP can be used for other experiments
- ISTC project 1860 Nuclear Polarization in H2D
2 molecules
- Direct Measurements of the Hyperfine levels
in the 2S12
2P12
state rarr Breit-Rabi diagram
rarr rarr
September 14 2007 Ralf Engels 31
Far Future Polarized Fusion
- First Experiments with the Polarized Internal Gas Target (PIT) at ANKECOSY
-
September 14 2007 Ralf Engels 11
PIT at ANKE
September 14 2007 Ralf Engels 12
Magnetic stray field of D2
PIT setup with shielded components at ANKE
x
y
z
90150135
61530
302555
4026300
200550300
60100300
303355
calculated field strength (G)measured field strength (G)permissible field strength for the device given by the producer (G)
September 14 2007 Ralf Engels 13
Test of the medium-field rf transition unit
0 0 E + 0 0
5 0 E - 0 8
1 0 E - 0 7
1 5 E - 0 7
2 0 E - 0 7
2 5 E - 0 7
3 0 E - 0 7
0 200 400 600 800 1000 1200 1400D2 current A
Pre
ssu
re i
n t
he
targ
et c
ham
ber
e-7
mb
ar
H beam OFF H beam ON states 1 + 2 H beam ON state 1 only
30
25
20
15
10
05
00
field strength in the D2 gap0 T 158 T
0 0 E + 0 0
5 0 E - 0 8
1 0 E - 0 7
1 5 E - 0 7
2 0 E - 0 7
2 5 E - 0 7
3 0 E - 0 7
0 200 400 600 800 1000 1200 1400D2 current A
Pre
ssu
re i
n t
he
targ
et c
ham
ber
e-7
mb
ar
H beam OFF H beam ON states 1 + 2 H beam ON state 1 only
30
25
20
15
10
05
00
field strength in the D2 gap0 T 158 T
no ABS beam
MFT off (HFS 1 and 2)
MFT on (HFS 1 only)
September 14 2007 Ralf Engels 14
Do we have a zero field crossing
Magnetic field scan with ANKE at 53ordm using a 3D Hallprobe (Gatchina)
Bx By By |B|
Magnetic field along ABS axisbullID2=563 A (~ 06 T)
bullID1D3=129484 A
1 Determine the local Larmor precession frequency ωL
2 The angular velocity of the magnetic field ωB
As long as the ratio R=ωLωB is large the spin of the atom follows the field directionrarr no depolarization due to zero crossings
ωL
R=ωLωB
ωB
September 14 2007 Ralf Engels 15
Tuning of the Transition Units
Supporting bridge betweenD1 and D2
Additional shielding fromthe D2 stray fields
Cryopump at the target chamber
Polarimeter ionizer underthe target chamber
September 14 2007 Ralf Engels 16
First Polarization Measurement with the LSP
Problems
- The magnetic stray field of the D2 magnet deflected the produced protons
- The quantization axis was rotated by the stray field and the LSP measures
only the projection on the horizontal beam line
Next time More shielding and a rotatable Wien filter to compensate the
misalignment of the polarization axis
WFT was tuned online at the ANKE target position near the D2 magnet
The measured asymetry was stable during the beam time
September 14 2007 Ralf Engels 17
37middot10-840middot10-9With catcher
30middot10-740middot10-9Without catcher
With
ABS jet
Without
ABS jet
ABS beam catcher
~13cm~13cm
Measured pressures in the target chamber mbar
AB
S-j
et d
ensi
ty c
m-3
integral thickness ~ 15 1011 cm-2
ABS jet
COSY Beam
The ABS jet target
September 14 2007 Ralf Engels 18
Storage cell setup
COSYbeam
XY-table Frame with storage cell and aperture
Target chamber
Feeding tube l = 120 mm Oslash = 10 mm
Extraction tube l = 230 mm Oslash = 10 mm
Beam tube l = 400 mm 20x20 mm2
400mm400mm
September 14 2007 Ralf Engels 19
The COSY beam size
at injection
with an accelerated beam
no target with cluster target(density ~ 1014 atcm2)
9x12 mm 16x15 mm
36x16 mm
15 x 15 mm2
September 14 2007 Ralf Engels 20
Storage cell Final setup for the 1 Experiment
Tools for the experiment New storage cell amp support
(20bull20bull390 mm)
gt high target density gt unpolarized gas feeding system
LSP below the target chamber
gt online measurement of the ABS beam polarization
Silicon Tracking Telescope (STT)
gt measurement of spectator protonsnearby the storage cell center
September 14 2007 Ralf Engels 21
Cooler stacking with the storage cell
28 stacks followed by bull 2s electron cooling bull after 58s acceleration toTp=600 MeV
Cooler Stacking allows for higher polarized beam intensities with cell
Without storage cell 25middot1010 ions were reached
September 14 2007 Ralf Engels 22
Results of the cell tests
single injection 3557empty cell
26no cell80 stacking +
electron cooling
flattop
(600 MeV)after
coolinginjection
empty cell
no cell
target
92ordm
0ordm
ΘANKE
30 stacking + electron cooling
83
number of stored protons 10 9
2030 stacking +
electron cooling
1421single injection
injection type
30 stacking + electron cooling92ordm
cell with H gas from ABS
empty cell
64
6
9
September 14 2007 Ralf Engels 23
Storage cell and stochastically cooled beam
Cooling off
Cooling on
Tp= 831 MeV
September 14 2007 Ralf Engels 24
First Experimental Beam Time
Stacking rarr 120 injection with 10 s e-coolingFlat top rarr 30 min to have about 60 duty time
0 20 50Time min
September 14 2007 Ralf Engels 25
First Experimental Beam Time
Stacking rarr 120 injection with 10 s e-coolingFlat top rarr 30 min to have about 23 duty time
0 20 50Time min
Switching on the gasto feed the storage cell
Acceleration withoutgas in the storage cell
7 109 polarized deuterons in the ring with gas in the target
September 14 2007 Ralf Engels 26
Td=12 GeV target H (N2) gas
dprarrdp
dp rarr rarr
First Double Polarized Experiment dp dp rarr rarr
September 14 2007 Ralf Engels 27
First Double Polarized Experiment dp dp rarr rarr
Td=12 GeV target H (N2) gas
dprarr(dpsp) πo
quasi-free nprarrd
πo
(High amp Low branch)
High branch
Low branch
dp rarr rarr
September 14 2007 Ralf Engels 28
First Polarization Measurement of the Target
ANKE
preliminary
dp Td=12 GeV polarized H gas
quasi-free nprarrd
πo
(High amp Low branch)
ltQygt = 075 plusmn 006
θd=50-150 θd=150-220 θd=220-280 θd=280-400
θd=1550-1650 θd=1650-1700 θd=1700-1770
rarr
quasi-free
np rarr dπ0
(High and low branch)
ltQygt = 079 plusmn 007
September 14 2007 Ralf Engels 29
Summary of commissioning and first experiment
1 Cell-target thickness for H (hyperfine state 1) ~ 2 middot 1013 cm-2
3 ABS jet-target thickness ~ 15 middot 1011 cm-2
bull Tests at ANKE with ABS and storage cell
with stacking injection (Nov 2005) and stochastic cooling (Mar 2006)
2 Average luminosity for the storage-cell test ~ 1 middot 1029 cm-2 s-1
4 Hydrogen polarization in the cell ~ 079 +- 007
bull First experiment dprarrppn - JanFeb 2007rarrrarr
September 14 2007 Ralf Engels 30
Plans for the future
December 07 ndash PIT reinstallation With rotatable Wien filter and
better shielding of the LSP
JanFeb rsquo08 ndash Next beam time d prarr (pp)n at 2435 ndash 37 GeVc
(5 Weeks)
March rsquo08 ndash PIT deinstallation
ABS and LSP can be used for other experiments
- ISTC project 1860 Nuclear Polarization in H2D
2 molecules
- Direct Measurements of the Hyperfine levels
in the 2S12
2P12
state rarr Breit-Rabi diagram
rarr rarr
September 14 2007 Ralf Engels 31
Far Future Polarized Fusion
- First Experiments with the Polarized Internal Gas Target (PIT) at ANKECOSY
-
September 14 2007 Ralf Engels 12
Magnetic stray field of D2
PIT setup with shielded components at ANKE
x
y
z
90150135
61530
302555
4026300
200550300
60100300
303355
calculated field strength (G)measured field strength (G)permissible field strength for the device given by the producer (G)
September 14 2007 Ralf Engels 13
Test of the medium-field rf transition unit
0 0 E + 0 0
5 0 E - 0 8
1 0 E - 0 7
1 5 E - 0 7
2 0 E - 0 7
2 5 E - 0 7
3 0 E - 0 7
0 200 400 600 800 1000 1200 1400D2 current A
Pre
ssu
re i
n t
he
targ
et c
ham
ber
e-7
mb
ar
H beam OFF H beam ON states 1 + 2 H beam ON state 1 only
30
25
20
15
10
05
00
field strength in the D2 gap0 T 158 T
0 0 E + 0 0
5 0 E - 0 8
1 0 E - 0 7
1 5 E - 0 7
2 0 E - 0 7
2 5 E - 0 7
3 0 E - 0 7
0 200 400 600 800 1000 1200 1400D2 current A
Pre
ssu
re i
n t
he
targ
et c
ham
ber
e-7
mb
ar
H beam OFF H beam ON states 1 + 2 H beam ON state 1 only
30
25
20
15
10
05
00
field strength in the D2 gap0 T 158 T
no ABS beam
MFT off (HFS 1 and 2)
MFT on (HFS 1 only)
September 14 2007 Ralf Engels 14
Do we have a zero field crossing
Magnetic field scan with ANKE at 53ordm using a 3D Hallprobe (Gatchina)
Bx By By |B|
Magnetic field along ABS axisbullID2=563 A (~ 06 T)
bullID1D3=129484 A
1 Determine the local Larmor precession frequency ωL
2 The angular velocity of the magnetic field ωB
As long as the ratio R=ωLωB is large the spin of the atom follows the field directionrarr no depolarization due to zero crossings
ωL
R=ωLωB
ωB
September 14 2007 Ralf Engels 15
Tuning of the Transition Units
Supporting bridge betweenD1 and D2
Additional shielding fromthe D2 stray fields
Cryopump at the target chamber
Polarimeter ionizer underthe target chamber
September 14 2007 Ralf Engels 16
First Polarization Measurement with the LSP
Problems
- The magnetic stray field of the D2 magnet deflected the produced protons
