Inverse kinematic studies of 12C(α,γ 16O with ERNA · Inverse kinematic studies of 12C(α,γ)16O...
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Transcript of Inverse kinematic studies of 12C(α,γ 16O with ERNA · Inverse kinematic studies of 12C(α,γ)16O...
Ruhr-Universität BochumLehrstuhl für Physik mit Ionenstrahlen (EP III)
Nukleare AstrophysikProf. Dr. C. Rolfs
Inverse kinematic studies of12C(α,γ)16O with ERNA
Daniel SchürmannERNA Collaboration
The Status of 12C(α,γ)16O, the ‘Holy Grail’ of Nuclear Astrophysics, Caltech 2006/12/15
Recoil Separator ERNA:an alternative approach to measure the reaction 12C(α,γ)16O
ion sourcedynamitron
tandem accelerator
ion beam purification
Gastarget & Post-Stripper
singlet
60° magnet
∆E-Etelescope
recoilseparation
doubletanalysingmagnet
recoilfocussing
Wien filter
Wien filter Wien filter
Wien filter
magneticquadrupolemultiplets
triplet
side FC
Nrecoils detected = Nprojectiles ⋅ ntarget ⋅ σ ⋅ TERNA ⋅ pq
Requirements• angular / energy acceptance• knowledge of charge state distribution• high purity of incoming 12C beam• suppression of 12C beam
Advantages•high efficiency ~pq•measure σtot•independent of γ‘s•(mostly) background free•γ-ray coincidences possible
Recoil Separator ERNA:an alternative approach to measure the reaction 12C(α,γ)16O
ion sourcedynamitron
tandem accelerator
ion beam purification
Gastarget & Post-Stripper
singlet
60° magnet
∆E-Etelescope
recoilseparation
doubletanalysingmagnet
recoilfocussing
Wien filter
Wien filter Wien filter
Wien filter
magneticquadrupolemultiplets
triplet
side FC
Nrecoils detected = Nprojectiles ⋅ ntarget ⋅ σ ⋅ TERNA ⋅ pq
Requirements• angular / energy acceptance• knowledge of charge state distribution• high purity of incoming 12C beam• suppression of 12C beam
Advantages•high efficiency ~pq•measure σtot•independent of γ‘s•(mostly) background free•γ-ray coincidences possible
GastargetGastarget
Density Determination• Energy Loss (Stopping Power)• 7Li(α,γ)11B• 7Li(α,α´)7Li*
Position [mm]-150 -100 -50 0 50 100 150
Aus
beut
e [a
.U.]
-510
-410
-310
-210
-110Messung upstream (d=2 mm)
Messung downstream (d=2 mm)
Messung ausserhalb (d=4 mm)
Integrand
Recoil Separator ERNA:an alternative approach to measure the reaction 12C(α,γ)16O
ion sourcedynamitron
tandem accelerator
ion beam purification
Gastarget & Post-Stripper
singlet
60° magnet
∆E-Etelescope
recoilseparation
doubletanalysingmagnet
recoilfocussing
Wien filter
Wien filter Wien filter
Wien filter
magneticquadrupolemultiplets
triplet
side FC
Nrecoils detected = Nprojectiles ⋅ ntarget ⋅ σ ⋅ TERNA ⋅ pq
Requirements• angular / energy acceptance• knowledge of charge state distribution• high purity of incoming 12C beam• suppression of 12C beam
Advantages•high efficiency ~pq•measure σtot•independent of γ‘s•(mostly) background free•γ-ray coincidences possible
Charge State DistributionCharge State Distributionelectron losselectron loss
pressure p[mbar]0 1 2 3 4 5
prob
abili
ty
0
0.2
0.4
0.6
0.8
1
pressure p[mbar]0 1 2 3 4 5
prob
abili
ty
0
0.2
0.4
0.6
0.8
1
calculatedqrecoil = qcarbon
measured
qrecoil = qcarbon +2
12C3+ → 16O6+
Ecm=3.2 MeV
pressure [mbar]0 1 2 3 4 5
prob
abili
ty [%
]
0
10
20
30
40
50
60
70
80
90
100q=3+q=4+q=5+q=6+q=7+
16 3+ 4O 9.60 MeV in He
inte
grat
e
Solution:post-target stripper
Recoil Separator ERNA:an alternative approach to measure the reaction 12C(α,γ)16O
ion sourcedynamitron
tandem accelerator
ion beam purification
Gastarget & Post-Stripper
singlet
60° magnet
∆E-Etelescope
recoilseparation
doubletanalysingmagnet
recoilfocussing
Wien filter
Wien filter Wien filter
Wien filter
magneticquadrupolemultiplets
triplet
side FC
Nrecoils detected = Nprojectiles ⋅ ntarget ⋅ σ ⋅ TERNA ⋅ pq
Requirements• angular / energy acceptance• knowledge of charge state distribution• high purity of incoming 12C beam• suppression of 12C beam
Advantages•high efficiency ~pq•measure σtot•independent of γ‘s•(mostly) background free•γ-ray coincidences possible
AcceptanceAcceptanceMatrix calculations:COSY INFINITY
These just give STARTING values:
Tune Separator with 16O pilot beam!