- The quantization axis was rotated by the stray field and the LSP measures
only the projection on the horizontal beam line
Next time More shielding and a rotatable Wien filter to compensate the
misalignment of the polarization axis
WFT was tuned online at the ANKE target position near the D2 magnet
The measured asymetry was stable during the beam time
September 14 2007 Ralf Engels 17
37middot10-840middot10-9With catcher
30middot10-740middot10-9Without catcher
With
ABS jet
Without
ABS jet
ABS beam catcher
~13cm~13cm
Measured pressures in the target chamber mbar
AB
S-j
et d
ensi
ty c
m-3
integral thickness ~ 15 1011 cm-2
ABS jet
COSY Beam
The ABS jet target
September 14 2007 Ralf Engels 18
Storage cell setup
COSYbeam
XY-table Frame with storage cell and aperture
Target chamber
Feeding tube l = 120 mm Oslash = 10 mm
Extraction tube l = 230 mm Oslash = 10 mm
Beam tube l = 400 mm 20x20 mm2
400mm400mm
September 14 2007 Ralf Engels 19
The COSY beam size
at injection
with an accelerated beam
no target with cluster target(density ~ 1014 atcm2)
9x12 mm 16x15 mm
36x16 mm
15 x 15 mm2
September 14 2007 Ralf Engels 20
Storage cell Final setup for the 1 Experiment
Tools for the experiment New storage cell amp support
(20bull20bull390 mm)
gt high target density gt unpolarized gas feeding system
LSP below the target chamber
gt online measurement of the ABS beam polarization
Silicon Tracking Telescope (STT)
gt measurement of spectator protonsnearby the storage cell center
September 14 2007 Ralf Engels 21
Cooler stacking with the storage cell
28 stacks followed by bull 2s electron cooling bull after 58s acceleration toTp=600 MeV
Cooler Stacking allows for higher polarized beam intensities with cell
Without storage cell 25middot1010 ions were reached
September 14 2007 Ralf Engels 22
Results of the cell tests
single injection 3557empty cell
26no cell80 stacking +
electron cooling
flattop
(600 MeV)after
coolinginjection
empty cell
no cell
target
92ordm
0ordm
ΘANKE
30 stacking + electron cooling
83
number of stored protons 10 9
2030 stacking +
electron cooling
1421single injection
injection type
30 stacking + electron cooling92ordm
cell with H gas from ABS
empty cell
64
6
9
September 14 2007 Ralf Engels 23
Storage cell and stochastically cooled beam
Cooling off
Cooling on
Tp= 831 MeV
September 14 2007 Ralf Engels 24
First Experimental Beam Time
Stacking rarr 120 injection with 10 s e-coolingFlat top rarr 30 min to have about 60 duty time
0 20 50Time min
September 14 2007 Ralf Engels 25
First Experimental Beam Time
Stacking rarr 120 injection with 10 s e-coolingFlat top rarr 30 min to have about 23 duty time
0 20 50Time min
Switching on the gasto feed the storage cell
Acceleration withoutgas in the storage cell
7 109 polarized deuterons in the ring with gas in the target
September 14 2007 Ralf Engels 26
Td=12 GeV target H (N2) gas
dprarrdp
dp rarr rarr
First Double Polarized Experiment dp dp rarr rarr
September 14 2007 Ralf Engels 27
First Double Polarized Experiment dp dp rarr rarr
Td=12 GeV target H (N2) gas
dprarr(dpsp) πo
quasi-free nprarrd
πo
(High amp Low branch)
High branch
Low branch
dp rarr rarr
September 14 2007 Ralf Engels 28
First Polarization Measurement of the Target
ANKE
preliminary
dp Td=12 GeV polarized H gas
quasi-free nprarrd
πo
(High amp Low branch)
ltQygt = 075 plusmn 006
θd=50-150 θd=150-220 θd=220-280 θd=280-400
θd=1550-1650 θd=1650-1700 θd=1700-1770
rarr
quasi-free
np rarr dπ0
(High and low branch)
ltQygt = 079 plusmn 007
September 14 2007 Ralf Engels 29
Summary of commissioning and first experiment
1 Cell-target thickness for H (hyperfine state 1) ~ 2 middot 1013 cm-2
3 ABS jet-target thickness ~ 15 middot 1011 cm-2
bull Tests at ANKE with ABS and storage cell
with stacking injection (Nov 2005) and stochastic cooling (Mar 2006)
2 Average luminosity for the storage-cell test ~ 1 middot 1029 cm-2 s-1
4 Hydrogen polarization in the cell ~ 079 +- 007
bull First experiment dprarrppn - JanFeb 2007rarrrarr
September 14 2007 Ralf Engels 30
Plans for the future
December 07 ndash PIT reinstallation With rotatable Wien filter and
better shielding of the LSP
JanFeb rsquo08 ndash Next beam time d prarr (pp)n at 2435 ndash 37 GeVc
(5 Weeks)
March rsquo08 ndash PIT deinstallation
ABS and LSP can be used for other experiments
- ISTC project 1860 Nuclear Polarization in H2D
2 molecules
- Direct Measurements of the Hyperfine levels
in the 2S12
2P12
state rarr Breit-Rabi diagram
rarr rarr
September 14 2007 Ralf Engels 31
Far Future Polarized Fusion
- First Experiments with the Polarized Internal Gas Target (PIT) at ANKECOSY
-
September 14 2007 Ralf Engels 13
Test of the medium-field rf transition unit
0 0 E + 0 0
5 0 E - 0 8
1 0 E - 0 7
1 5 E - 0 7
2 0 E - 0 7
2 5 E - 0 7
3 0 E - 0 7
0 200 400 600 800 1000 1200 1400D2 current A
Pre
ssu
re i
n t
he
targ
et c
ham
ber
e-7
mb
ar
H beam OFF H beam ON states 1 + 2 H beam ON state 1 only
30
25
20
15
10
05
00
field strength in the D2 gap0 T 158 T
0 0 E + 0 0
5 0 E - 0 8
1 0 E - 0 7
1 5 E - 0 7
2 0 E - 0 7
2 5 E - 0 7
3 0 E - 0 7
0 200 400 600 800 1000 1200 1400D2 current A
Pre
ssu
re i
n t
he
targ
et c
ham
ber
e-7
mb
ar
H beam OFF H beam ON states 1 + 2 H beam ON state 1 only
30
25
20
15
10
05
00
field strength in the D2 gap0 T 158 T
no ABS beam
MFT off (HFS 1 and 2)
MFT on (HFS 1 only)
September 14 2007 Ralf Engels 14
Do we have a zero field crossing
Magnetic field scan with ANKE at 53ordm using a 3D Hallprobe (Gatchina)
Bx By By |B|
Magnetic field along ABS axisbullID2=563 A (~ 06 T)
bullID1D3=129484 A
1 Determine the local Larmor precession frequency ωL
2 The angular velocity of the magnetic field ωB
As long as the ratio R=ωLωB is large the spin of the atom follows the field directionrarr no depolarization due to zero crossings
ωL
R=ωLωB
ωB
September 14 2007 Ralf Engels 15
Tuning of the Transition Units
Supporting bridge betweenD1 and D2
Additional shielding fromthe D2 stray fields
Cryopump at the target chamber
Polarimeter ionizer underthe target chamber
September 14 2007 Ralf Engels 16
First Polarization Measurement with the LSP
Problems
- The magnetic stray field of the D2 magnet deflected the produced protons
- The quantization axis was rotated by the stray field and the LSP measures
only the projection on the horizontal beam line
Next time More shielding and a rotatable Wien filter to compensate the
misalignment of the polarization axis
WFT was tuned online at the ANKE target position near the D2 magnet
The measured asymetry was stable during the beam time
September 14 2007 Ralf Engels 17
37middot10-840middot10-9With catcher
30middot10-740middot10-9Without catcher
With
ABS jet
Without
ABS jet
ABS beam catcher
~13cm~13cm
Measured pressures in the target chamber mbar
AB
S-j
et d
ensi
ty c
m-3
integral thickness ~ 15 1011 cm-2
ABS jet
COSY Beam
The ABS jet target
September 14 2007 Ralf Engels 18
Storage cell setup
COSYbeam
XY-table Frame with storage cell and aperture
Target chamber
Feeding tube l = 120 mm Oslash = 10 mm
Extraction tube l = 230 mm Oslash = 10 mm
Beam tube l = 400 mm 20x20 mm2
400mm400mm
September 14 2007 Ralf Engels 19
The COSY beam size
at injection
with an accelerated beam
no target with cluster target(density ~ 1014 atcm2)
9x12 mm 16x15 mm
36x16 mm
15 x 15 mm2
September 14 2007 Ralf Engels 20
Storage cell Final setup for the 1 Experiment
Tools for the experiment New storage cell amp support
(20bull20bull390 mm)
gt high target density gt unpolarized gas feeding system
LSP below the target chamber
gt online measurement of the ABS beam polarization
Silicon Tracking Telescope (STT)
gt measurement of spectator protonsnearby the storage cell center
September 14 2007 Ralf Engels 21
Cooler stacking with the storage cell
28 stacks followed by bull 2s electron cooling bull after 58s acceleration toTp=600 MeV
Cooler Stacking allows for higher polarized beam intensities with cell
Without storage cell 25middot1010 ions were reached
September 14 2007 Ralf Engels 22
Results of the cell tests
single injection 3557empty cell
26no cell80 stacking +
electron cooling
flattop
(600 MeV)after
coolinginjection
empty cell
no cell
target
92ordm
0ordm
ΘANKE
30 stacking + electron cooling
83
number of stored protons 10 9
2030 stacking +
electron cooling
1421single injection
injection type
30 stacking + electron cooling92ordm
cell with H gas from ABS
empty cell
64
6
9
September 14 2007 Ralf Engels 23
Storage cell and stochastically cooled beam
Cooling off
Cooling on
Tp= 831 MeV
September 14 2007 Ralf Engels 24
First Experimental Beam Time
Stacking rarr 120 injection with 10 s e-coolingFlat top rarr 30 min to have about 60 duty time
0 20 50Time min
September 14 2007 Ralf Engels 25
First Experimental Beam Time