Good tuning
Bad tuning
AngularAngular AcceptanceAcceptance
[mrad]ϑ-40 -30 -20 -10 0 10 20 30 40
Tran
smis
sion
0
0.2
0.4
0.6
0.8
1
Bext. Triplet changed by 0.7% !
Energy AcceptanceEnergy Acceptance
-20 -15 -10 -5 0 5 10 15 200.0
0.2
0.4
0.6
0.8
1.0
trans
mis
sion
∆E / E0 [ % ]experimental
calculated
by variation of beam energy
Recoil Separator ERNA:an alternative approach to measure the reaction 12C(α,γ)16O
ion sourcedynamitron
tandem accelerator
ion beam purification
Gastarget & Post-Stripper
singlet
60° magnet
∆E-Etelescope
recoilseparation
doubletanalysingmagnet
recoilfocussing
Wien filter
Wien filter Wien filter
Wien filter
magneticquadrupolemultiplets
triplet
side FC
Nrecoils detected = Nprojectiles ⋅ ntarget ⋅ σ ⋅ TERNA ⋅ pq
Requirements• angular / energy acceptance• knowledge of charge state distribution• high purity of incoming 12C beam• suppression of 12C beam
Advantages•high efficiency ~pq•measure σtot•independent of γ‘s•(mostly) background free•γ-ray coincidences possible
SuppressionSuppression
E [MeV]1.5 2 2.5 3 3.5 4 4.5 5
Rat
e R
910
1010
1110
R = # beam particles# leaky beam in ∆E-E
1212C(C(α,γα,γ))1616O total cross O total cross sectionsection
[MeV]cmE2 2.5 3 3.5 4 4.5 5
[nb]
σ
-110
1
10
210
310
410
-1
+2+4 +4
+2
+0
Beam purification systemWien-Filters
Purification WF: OFF On [channel]restE
500 1000 1500 2000 2500 3000 3500 4000 [channel]restE
0 500 1000 1500 2000 2500 3000 3500 4000
E [c
hann
el]
∆
0
500
1000
1500
2000
2500
3000
3500
4000
C12
O16
RT*50
PO ~ 10-12
PWF < 10-9
Background: Background: 1212C + C + 1212CC
[channel]restE0 20 40 60 80 100 120 140
E [c
hann
el]
∆
0
20
40
60
80
100
120
140
[channel]restE0 20 40 60 80 100 120 140
restE0 50 100 150 200 250
E∆
0
20
40
60
80
100
120
140
160
180
200
C (leaky beam)12
O16
restE0 50 100 150 200 250
20
40
60
80
100
120
140
160
180
200
Ne20
O16
restE0 50 100 150 200 250
1
10
210
310
pre target aperture-> Rate x50
carbonfoil
Background ?Background ?
Sources:• 16O impurities in 12C beam 105 to small
• scattering of 16O restgas 102 to small• 12C + 12C most probably !
(but: background almost constant)
Comparison ERNA <-> Calculation Kunz. et al.(Kunz R. et al., ApJ 567, 643-650 2002)
Basic resonance properties well reproducedClear need for improved (new) R-Matrix calculation
ERNA CollaborationERNA CollaborationBochumBochumA. A. DiDi LevaLevaR. KunzR. KunzD. D. RogallaRogallaC. RolfsC. RolfsF. F. SchümannSchümannD. SchürmannD. SchürmannF. F. StriederStriederH.H.--P. P. TrautvetterTrautvetter
Naples & CasertaN. De CesareL. GialanellaA. D’OnofrioG. ImbrianiC. LubrittoA. OrdineV. RocaM. RomanoF. Terrasi
Thank you!
[MeV]cmE2 2.5 3 3.5 4 4.5 5
S(E
) [k
eV-b
arn
]
10
210
310
1-
2+
4+
4+
2+
0+
12C(α,γ)16O total cross section
[MeV]cmE0.5 1 1.5 2 2.5 3
[keV
-bar
n]E1S
1
10
210
E1 calcFey (Turntable)Fey (Eurogam)Kunzouellet
[MeV]αE0.5 1 1.5 2 2.5
N
1
10
210
310
410
510
16N decay
[MeV]αE0.5 1 1.5 2 2.5
N
1
10
210
310
410
510
16N decay
[MeV]cmE0.5 1 1.5 2 2.5 3
[keV
-bar
n]E1S
1
10
210
E1 calcFey (Turntable)Fey (Eurogam)Kunzouellet
Fit to E1 groundstate data Assuncao et al.
γγ--Recoil CoincidencesRecoil CoincidencesEcm = 2.4 MeV (1-)8x BaF2
channel0 200 400 600 800 1000 1200 1400 1600 1800 2000 2200
cou
nts
1
10
102
103
104
105
E = 2.4 MeVSINGLE
coinc.γO-16
cascade
ground state transition
GastargetGastarget: pressure profile: pressure profile
7Li(α,γ)11B, Γcm=4keV
7Li(α,α’)Γcm=130keV
Independent of stopping powers!
p0/p > 20!
12C(α,γ)16O - 16O level scheme
0-
0+
0+
3-
1-
1-
2+
2+
4+
2-
6049
6130
0
6917
7117
8872
9580
9847
10367
10957
Jπ
400
Ex(keV) Γcm(keV)
27
0.6
Gamow window
2418
2685
3195
Ecm(keV)
Experiments E1 E212C+4He
Q = 7162 keV - 45- 245
16O g.s. casc.