Stacking rarr 120 injection with 10 s e-coolingFlat top rarr 30 min to have about 23 duty time
0 20 50Time min
Switching on the gasto feed the storage cell
Acceleration withoutgas in the storage cell
7 109 polarized deuterons in the ring with gas in the target
September 14 2007 Ralf Engels 26
Td=12 GeV target H (N2) gas
dprarrdp
dp rarr rarr
First Double Polarized Experiment dp dp rarr rarr
September 14 2007 Ralf Engels 27
First Double Polarized Experiment dp dp rarr rarr
Td=12 GeV target H (N2) gas
dprarr(dpsp) πo
quasi-free nprarrd
πo
(High amp Low branch)
High branch
Low branch
dp rarr rarr
September 14 2007 Ralf Engels 28
First Polarization Measurement of the Target
ANKE
preliminary
dp Td=12 GeV polarized H gas
quasi-free nprarrd
πo
(High amp Low branch)
ltQygt = 075 plusmn 006
θd=50-150 θd=150-220 θd=220-280 θd=280-400
θd=1550-1650 θd=1650-1700 θd=1700-1770
rarr
quasi-free
np rarr dπ0
(High and low branch)
ltQygt = 079 plusmn 007
September 14 2007 Ralf Engels 29
Summary of commissioning and first experiment
1 Cell-target thickness for H (hyperfine state 1) ~ 2 middot 1013 cm-2
3 ABS jet-target thickness ~ 15 middot 1011 cm-2
bull Tests at ANKE with ABS and storage cell
with stacking injection (Nov 2005) and stochastic cooling (Mar 2006)
2 Average luminosity for the storage-cell test ~ 1 middot 1029 cm-2 s-1
4 Hydrogen polarization in the cell ~ 079 +- 007
bull First experiment dprarrppn - JanFeb 2007rarrrarr
September 14 2007 Ralf Engels 30
Plans for the future
December 07 ndash PIT reinstallation With rotatable Wien filter and
better shielding of the LSP
JanFeb rsquo08 ndash Next beam time d prarr (pp)n at 2435 ndash 37 GeVc
(5 Weeks)
March rsquo08 ndash PIT deinstallation
ABS and LSP can be used for other experiments
- ISTC project 1860 Nuclear Polarization in H2D
2 molecules
- Direct Measurements of the Hyperfine levels
in the 2S12
2P12
state rarr Breit-Rabi diagram
rarr rarr
September 14 2007 Ralf Engels 31
Far Future Polarized Fusion
- First Experiments with the Polarized Internal Gas Target (PIT) at ANKECOSY
-
September 14 2007 Ralf Engels 14
Do we have a zero field crossing
Magnetic field scan with ANKE at 53ordm using a 3D Hallprobe (Gatchina)
Bx By By |B|
Magnetic field along ABS axisbullID2=563 A (~ 06 T)
bullID1D3=129484 A
1 Determine the local Larmor precession frequency ωL
2 The angular velocity of the magnetic field ωB
As long as the ratio R=ωLωB is large the spin of the atom follows the field directionrarr no depolarization due to zero crossings
ωL
R=ωLωB
ωB
September 14 2007 Ralf Engels 15
Tuning of the Transition Units
Supporting bridge betweenD1 and D2
Additional shielding fromthe D2 stray fields
Cryopump at the target chamber
Polarimeter ionizer underthe target chamber
September 14 2007 Ralf Engels 16
First Polarization Measurement with the LSP
Problems
- The magnetic stray field of the D2 magnet deflected the produced protons
- The quantization axis was rotated by the stray field and the LSP measures
only the projection on the horizontal beam line
Next time More shielding and a rotatable Wien filter to compensate the
misalignment of the polarization axis
WFT was tuned online at the ANKE target position near the D2 magnet
The measured asymetry was stable during the beam time
September 14 2007 Ralf Engels 17
37middot10-840middot10-9With catcher
30middot10-740middot10-9Without catcher
With
ABS jet
Without
ABS jet
ABS beam catcher
~13cm~13cm
Measured pressures in the target chamber mbar
AB
S-j
et d
ensi
ty c
m-3
integral thickness ~ 15 1011 cm-2
ABS jet
COSY Beam
The ABS jet target
September 14 2007 Ralf Engels 18
Storage cell setup
COSYbeam
XY-table Frame with storage cell and aperture
Target chamber
Feeding tube l = 120 mm Oslash = 10 mm
Extraction tube l = 230 mm Oslash = 10 mm
Beam tube l = 400 mm 20x20 mm2
400mm400mm
September 14 2007 Ralf Engels 19
The COSY beam size
at injection
with an accelerated beam
no target with cluster target(density ~ 1014 atcm2)
9x12 mm 16x15 mm
36x16 mm
15 x 15 mm2
September 14 2007 Ralf Engels 20
Storage cell Final setup for the 1 Experiment
Tools for the experiment New storage cell amp support
(20bull20bull390 mm)
gt high target density gt unpolarized gas feeding system
LSP below the target chamber
gt online measurement of the ABS beam polarization
Silicon Tracking Telescope (STT)
gt measurement of spectator protonsnearby the storage cell center
September 14 2007 Ralf Engels 21
Cooler stacking with the storage cell
28 stacks followed by bull 2s electron cooling bull after 58s acceleration toTp=600 MeV
Cooler Stacking allows for higher polarized beam intensities with cell
Without storage cell 25middot1010 ions were reached
September 14 2007 Ralf Engels 22
Results of the cell tests
single injection 3557empty cell
26no cell80 stacking +
electron cooling
flattop
(600 MeV)after
coolinginjection
empty cell
no cell
target
92ordm
0ordm
ΘANKE
30 stacking + electron cooling
83
number of stored protons 10 9
2030 stacking +
electron cooling
1421single injection
injection type
30 stacking + electron cooling92ordm
cell with H gas from ABS
empty cell
64
6
9
September 14 2007 Ralf Engels 23
Storage cell and stochastically cooled beam
Cooling off
Cooling on
Tp= 831 MeV
September 14 2007 Ralf Engels 24
First Experimental Beam Time
Stacking rarr 120 injection with 10 s e-coolingFlat top rarr 30 min to have about 60 duty time
0 20 50Time min
September 14 2007 Ralf Engels 25
First Experimental Beam Time
Stacking rarr 120 injection with 10 s e-coolingFlat top rarr 30 min to have about 23 duty time
0 20 50Time min
Switching on the gasto feed the storage cell
Acceleration withoutgas in the storage cell
7 109 polarized deuterons in the ring with gas in the target
September 14 2007 Ralf Engels 26
Td=12 GeV target H (N2) gas
dprarrdp
dp rarr rarr
First Double Polarized Experiment dp dp rarr rarr
September 14 2007 Ralf Engels 27
First Double Polarized Experiment dp dp rarr rarr
Td=12 GeV target H (N2) gas
dprarr(dpsp) πo
quasi-free nprarrd
πo
(High amp Low branch)
High branch
Low branch
dp rarr rarr
September 14 2007 Ralf Engels 28
First Polarization Measurement of the Target
ANKE
preliminary
dp Td=12 GeV polarized H gas
quasi-free nprarrd
πo
(High amp Low branch)
ltQygt = 075 plusmn 006
θd=50-150 θd=150-220 θd=220-280 θd=280-400
θd=1550-1650 θd=1650-1700 θd=1700-1770
rarr
quasi-free
np rarr dπ0
(High and low branch)
ltQygt = 079 plusmn 007
September 14 2007 Ralf Engels 29
Summary of commissioning and first experiment
1 Cell-target thickness for H (hyperfine state 1) ~ 2 middot 1013 cm-2
3 ABS jet-target thickness ~ 15 middot 1011 cm-2
bull Tests at ANKE with ABS and storage cell
with stacking injection (Nov 2005) and stochastic cooling (Mar 2006)
2 Average luminosity for the storage-cell test ~ 1 middot 1029 cm-2 s-1
4 Hydrogen polarization in the cell ~ 079 +- 007
bull First experiment dprarrppn - JanFeb 2007rarrrarr
September 14 2007 Ralf Engels 30
Plans for the future
December 07 ndash PIT reinstallation With rotatable Wien filter and
better shielding of the LSP
JanFeb rsquo08 ndash Next beam time d prarr (pp)n at 2435 ndash 37 GeVc
(5 Weeks)
March rsquo08 ndash PIT deinstallation
ABS and LSP can be used for other experiments
- ISTC project 1860 Nuclear Polarization in H2D
2 molecules
- Direct Measurements of the Hyperfine levels
in the 2S12
2P12
state rarr Breit-Rabi diagram
rarr rarr
September 14 2007 Ralf Engels 31
Far Future Polarized Fusion
- First Experiments with the Polarized Internal Gas Target (PIT) at ANKECOSY
-
September 14 2007 Ralf Engels 15
Tuning of the Transition Units
Supporting bridge betweenD1 and D2
Additional shielding fromthe D2 stray fields
Cryopump at the target chamber
Polarimeter ionizer underthe target chamber
September 14 2007 Ralf Engels 16
First Polarization Measurement with the LSP
Problems
- The magnetic stray field of the D2 magnet deflected the produced protons
- The quantization axis was rotated by the stray field and the LSP measures
only the projection on the horizontal beam line
Next time More shielding and a rotatable Wien filter to compensate the
misalignment of the polarization axis
WFT was tuned online at the ANKE target position near the D2 magnet
The measured asymetry was stable during the beam time
September 14 2007 Ralf Engels 17
37middot10-840middot10-9With catcher
30middot10-740middot10-9Without catcher
With
ABS jet
Without
ABS jet
ABS beam catcher
~13cm~13cm
Measured pressures in the target chamber mbar
AB
S-j
et d
ensi
ty c
m-3
integral thickness ~ 15 1011 cm-2
ABS jet
COSY Beam
The ABS jet target
September 14 2007 Ralf Engels 18
Storage cell setup
COSYbeam
XY-table Frame with storage cell and aperture
Target chamber
Feeding tube l = 120 mm Oslash = 10 mm
Extraction tube l = 230 mm Oslash = 10 mm
Beam tube l = 400 mm 20x20 mm2
400mm400mm
September 14 2007 Ralf Engels 19
The COSY beam size
at injection
with an accelerated beam
no target with cluster target(density ~ 1014 atcm2)
9x12 mm 16x15 mm
36x16 mm
15 x 15 mm2
September 14 2007 Ralf Engels 20
Storage cell Final setup for the 1 Experiment
Tools for the experiment New storage cell amp support
(20bull20bull390 mm)
gt high target density gt unpolarized gas feeding system
LSP below the target chamber
gt online measurement of the ABS beam polarization
Silicon Tracking Telescope (STT)
gt measurement of spectator protonsnearby the storage cell center
September 14 2007 Ralf Engels 21
Cooler stacking with the storage cell
28 stacks followed by bull 2s electron cooling bull after 58s acceleration toTp=600 MeV
Cooler Stacking allows for higher polarized beam intensities with cell
Without storage cell 25middot1010 ions were reached
September 14 2007 Ralf Engels 22
Results of the cell tests
single injection 3557empty cell
26no cell80 stacking +
electron cooling
flattop
(600 MeV)after
coolinginjection
empty cell
no cell
target
92ordm
0ordm
ΘANKE
30 stacking + electron cooling
83
number of stored protons 10 9
2030 stacking +
electron cooling
1421single injection
injection type
30 stacking + electron cooling92ordm
cell with H gas from ABS
empty cell
64
6
9
September 14 2007 Ralf Engels 23
Storage cell and stochastically cooled beam
Cooling off
Cooling on
Tp= 831 MeV
September 14 2007 Ralf Engels 24
First Experimental Beam Time
Stacking rarr 120 injection with 10 s e-coolingFlat top rarr 30 min to have about 60 duty time
0 20 50Time min
September 14 2007 Ralf Engels 25
First Experimental Beam Time
Stacking rarr 120 injection with 10 s e-coolingFlat top rarr 30 min to have about 23 duty time
0 20 50Time min
Switching on the gasto feed the storage cell
Acceleration withoutgas in the storage cell
7 109 polarized deuterons in the ring with gas in the target
September 14 2007 Ralf Engels 26
Td=12 GeV target H (N2) gas
dprarrdp
dp rarr rarr
First Double Polarized Experiment dp dp rarr rarr
September 14 2007 Ralf Engels 27
First Double Polarized Experiment dp dp rarr rarr
Td=12 GeV target H (N2) gas
dprarr(dpsp) πo
quasi-free nprarrd
πo
(High amp Low branch)
High branch
Low branch
dp rarr rarr
September 14 2007 Ralf Engels 28
First Polarization Measurement of the Target
ANKE
preliminary
dp Td=12 GeV polarized H gas
quasi-free nprarrd
πo
(High amp Low branch)
ltQygt = 075 plusmn 006
θd=50-150 θd=150-220 θd=220-280 θd=280-400
θd=1550-1650 θd=1650-1700 θd=1700-1770
rarr
quasi-free
np rarr dπ0
(High and low branch)
ltQygt = 079 plusmn 007
September 14 2007 Ralf Engels 29
Summary of commissioning and first experiment
1 Cell-target thickness for H (hyperfine state 1) ~ 2 middot 1013 cm-2
3 ABS jet-target thickness ~ 15 middot 1011 cm-2
bull Tests at ANKE with ABS and storage cell
with stacking injection (Nov 2005) and stochastic cooling (Mar 2006)
2 Average luminosity for the storage-cell test ~ 1 middot 1029 cm-2 s-1
4 Hydrogen polarization in the cell ~ 079 +- 007
bull First experiment dprarrppn - JanFeb 2007rarrrarr
September 14 2007 Ralf Engels 30
Plans for the future
December 07 ndash PIT reinstallation With rotatable Wien filter and
better shielding of the LSP
JanFeb rsquo08 ndash Next beam time d prarr (pp)n at 2435 ndash 37 GeVc
(5 Weeks)
March rsquo08 ndash PIT deinstallation
ABS and LSP can be used for other experiments
- ISTC project 1860 Nuclear Polarization in H2D
2 molecules
- Direct Measurements of the Hyperfine levels
in the 2S12
2P12
state rarr Breit-Rabi diagram
rarr rarr
September 14 2007 Ralf Engels 31
Far Future Polarized Fusion
- First Experiments with the Polarized Internal Gas Target (PIT) at ANKECOSY
-
September 14 2007 Ralf Engels 16
First Polarization Measurement with the LSP
Problems
- The magnetic stray field of the D2 magnet deflected the produced protons
- The quantization axis was rotated by the stray field and the LSP measures
only the projection on the horizontal beam line
Next time More shielding and a rotatable Wien filter to compensate the
misalignment of the polarization axis
WFT was tuned online at the ANKE target position near the D2 magnet
The measured asymetry was stable during the beam time
September 14 2007 Ralf Engels 17
37middot10-840middot10-9With catcher
30middot10-740middot10-9Without catcher
With
ABS jet
Without
ABS jet
ABS beam catcher
~13cm~13cm
Measured pressures in the target chamber mbar
AB
S-j
et d
ensi
ty c
m-3
integral thickness ~ 15 1011 cm-2
ABS jet
COSY Beam
The ABS jet target
September 14 2007 Ralf Engels 18
Storage cell setup
COSYbeam
XY-table Frame with storage cell and aperture
Target chamber
Feeding tube l = 120 mm Oslash = 10 mm
Extraction tube l = 230 mm Oslash = 10 mm
Beam tube l = 400 mm 20x20 mm2
400mm400mm
September 14 2007 Ralf Engels 19
The COSY beam size
at injection
with an accelerated beam
no target with cluster target(density ~ 1014 atcm2)
9x12 mm 16x15 mm
36x16 mm
15 x 15 mm2
September 14 2007 Ralf Engels 20
Storage cell Final setup for the 1 Experiment
Tools for the experiment New storage cell amp support
(20bull20bull390 mm)
gt high target density gt unpolarized gas feeding system
LSP below the target chamber
gt online measurement of the ABS beam polarization
Silicon Tracking Telescope (STT)
gt measurement of spectator protonsnearby the storage cell center
September 14 2007 Ralf Engels 21
Cooler stacking with the storage cell
28 stacks followed by bull 2s electron cooling bull after 58s acceleration toTp=600 MeV
Cooler Stacking allows for higher polarized beam intensities with cell
Without storage cell 25middot1010 ions were reached
September 14 2007 Ralf Engels 22
Results of the cell tests
single injection 3557empty cell
26no cell80 stacking +
electron cooling
flattop
(600 MeV)after
coolinginjection
empty cell
no cell
target
92ordm
0ordm
ΘANKE
30 stacking + electron cooling
83
number of stored protons 10 9
2030 stacking +
electron cooling
1421single injection
injection type
30 stacking + electron cooling92ordm
cell with H gas from ABS
empty cell
64
6
9
September 14 2007 Ralf Engels 23
Storage cell and stochastically cooled beam
Cooling off
Cooling on
Tp= 831 MeV
September 14 2007 Ralf Engels 24
First Experimental Beam Time
Stacking rarr 120 injection with 10 s e-coolingFlat top rarr 30 min to have about 60 duty time
0 20 50Time min
September 14 2007 Ralf Engels 25
First Experimental Beam Time
Stacking rarr 120 injection with 10 s e-coolingFlat top rarr 30 min to have about 23 duty time
0 20 50Time min
Switching on the gasto feed the storage cell
Acceleration withoutgas in the storage cell
7 109 polarized deuterons in the ring with gas in the target
September 14 2007 Ralf Engels 26
Td=12 GeV target H (N2) gas
dprarrdp
dp rarr rarr
First Double Polarized Experiment dp dp rarr rarr
September 14 2007 Ralf Engels 27
First Double Polarized Experiment dp dp rarr rarr
Td=12 GeV target H (N2) gas
dprarr(dpsp) πo
quasi-free nprarrd
πo
(High amp Low branch)
High branch
Low branch
dp rarr rarr
September 14 2007 Ralf Engels 28
First Polarization Measurement of the Target
ANKE
preliminary
dp Td=12 GeV polarized H gas
quasi-free nprarrd
πo
(High amp Low branch)
ltQygt = 075 plusmn 006
θd=50-150 θd=150-220 θd=220-280 θd=280-400
θd=1550-1650 θd=1650-1700 θd=1700-1770
rarr
quasi-free
np rarr dπ0
(High and low branch)
ltQygt = 079 plusmn 007
September 14 2007 Ralf Engels 29
Summary of commissioning and first experiment
1 Cell-target thickness for H (hyperfine state 1) ~ 2 middot 1013 cm-2
3 ABS jet-target thickness ~ 15 middot 1011 cm-2
bull Tests at ANKE with ABS and storage cell
with stacking injection (Nov 2005) and stochastic cooling (Mar 2006)
2 Average luminosity for the storage-cell test ~ 1 middot 1029 cm-2 s-1
4 Hydrogen polarization in the cell ~ 079 +- 007
bull First experiment dprarrppn - JanFeb 2007rarrrarr
September 14 2007 Ralf Engels 30
Plans for the future
December 07 ndash PIT reinstallation With rotatable Wien filter and
better shielding of the LSP
JanFeb rsquo08 ndash Next beam time d prarr (pp)n at 2435 ndash 37 GeVc
(5 Weeks)
March rsquo08 ndash PIT deinstallation
ABS and LSP can be used for other experiments
- ISTC project 1860 Nuclear Polarization in H2D
2 molecules
- Direct Measurements of the Hyperfine levels
in the 2S12
2P12
state rarr Breit-Rabi diagram
rarr rarr
September 14 2007 Ralf Engels 31
Far Future Polarized Fusion
- First Experiments with the Polarized Internal Gas Target (PIT) at ANKECOSY
-
September 14 2007 Ralf Engels 17
37middot10-840middot10-9With catcher
30middot10-740middot10-9Without catcher
With
ABS jet
Without
ABS jet
ABS beam catcher
~13cm~13cm
Measured pressures in the target chamber mbar
AB
S-j
et d
ensi
ty c
m-3
integral thickness ~ 15 1011 cm-2
ABS jet
COSY Beam
The ABS jet target
September 14 2007 Ralf Engels 18
Storage cell setup
COSYbeam
XY-table Frame with storage cell and aperture
Target chamber
Feeding tube l = 120 mm Oslash = 10 mm
Extraction tube l = 230 mm Oslash = 10 mm
Beam tube l = 400 mm 20x20 mm2
400mm400mm
September 14 2007 Ralf Engels 19
The COSY beam size
at injection
with an accelerated beam
no target with cluster target(density ~ 1014 atcm2)
9x12 mm 16x15 mm
36x16 mm
15 x 15 mm2
September 14 2007 Ralf Engels 20
Storage cell Final setup for the 1 Experiment
Tools for the experiment New storage cell amp support
(20bull20bull390 mm)
gt high target density gt unpolarized gas feeding system
LSP below the target chamber
gt online measurement of the ABS beam polarization
Silicon Tracking Telescope (STT)
gt measurement of spectator protonsnearby the storage cell center
September 14 2007 Ralf Engels 21
Cooler stacking with the storage cell
28 stacks followed by bull 2s electron cooling bull after 58s acceleration toTp=600 MeV
Cooler Stacking allows for higher polarized beam intensities with cell
Without storage cell 25middot1010 ions were reached
September 14 2007 Ralf Engels 22
Results of the cell tests
single injection 3557empty cell
26no cell80 stacking +
electron cooling
flattop
(600 MeV)after
coolinginjection
empty cell
no cell
target
92ordm
0ordm
ΘANKE
30 stacking + electron cooling
83
number of stored protons 10 9
2030 stacking +
electron cooling
1421single injection
injection type
30 stacking + electron cooling92ordm
cell with H gas from ABS
empty cell
64
6
9
September 14 2007 Ralf Engels 23
Storage cell and stochastically cooled beam
Cooling off
Cooling on
Tp= 831 MeV
September 14 2007 Ralf Engels 24
First Experimental Beam Time
Stacking rarr 120 injection with 10 s e-coolingFlat top rarr 30 min to have about 60 duty time
0 20 50Time min
September 14 2007 Ralf Engels 25
First Experimental Beam Time
Stacking rarr 120 injection with 10 s e-coolingFlat top rarr 30 min to have about 23 duty time
0 20 50Time min
Switching on the gasto feed the storage cell
Acceleration withoutgas in the storage cell
7 109 polarized deuterons in the ring with gas in the target
September 14 2007 Ralf Engels 26
Td=12 GeV target H (N2) gas
dprarrdp
dp rarr rarr
First Double Polarized Experiment dp dp rarr rarr
September 14 2007 Ralf Engels 27
First Double Polarized Experiment dp dp rarr rarr
Td=12 GeV target H (N2) gas
dprarr(dpsp) πo
quasi-free nprarrd
πo
(High amp Low branch)
High branch
Low branch
dp rarr rarr
September 14 2007 Ralf Engels 28
First Polarization Measurement of the Target
ANKE
preliminary
dp Td=12 GeV polarized H gas
quasi-free nprarrd
πo
(High amp Low branch)
ltQygt = 075 plusmn 006
θd=50-150 θd=150-220 θd=220-280 θd=280-400
θd=1550-1650 θd=1650-1700 θd=1700-1770
rarr
quasi-free
np rarr dπ0
(High and low branch)
ltQygt = 079 plusmn 007
September 14 2007 Ralf Engels 29
Summary of commissioning and first experiment
1 Cell-target thickness for H (hyperfine state 1) ~ 2 middot 1013 cm-2
3 ABS jet-target thickness ~ 15 middot 1011 cm-2
bull Tests at ANKE with ABS and storage cell
with stacking injection (Nov 2005) and stochastic cooling (Mar 2006)
2 Average luminosity for the storage-cell test ~ 1 middot 1029 cm-2 s-1
4 Hydrogen polarization in the cell ~ 079 +- 007
bull First experiment dprarrppn - JanFeb 2007rarrrarr
September 14 2007 Ralf Engels 30
Plans for the future
December 07 ndash PIT reinstallation With rotatable Wien filter and
better shielding of the LSP
JanFeb rsquo08 ndash Next beam time d prarr (pp)n at 2435 ndash 37 GeVc
(5 Weeks)
March rsquo08 ndash PIT deinstallation
ABS and LSP can be used for other experiments
- ISTC project 1860 Nuclear Polarization in H2D
2 molecules
- Direct Measurements of the Hyperfine levels
in the 2S12
2P12
state rarr Breit-Rabi diagram
rarr rarr
September 14 2007 Ralf Engels 31
Far Future Polarized Fusion
- First Experiments with the Polarized Internal Gas Target (PIT) at ANKECOSY
-
September 14 2007 Ralf Engels 18
Storage cell setup
COSYbeam
XY-table Frame with storage cell and aperture
Target chamber
Feeding tube l = 120 mm Oslash = 10 mm
Extraction tube l = 230 mm Oslash = 10 mm
Beam tube l = 400 mm 20x20 mm2
400mm400mm
September 14 2007 Ralf Engels 19
The COSY beam size
at injection
with an accelerated beam
no target with cluster target(density ~ 1014 atcm2)
9x12 mm 16x15 mm
36x16 mm
15 x 15 mm2
September 14 2007 Ralf Engels 20
Storage cell Final setup for the 1 Experiment
Tools for the experiment New storage cell amp support
(20bull20bull390 mm)
gt high target density gt unpolarized gas feeding system
LSP below the target chamber
gt online measurement of the ABS beam polarization
Silicon Tracking Telescope (STT)
gt measurement of spectator protonsnearby the storage cell center
September 14 2007 Ralf Engels 21
Cooler stacking with the storage cell
28 stacks followed by bull 2s electron cooling bull after 58s acceleration toTp=600 MeV
Cooler Stacking allows for higher polarized beam intensities with cell
Without storage cell 25middot1010 ions were reached
September 14 2007 Ralf Engels 22
Results of the cell tests
single injection 3557empty cell
26no cell80 stacking +
electron cooling
flattop
(600 MeV)after
coolinginjection
empty cell
no cell
target
92ordm
0ordm
ΘANKE
30 stacking + electron cooling
83
number of stored protons 10 9
2030 stacking +
electron cooling
1421single injection
injection type
30 stacking + electron cooling92ordm
cell with H gas from ABS
empty cell
64
6
9
September 14 2007 Ralf Engels 23
Storage cell and stochastically cooled beam
Cooling off
Cooling on
Tp= 831 MeV
September 14 2007 Ralf Engels 24
First Experimental Beam Time
Stacking rarr 120 injection with 10 s e-coolingFlat top rarr 30 min to have about 60 duty time
0 20 50Time min
September 14 2007 Ralf Engels 25
First Experimental Beam Time
Stacking rarr 120 injection with 10 s e-coolingFlat top rarr 30 min to have about 23 duty time
0 20 50Time min
Switching on the gasto feed the storage cell
Acceleration withoutgas in the storage cell
7 109 polarized deuterons in the ring with gas in the target
September 14 2007 Ralf Engels 26
Td=12 GeV target H (N2) gas
dprarrdp
dp rarr rarr
First Double Polarized Experiment dp dp rarr rarr
September 14 2007 Ralf Engels 27
First Double Polarized Experiment dp dp rarr rarr
Td=12 GeV target H (N2) gas
dprarr(dpsp) πo
quasi-free nprarrd
πo
(High amp Low branch)
High branch
Low branch
dp rarr rarr
September 14 2007 Ralf Engels 28
First Polarization Measurement of the Target
ANKE
preliminary
dp Td=12 GeV polarized H gas
quasi-free nprarrd
πo
(High amp Low branch)
ltQygt = 075 plusmn 006
θd=50-150 θd=150-220 θd=220-280 θd=280-400
θd=1550-1650 θd=1650-1700 θd=1700-1770
rarr
quasi-free
np rarr dπ0
(High and low branch)
ltQygt = 079 plusmn 007
September 14 2007 Ralf Engels 29
Summary of commissioning and first experiment
1 Cell-target thickness for H (hyperfine state 1) ~ 2 middot 1013 cm-2
3 ABS jet-target thickness ~ 15 middot 1011 cm-2
bull Tests at ANKE with ABS and storage cell
with stacking injection (Nov 2005) and stochastic cooling (Mar 2006)
2 Average luminosity for the storage-cell test ~ 1 middot 1029 cm-2 s-1
4 Hydrogen polarization in the cell ~ 079 +- 007
bull First experiment dprarrppn - JanFeb 2007rarrrarr
September 14 2007 Ralf Engels 30
Plans for the future
December 07 ndash PIT reinstallation With rotatable Wien filter and
better shielding of the LSP
JanFeb rsquo08 ndash Next beam time d prarr (pp)n at 2435 ndash 37 GeVc
(5 Weeks)
March rsquo08 ndash PIT deinstallation
ABS and LSP can be used for other experiments
- ISTC project 1860 Nuclear Polarization in H2D
2 molecules
- Direct Measurements of the Hyperfine levels
in the 2S12
2P12
state rarr Breit-Rabi diagram
rarr rarr
September 14 2007 Ralf Engels 31
Far Future Polarized Fusion
- First Experiments with the Polarized Internal Gas Target (PIT) at ANKECOSY
-
September 14 2007 Ralf Engels 19
The COSY beam size
at injection
with an accelerated beam
no target with cluster target(density ~ 1014 atcm2)
9x12 mm 16x15 mm
36x16 mm
15 x 15 mm2
September 14 2007 Ralf Engels 20
Storage cell Final setup for the 1 Experiment
Tools for the experiment New storage cell amp support
(20bull20bull390 mm)
gt high target density gt unpolarized gas feeding system
LSP below the target chamber
gt online measurement of the ABS beam polarization
Silicon Tracking Telescope (STT)
gt measurement of spectator protonsnearby the storage cell center
September 14 2007 Ralf Engels 21
Cooler stacking with the storage cell
28 stacks followed by bull 2s electron cooling bull after 58s acceleration toTp=600 MeV
Cooler Stacking allows for higher polarized beam intensities with cell
Without storage cell 25middot1010 ions were reached
September 14 2007 Ralf Engels 22
Results of the cell tests
single injection 3557empty cell
26no cell80 stacking +
electron cooling
flattop
(600 MeV)after
coolinginjection
empty cell
no cell
target
92ordm
0ordm
ΘANKE
30 stacking + electron cooling
83
number of stored protons 10 9
2030 stacking +
electron cooling
1421single injection
injection type
30 stacking + electron cooling92ordm
cell with H gas from ABS
empty cell
64
6
9
September 14 2007 Ralf Engels 23
Storage cell and stochastically cooled beam
Cooling off
Cooling on
Tp= 831 MeV
September 14 2007 Ralf Engels 24
First Experimental Beam Time
Stacking rarr 120 injection with 10 s e-coolingFlat top rarr 30 min to have about 60 duty time
0 20 50Time min
September 14 2007 Ralf Engels 25
First Experimental Beam Time
Stacking rarr 120 injection with 10 s e-coolingFlat top rarr 30 min to have about 23 duty time
0 20 50Time min
Switching on the gasto feed the storage cell
Acceleration withoutgas in the storage cell
7 109 polarized deuterons in the ring with gas in the target
September 14 2007 Ralf Engels 26
Td=12 GeV target H (N2) gas
dprarrdp
dp rarr rarr
First Double Polarized Experiment dp dp rarr rarr
September 14 2007 Ralf Engels 27
First Double Polarized Experiment dp dp rarr rarr
Td=12 GeV target H (N2) gas
dprarr(dpsp) πo
quasi-free nprarrd
πo
(High amp Low branch)
High branch
Low branch
dp rarr rarr
September 14 2007 Ralf Engels 28
First Polarization Measurement of the Target
ANKE
preliminary
dp Td=12 GeV polarized H gas
quasi-free nprarrd
πo
(High amp Low branch)
ltQygt = 075 plusmn 006
θd=50-150 θd=150-220 θd=220-280 θd=280-400
θd=1550-1650 θd=1650-1700 θd=1700-1770
rarr
quasi-free
np rarr dπ0
(High and low branch)
ltQygt = 079 plusmn 007
September 14 2007 Ralf Engels 29
Summary of commissioning and first experiment
1 Cell-target thickness for H (hyperfine state 1) ~ 2 middot 1013 cm-2
3 ABS jet-target thickness ~ 15 middot 1011 cm-2
bull Tests at ANKE with ABS and storage cell
with stacking injection (Nov 2005) and stochastic cooling (Mar 2006)
2 Average luminosity for the storage-cell test ~ 1 middot 1029 cm-2 s-1
4 Hydrogen polarization in the cell ~ 079 +- 007
bull First experiment dprarrppn - JanFeb 2007rarrrarr
September 14 2007 Ralf Engels 30
Plans for the future
December 07 ndash PIT reinstallation With rotatable Wien filter and
better shielding of the LSP
JanFeb rsquo08 ndash Next beam time d prarr (pp)n at 2435 ndash 37 GeVc
(5 Weeks)
March rsquo08 ndash PIT deinstallation
ABS and LSP can be used for other experiments
- ISTC project 1860 Nuclear Polarization in H2D
2 molecules
- Direct Measurements of the Hyperfine levels
in the 2S12
2P12
state rarr Breit-Rabi diagram
rarr rarr
September 14 2007 Ralf Engels 31
Far Future Polarized Fusion
- First Experiments with the Polarized Internal Gas Target (PIT) at ANKECOSY
-
September 14 2007 Ralf Engels 20
Storage cell Final setup for the 1 Experiment
Tools for the experiment New storage cell amp support
(20bull20bull390 mm)
gt high target density gt unpolarized gas feeding system
LSP below the target chamber
gt online measurement of the ABS beam polarization
Silicon Tracking Telescope (STT)
gt measurement of spectator protonsnearby the storage cell center
September 14 2007 Ralf Engels 21
Cooler stacking with the storage cell
28 stacks followed by bull 2s electron cooling bull after 58s acceleration toTp=600 MeV
Cooler Stacking allows for higher polarized beam intensities with cell
Without storage cell 25middot1010 ions were reached
September 14 2007 Ralf Engels 22
Results of the cell tests
single injection 3557empty cell
26no cell80 stacking +
electron cooling
flattop
(600 MeV)after
coolinginjection
empty cell
no cell
target
92ordm
0ordm
ΘANKE
30 stacking + electron cooling
83
number of stored protons 10 9
2030 stacking +
electron cooling
1421single injection
injection type
30 stacking + electron cooling92ordm
cell with H gas from ABS
empty cell
64
6
9
September 14 2007 Ralf Engels 23
Storage cell and stochastically cooled beam
Cooling off
Cooling on
Tp= 831 MeV
September 14 2007 Ralf Engels 24
First Experimental Beam Time
Stacking rarr 120 injection with 10 s e-coolingFlat top rarr 30 min to have about 60 duty time
0 20 50Time min
September 14 2007 Ralf Engels 25
First Experimental Beam Time
Stacking rarr 120 injection with 10 s e-coolingFlat top rarr 30 min to have about 23 duty time
0 20 50Time min
Switching on the gasto feed the storage cell
Acceleration withoutgas in the storage cell
7 109 polarized deuterons in the ring with gas in the target
September 14 2007 Ralf Engels 26
Td=12 GeV target H (N2) gas
dprarrdp
dp rarr rarr
First Double Polarized Experiment dp dp rarr rarr
September 14 2007 Ralf Engels 27
First Double Polarized Experiment dp dp rarr rarr
Td=12 GeV target H (N2) gas
dprarr(dpsp) πo
quasi-free nprarrd
πo
(High amp Low branch)
High branch
Low branch
dp rarr rarr
September 14 2007 Ralf Engels 28
First Polarization Measurement of the Target
ANKE
preliminary
dp Td=12 GeV polarized H gas
quasi-free nprarrd
πo
(High amp Low branch)
ltQygt = 075 plusmn 006
θd=50-150 θd=150-220 θd=220-280 θd=280-400
θd=1550-1650 θd=1650-1700 θd=1700-1770
rarr
quasi-free
np rarr dπ0
(High and low branch)
ltQygt = 079 plusmn 007
September 14 2007 Ralf Engels 29
Summary of commissioning and first experiment
1 Cell-target thickness for H (hyperfine state 1) ~ 2 middot 1013 cm-2
3 ABS jet-target thickness ~ 15 middot 1011 cm-2
bull Tests at ANKE with ABS and storage cell
with stacking injection (Nov 2005) and stochastic cooling (Mar 2006)
2 Average luminosity for the storage-cell test ~ 1 middot 1029 cm-2 s-1
4 Hydrogen polarization in the cell ~ 079 +- 007
bull First experiment dprarrppn - JanFeb 2007rarrrarr
September 14 2007 Ralf Engels 30
Plans for the future
December 07 ndash PIT reinstallation With rotatable Wien filter and
better shielding of the LSP
JanFeb rsquo08 ndash Next beam time d prarr (pp)n at 2435 ndash 37 GeVc
(5 Weeks)
March rsquo08 ndash PIT deinstallation
ABS and LSP can be used for other experiments
- ISTC project 1860 Nuclear Polarization in H2D
2 molecules
- Direct Measurements of the Hyperfine levels
in the 2S12
2P12
state rarr Breit-Rabi diagram
rarr rarr
September 14 2007 Ralf Engels 31
Far Future Polarized Fusion
- First Experiments with the Polarized Internal Gas Target (PIT) at ANKECOSY
-
September 14 2007 Ralf Engels 21
Cooler stacking with the storage cell
28 stacks followed by bull 2s electron cooling bull after 58s acceleration toTp=600 MeV
Cooler Stacking allows for higher polarized beam intensities with cell
Without storage cell 25middot1010 ions were reached
September 14 2007 Ralf Engels 22
Results of the cell tests
single injection 3557empty cell
26no cell80 stacking +
electron cooling
flattop
(600 MeV)after
coolinginjection
empty cell
no cell
target
92ordm
0ordm
ΘANKE
30 stacking + electron cooling
83
number of stored protons 10 9
2030 stacking +
electron cooling
1421single injection
injection type
30 stacking + electron cooling92ordm
cell with H gas from ABS
empty cell
64
6
9
September 14 2007 Ralf Engels 23
Storage cell and stochastically cooled beam
Cooling off
Cooling on
Tp= 831 MeV
September 14 2007 Ralf Engels 24
First Experimental Beam Time
Stacking rarr 120 injection with 10 s e-coolingFlat top rarr 30 min to have about 60 duty time
0 20 50Time min
September 14 2007 Ralf Engels 25
First Experimental Beam Time
Stacking rarr 120 injection with 10 s e-coolingFlat top rarr 30 min to have about 23 duty time
0 20 50Time min
Switching on the gasto feed the storage cell
Acceleration withoutgas in the storage cell
7 109 polarized deuterons in the ring with gas in the target
September 14 2007 Ralf Engels 26
Td=12 GeV target H (N2) gas
dprarrdp
dp rarr rarr
First Double Polarized Experiment dp dp rarr rarr
September 14 2007 Ralf Engels 27
First Double Polarized Experiment dp dp rarr rarr
Td=12 GeV target H (N2) gas
dprarr(dpsp) πo
quasi-free nprarrd
πo
(High amp Low branch)
High branch
Low branch
dp rarr rarr
September 14 2007 Ralf Engels 28
First Polarization Measurement of the Target
ANKE
preliminary
dp Td=12 GeV polarized H gas
quasi-free nprarrd
πo
(High amp Low branch)
ltQygt = 075 plusmn 006
θd=50-150 θd=150-220 θd=220-280 θd=280-400
θd=1550-1650 θd=1650-1700 θd=1700-1770
rarr
quasi-free
np rarr dπ0
(High and low branch)
ltQygt = 079 plusmn 007
September 14 2007 Ralf Engels 29
Summary of commissioning and first experiment
1 Cell-target thickness for H (hyperfine state 1) ~ 2 middot 1013 cm-2
3 ABS jet-target thickness ~ 15 middot 1011 cm-2
bull Tests at ANKE with ABS and storage cell
with stacking injection (Nov 2005) and stochastic cooling (Mar 2006)
2 Average luminosity for the storage-cell test ~ 1 middot 1029 cm-2 s-1
4 Hydrogen polarization in the cell ~ 079 +- 007
bull First experiment dprarrppn - JanFeb 2007rarrrarr
September 14 2007 Ralf Engels 30
Plans for the future
December 07 ndash PIT reinstallation With rotatable Wien filter and
better shielding of the LSP
JanFeb rsquo08 ndash Next beam time d prarr (pp)n at 2435 ndash 37 GeVc
(5 Weeks)
March rsquo08 ndash PIT deinstallation
ABS and LSP can be used for other experiments
- ISTC project 1860 Nuclear Polarization in H2D
2 molecules
- Direct Measurements of the Hyperfine levels
in the 2S12
2P12
state rarr Breit-Rabi diagram
rarr rarr
September 14 2007 Ralf Engels 31
Far Future Polarized Fusion
- First Experiments with the Polarized Internal Gas Target (PIT) at ANKECOSY
-
September 14 2007 Ralf Engels 22
Results of the cell tests
single injection 3557empty cell
26no cell80 stacking +
electron cooling
flattop
(600 MeV)after
coolinginjection
empty cell
no cell
target
92ordm
0ordm
ΘANKE
30 stacking + electron cooling
83
number of stored protons 10 9
2030 stacking +
electron cooling
1421single injection
injection type
30 stacking + electron cooling92ordm
cell with H gas from ABS
empty cell
64
6
9
September 14 2007 Ralf Engels 23
Storage cell and stochastically cooled beam
Cooling off
Cooling on
Tp= 831 MeV
September 14 2007 Ralf Engels 24
First Experimental Beam Time
Stacking rarr 120 injection with 10 s e-coolingFlat top rarr 30 min to have about 60 duty time
0 20 50Time min
September 14 2007 Ralf Engels 25
First Experimental Beam Time
Stacking rarr 120 injection with 10 s e-coolingFlat top rarr 30 min to have about 23 duty time
0 20 50Time min
Switching on the gasto feed the storage cell
Acceleration withoutgas in the storage cell
7 109 polarized deuterons in the ring with gas in the target
September 14 2007 Ralf Engels 26
Td=12 GeV target H (N2) gas
dprarrdp
dp rarr rarr
First Double Polarized Experiment dp dp rarr rarr
September 14 2007 Ralf Engels 27
First Double Polarized Experiment dp dp rarr rarr
Td=12 GeV target H (N2) gas
dprarr(dpsp) πo
quasi-free nprarrd
πo
(High amp Low branch)
High branch
Low branch
dp rarr rarr
September 14 2007 Ralf Engels 28
First Polarization Measurement of the Target
ANKE
preliminary
dp Td=12 GeV polarized H gas
quasi-free nprarrd
πo
(High amp Low branch)
ltQygt = 075 plusmn 006
θd=50-150 θd=150-220 θd=220-280 θd=280-400
θd=1550-1650 θd=1650-1700 θd=1700-1770
rarr
quasi-free
np rarr dπ0
(High and low branch)
ltQygt = 079 plusmn 007
September 14 2007 Ralf Engels 29
Summary of commissioning and first experiment
1 Cell-target thickness for H (hyperfine state 1) ~ 2 middot 1013 cm-2
3 ABS jet-target thickness ~ 15 middot 1011 cm-2
bull Tests at ANKE with ABS and storage cell
with stacking injection (Nov 2005) and stochastic cooling (Mar 2006)
2 Average luminosity for the storage-cell test ~ 1 middot 1029 cm-2 s-1
4 Hydrogen polarization in the cell ~ 079 +- 007
bull First experiment dprarrppn - JanFeb 2007rarrrarr
September 14 2007 Ralf Engels 30
Plans for the future
December 07 ndash PIT reinstallation With rotatable Wien filter and
better shielding of the LSP
JanFeb rsquo08 ndash Next beam time d prarr (pp)n at 2435 ndash 37 GeVc
(5 Weeks)
March rsquo08 ndash PIT deinstallation
ABS and LSP can be used for other experiments
- ISTC project 1860 Nuclear Polarization in H2D
2 molecules
- Direct Measurements of the Hyperfine levels
in the 2S12
2P12
state rarr Breit-Rabi diagram
rarr rarr
September 14 2007 Ralf Engels 31
Far Future Polarized Fusion
- First Experiments with the Polarized Internal Gas Target (PIT) at ANKECOSY
-
September 14 2007 Ralf Engels 23
Storage cell and stochastically cooled beam
Cooling off
Cooling on
Tp= 831 MeV
September 14 2007 Ralf Engels 24
First Experimental Beam Time
Stacking rarr 120 injection with 10 s e-coolingFlat top rarr 30 min to have about 60 duty time
0 20 50Time min
September 14 2007 Ralf Engels 25
First Experimental Beam Time
Stacking rarr 120 injection with 10 s e-coolingFlat top rarr 30 min to have about 23 duty time
0 20 50Time min
Switching on the gasto feed the storage cell
Acceleration withoutgas in the storage cell
7 109 polarized deuterons in the ring with gas in the target
September 14 2007 Ralf Engels 26
Td=12 GeV target H (N2) gas
dprarrdp
dp rarr rarr
First Double Polarized Experiment dp dp rarr rarr
September 14 2007 Ralf Engels 27
First Double Polarized Experiment dp dp rarr rarr
Td=12 GeV target H (N2) gas
dprarr(dpsp) πo
quasi-free nprarrd
πo
(High amp Low branch)
High branch
Low branch
dp rarr rarr
September 14 2007 Ralf Engels 28
First Polarization Measurement of the Target
ANKE
preliminary
dp Td=12 GeV polarized H gas
quasi-free nprarrd
πo
(High amp Low branch)
ltQygt = 075 plusmn 006
θd=50-150 θd=150-220 θd=220-280 θd=280-400
θd=1550-1650 θd=1650-1700 θd=1700-1770
rarr
quasi-free
np rarr dπ0
(High and low branch)
ltQygt = 079 plusmn 007
September 14 2007 Ralf Engels 29
Summary of commissioning and first experiment
1 Cell-target thickness for H (hyperfine state 1) ~ 2 middot 1013 cm-2
3 ABS jet-target thickness ~ 15 middot 1011 cm-2
bull Tests at ANKE with ABS and storage cell
with stacking injection (Nov 2005) and stochastic cooling (Mar 2006)
2 Average luminosity for the storage-cell test ~ 1 middot 1029 cm-2 s-1
4 Hydrogen polarization in the cell ~ 079 +- 007
bull First experiment dprarrppn - JanFeb 2007rarrrarr
September 14 2007 Ralf Engels 30
Plans for the future
December 07 ndash PIT reinstallation With rotatable Wien filter and
better shielding of the LSP
JanFeb rsquo08 ndash Next beam time d prarr (pp)n at 2435 ndash 37 GeVc
(5 Weeks)
March rsquo08 ndash PIT deinstallation
ABS and LSP can be used for other experiments
- ISTC project 1860 Nuclear Polarization in H2D
2 molecules
- Direct Measurements of the Hyperfine levels
in the 2S12
2P12
state rarr Breit-Rabi diagram
rarr rarr
September 14 2007 Ralf Engels 31
Far Future Polarized Fusion
- First Experiments with the Polarized Internal Gas Target (PIT) at ANKECOSY
-
September 14 2007 Ralf Engels 24
First Experimental Beam Time
Stacking rarr 120 injection with 10 s e-coolingFlat top rarr 30 min to have about 60 duty time
0 20 50Time min
September 14 2007 Ralf Engels 25
First Experimental Beam Time
Stacking rarr 120 injection with 10 s e-coolingFlat top rarr 30 min to have about 23 duty time
0 20 50Time min
Switching on the gasto feed the storage cell
Acceleration withoutgas in the storage cell
7 109 polarized deuterons in the ring with gas in the target
September 14 2007 Ralf Engels 26
Td=12 GeV target H (N2) gas
dprarrdp
dp rarr rarr
First Double Polarized Experiment dp dp rarr rarr
September 14 2007 Ralf Engels 27
First Double Polarized Experiment dp dp rarr rarr
Td=12 GeV target H (N2) gas
dprarr(dpsp) πo
quasi-free nprarrd
πo
(High amp Low branch)
High branch
Low branch
dp rarr rarr
September 14 2007 Ralf Engels 28
First Polarization Measurement of the Target
ANKE
preliminary
dp Td=12 GeV polarized H gas
quasi-free nprarrd
πo
(High amp Low branch)
ltQygt = 075 plusmn 006
θd=50-150 θd=150-220 θd=220-280 θd=280-400
θd=1550-1650 θd=1650-1700 θd=1700-1770
rarr
quasi-free
np rarr dπ0
(High and low branch)
ltQygt = 079 plusmn 007
September 14 2007 Ralf Engels 29
Summary of commissioning and first experiment
1 Cell-target thickness for H (hyperfine state 1) ~ 2 middot 1013 cm-2
3 ABS jet-target thickness ~ 15 middot 1011 cm-2
bull Tests at ANKE with ABS and storage cell
with stacking injection (Nov 2005) and stochastic cooling (Mar 2006)
2 Average luminosity for the storage-cell test ~ 1 middot 1029 cm-2 s-1
4 Hydrogen polarization in the cell ~ 079 +- 007
bull First experiment dprarrppn - JanFeb 2007rarrrarr
September 14 2007 Ralf Engels 30
Plans for the future
December 07 ndash PIT reinstallation With rotatable Wien filter and
better shielding of the LSP
JanFeb rsquo08 ndash Next beam time d prarr (pp)n at 2435 ndash 37 GeVc
(5 Weeks)
March rsquo08 ndash PIT deinstallation
ABS and LSP can be used for other experiments
- ISTC project 1860 Nuclear Polarization in H2D
2 molecules
- Direct Measurements of the Hyperfine levels
in the 2S12
2P12
state rarr Breit-Rabi diagram
rarr rarr
September 14 2007 Ralf Engels 31
Far Future Polarized Fusion
- First Experiments with the Polarized Internal Gas Target (PIT) at ANKECOSY
-
September 14 2007 Ralf Engels 25
First Experimental Beam Time
Stacking rarr 120 injection with 10 s e-coolingFlat top rarr 30 min to have about 23 duty time
0 20 50Time min
Switching on the gasto feed the storage cell
Acceleration withoutgas in the storage cell
7 109 polarized deuterons in the ring with gas in the target
September 14 2007 Ralf Engels 26
Td=12 GeV target H (N2) gas
dprarrdp
dp rarr rarr
First Double Polarized Experiment dp dp rarr rarr
September 14 2007 Ralf Engels 27
First Double Polarized Experiment dp dp rarr rarr
Td=12 GeV target H (N2) gas
dprarr(dpsp) πo
quasi-free nprarrd
πo
(High amp Low branch)
High branch
Low branch
dp rarr rarr
September 14 2007 Ralf Engels 28
First Polarization Measurement of the Target
ANKE
preliminary
dp Td=12 GeV polarized H gas
quasi-free nprarrd
πo
(High amp Low branch)
ltQygt = 075 plusmn 006
θd=50-150 θd=150-220 θd=220-280 θd=280-400
θd=1550-1650 θd=1650-1700 θd=1700-1770
rarr
quasi-free
np rarr dπ0
(High and low branch)
ltQygt = 079 plusmn 007
September 14 2007 Ralf Engels 29
Summary of commissioning and first experiment
1 Cell-target thickness for H (hyperfine state 1) ~ 2 middot 1013 cm-2
3 ABS jet-target thickness ~ 15 middot 1011 cm-2
bull Tests at ANKE with ABS and storage cell
with stacking injection (Nov 2005) and stochastic cooling (Mar 2006)
2 Average luminosity for the storage-cell test ~ 1 middot 1029 cm-2 s-1
4 Hydrogen polarization in the cell ~ 079 +- 007
bull First experiment dprarrppn - JanFeb 2007rarrrarr
September 14 2007 Ralf Engels 30
Plans for the future
December 07 ndash PIT reinstallation With rotatable Wien filter and
better shielding of the LSP
JanFeb rsquo08 ndash Next beam time d prarr (pp)n at 2435 ndash 37 GeVc
(5 Weeks)
March rsquo08 ndash PIT deinstallation
ABS and LSP can be used for other experiments
- ISTC project 1860 Nuclear Polarization in H2D
2 molecules
- Direct Measurements of the Hyperfine levels
in the 2S12
2P12
state rarr Breit-Rabi diagram
rarr rarr
September 14 2007 Ralf Engels 31
Far Future Polarized Fusion
- First Experiments with the Polarized Internal Gas Target (PIT) at ANKECOSY
-
September 14 2007 Ralf Engels 26
Td=12 GeV target H (N2) gas
dprarrdp
dp rarr rarr
First Double Polarized Experiment dp dp rarr rarr
September 14 2007 Ralf Engels 27
First Double Polarized Experiment dp dp rarr rarr
Td=12 GeV target H (N2) gas
dprarr(dpsp) πo
quasi-free nprarrd
πo
(High amp Low branch)
High branch
Low branch
dp rarr rarr
September 14 2007 Ralf Engels 28
First Polarization Measurement of the Target
ANKE
preliminary
dp Td=12 GeV polarized H gas
quasi-free nprarrd
πo
(High amp Low branch)
ltQygt = 075 plusmn 006
θd=50-150 θd=150-220 θd=220-280 θd=280-400
θd=1550-1650 θd=1650-1700 θd=1700-1770
rarr
quasi-free
np rarr dπ0
(High and low branch)
ltQygt = 079 plusmn 007
September 14 2007 Ralf Engels 29
Summary of commissioning and first experiment
1 Cell-target thickness for H (hyperfine state 1) ~ 2 middot 1013 cm-2
3 ABS jet-target thickness ~ 15 middot 1011 cm-2
bull Tests at ANKE with ABS and storage cell
with stacking injection (Nov 2005) and stochastic cooling (Mar 2006)
2 Average luminosity for the storage-cell test ~ 1 middot 1029 cm-2 s-1
4 Hydrogen polarization in the cell ~ 079 +- 007
bull First experiment dprarrppn - JanFeb 2007rarrrarr
September 14 2007 Ralf Engels 30
Plans for the future
December 07 ndash PIT reinstallation With rotatable Wien filter and
better shielding of the LSP
JanFeb rsquo08 ndash Next beam time d prarr (pp)n at 2435 ndash 37 GeVc
(5 Weeks)
March rsquo08 ndash PIT deinstallation
ABS and LSP can be used for other experiments
- ISTC project 1860 Nuclear Polarization in H2D
2 molecules
- Direct Measurements of the Hyperfine levels
in the 2S12
2P12
state rarr Breit-Rabi diagram
rarr rarr
September 14 2007 Ralf Engels 31
Far Future Polarized Fusion
- First Experiments with the Polarized Internal Gas Target (PIT) at ANKECOSY
-
September 14 2007 Ralf Engels 27
First Double Polarized Experiment dp dp rarr rarr
Td=12 GeV target H (N2) gas
dprarr(dpsp) πo
quasi-free nprarrd
πo
(High amp Low branch)
High branch
Low branch
dp rarr rarr
September 14 2007 Ralf Engels 28
First Polarization Measurement of the Target
ANKE
preliminary
dp Td=12 GeV polarized H gas
quasi-free nprarrd
πo
(High amp Low branch)
ltQygt = 075 plusmn 006
θd=50-150 θd=150-220 θd=220-280 θd=280-400
θd=1550-1650 θd=1650-1700 θd=1700-1770
rarr
quasi-free
np rarr dπ0
(High and low branch)
ltQygt = 079 plusmn 007
September 14 2007 Ralf Engels 29
Summary of commissioning and first experiment
1 Cell-target thickness for H (hyperfine state 1) ~ 2 middot 1013 cm-2
3 ABS jet-target thickness ~ 15 middot 1011 cm-2
bull Tests at ANKE with ABS and storage cell
with stacking injection (Nov 2005) and stochastic cooling (Mar 2006)
2 Average luminosity for the storage-cell test ~ 1 middot 1029 cm-2 s-1
4 Hydrogen polarization in the cell ~ 079 +- 007
bull First experiment dprarrppn - JanFeb 2007rarrrarr
September 14 2007 Ralf Engels 30
Plans for the future
December 07 ndash PIT reinstallation With rotatable Wien filter and
better shielding of the LSP
JanFeb rsquo08 ndash Next beam time d prarr (pp)n at 2435 ndash 37 GeVc
(5 Weeks)
March rsquo08 ndash PIT deinstallation
ABS and LSP can be used for other experiments
- ISTC project 1860 Nuclear Polarization in H2D
2 molecules
- Direct Measurements of the Hyperfine levels
in the 2S12
2P12
state rarr Breit-Rabi diagram
rarr rarr
September 14 2007 Ralf Engels 31
Far Future Polarized Fusion
- First Experiments with the Polarized Internal Gas Target (PIT) at ANKECOSY
-
September 14 2007 Ralf Engels 28
First Polarization Measurement of the Target
ANKE
preliminary
dp Td=12 GeV polarized H gas
quasi-free nprarrd
πo
(High amp Low branch)
ltQygt = 075 plusmn 006
θd=50-150 θd=150-220 θd=220-280 θd=280-400
θd=1550-1650 θd=1650-1700 θd=1700-1770
rarr
quasi-free
np rarr dπ0
(High and low branch)
ltQygt = 079 plusmn 007
September 14 2007 Ralf Engels 29
Summary of commissioning and first experiment
1 Cell-target thickness for H (hyperfine state 1) ~ 2 middot 1013 cm-2
3 ABS jet-target thickness ~ 15 middot 1011 cm-2
bull Tests at ANKE with ABS and storage cell
with stacking injection (Nov 2005) and stochastic cooling (Mar 2006)
2 Average luminosity for the storage-cell test ~ 1 middot 1029 cm-2 s-1
4 Hydrogen polarization in the cell ~ 079 +- 007
bull First experiment dprarrppn - JanFeb 2007rarrrarr
September 14 2007 Ralf Engels 30
Plans for the future
December 07 ndash PIT reinstallation With rotatable Wien filter and
better shielding of the LSP
JanFeb rsquo08 ndash Next beam time d prarr (pp)n at 2435 ndash 37 GeVc
(5 Weeks)
March rsquo08 ndash PIT deinstallation
ABS and LSP can be used for other experiments
- ISTC project 1860 Nuclear Polarization in H2D
2 molecules
- Direct Measurements of the Hyperfine levels
in the 2S12
2P12
state rarr Breit-Rabi diagram
rarr rarr
September 14 2007 Ralf Engels 31
Far Future Polarized Fusion
- First Experiments with the Polarized Internal Gas Target (PIT) at ANKECOSY
-
September 14 2007 Ralf Engels 29
Summary of commissioning and first experiment
1 Cell-target thickness for H (hyperfine state 1) ~ 2 middot 1013 cm-2
3 ABS jet-target thickness ~ 15 middot 1011 cm-2
bull Tests at ANKE with ABS and storage cell
with stacking injection (Nov 2005) and stochastic cooling (Mar 2006)
2 Average luminosity for the storage-cell test ~ 1 middot 1029 cm-2 s-1
4 Hydrogen polarization in the cell ~ 079 +- 007
bull First experiment dprarrppn - JanFeb 2007rarrrarr
September 14 2007 Ralf Engels 30
Plans for the future
December 07 ndash PIT reinstallation With rotatable Wien filter and
better shielding of the LSP
JanFeb rsquo08 ndash Next beam time d prarr (pp)n at 2435 ndash 37 GeVc
(5 Weeks)
March rsquo08 ndash PIT deinstallation
ABS and LSP can be used for other experiments
- ISTC project 1860 Nuclear Polarization in H2D
2 molecules
- Direct Measurements of the Hyperfine levels
in the 2S12
2P12
state rarr Breit-Rabi diagram
rarr rarr
September 14 2007 Ralf Engels 31
Far Future Polarized Fusion
- First Experiments with the Polarized Internal Gas Target (PIT) at ANKECOSY
-
September 14 2007 Ralf Engels 30
Plans for the future
December 07 ndash PIT reinstallation With rotatable Wien filter and
better shielding of the LSP
JanFeb rsquo08 ndash Next beam time d prarr (pp)n at 2435 ndash 37 GeVc
(5 Weeks)
March rsquo08 ndash PIT deinstallation
ABS and LSP can be used for other experiments
- ISTC project 1860 Nuclear Polarization in H2D
2 molecules
- Direct Measurements of the Hyperfine levels
in the 2S12
2P12
state rarr Breit-Rabi diagram
rarr rarr
September 14 2007 Ralf Engels 31
Far Future Polarized Fusion
- First Experiments with the Polarized Internal Gas Target (PIT) at ANKECOSY
-
September 14 2007 Ralf Engels 31
Far Future Polarized Fusion
- First Experiments with the Polarized Internal Gas Target (PIT) at ANKECOSY
-