direct measurement of the 4 he( 12 c, 16 o) g cross section near stellar energy
DESCRIPTION
Direct measurement of the 4 He( 12 C, 16 O) g cross section near stellar energy. Kunihiro FUJITA K. Sagara , T. Teranishi , T. Goto , R. Iwabuchi , S. Matsuda, K. Nakano, N. Oba, M. Taniguchi and H. Yamaguchi Department of Physics, Kyushu University, Japan - PowerPoint PPT PresentationTRANSCRIPT
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Direct measurement of the 4He(12C,16O)g cross section near
stellar energyKunihiro FUJITA
K. Sagara, T. Teranishi, T. Goto, R. Iwabuchi, S. Matsuda, K. Nakano, N. Oba, M. Taniguchi and H. Yamaguchi
Department of Physics, Kyushu University, JapanKyushu University Tandem Laboratory (KUTL)
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Introduction• 12C/ 16O ratio: after helium burning process
– affects evolution of heavy stars – supernova or white dwarf– abundance of element of universe
• Cross Section of 4He(12C,16O)g – very small (~10-8 nb) – coulomb barrier – varies drastically around stellar energy(0.3MeV)
• Extrapolation with experimental dataEcm (MeV) s (nbarn)2.4 601.5 1
1.15 0.11.0 3x10-2
0.85 10-2
0.7 10-3
0.3 10-8
our experiment( 10% accuracy)
extrapolation
stellar energy
E1
E2
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16O measurement① 4He beam + g measurement② 16N decay measurement③ direct 16O measurement with 12C beam and 4He target
– high efficiency (~ 40%: charge fraction)– total S-factor can be obtained
• necessary components for Ecm=0.7MeV experiment– background separation system: NBG/N12C ratio of 10-19
– thick gas target : ~25 Torr x 3 cm– high intensity beam: ~ 10 pmA
• Y(16O) ~ 5 counts/day→ 1 month experiment for 10% error
Cross section (S=const.)
10-5
10-5
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Experimental Setup• Layout of Kyushu University Tandem Laboratory (KUTL)
Detector (Si-SSD)
Sputterion source
12C beam
Tandem Accelerator
Final focal plane(mass separation)
Blow in windowless4He gas target
Long-time chopper
chopperbuncher
16O
12C
Recoil Mass Separator(RMS)
Ecm = 2.4~0.7 MeVE(12C)=9.6~2.8 MeVE(16O)=7.2~2.1 MeV
Tandem
RMS
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RMS
TMP3
TMP4MBP2TMP2TMP5
MBP1
beam
TMP1
DP
1500 l/s
3000 l/s330 l/s
330 l/s520 l/s 520 l/s
520 l/s
350 l/s
Windowless Gas Target
Differential pumping system (side view)
• center pressure: 24 Torr - post stripper is not necessary• effective length: 3.98 ± 0.12 cm (measured by p+a elastic scattering)
→ target thickness is sufficient for our experiment (limited by energy loss of 12C beam)
24Torr
SSD: beam monitor4.5cm
• Blow-In Gas Target (BIGT)– windowless & high confinement capability
beam
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BG Reduction and 16O Detection
movable slits
v dispersionm dispersion
Recoil Mass Separator– 12C/16O separation : ratio of 10-11
– angular acceptance: ±1.9deg 100% 16O can be observed
• Background 12C– charge exchange– multiple scattering p/q value is nearly equal to 16O
• Background reduction① RF deflector (Long-Time Chopper)
– background reduction ~10-3 ② movable slits
– combination with trajectory analysis
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Trajectory Analysis• 12C backgrounds were rejected by slit
control based on trajectory analysis16O3+ 4.5MeV (Ecm=1.5MeV)
12C3+ 6.0MeV
12C2+ 3.0MeVslits
target
ED D1 D2final focal plane(detector)
v dispersion
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Ecm=2.4MeV experiment• beam: 12C2+, frequency: 6.063MHz
– energy: 9.6MeV , intensity: ~35pnA• target: 4He gas ~ 23.9 Torr x 3.98 cm• observable: 16O5+ 7.2 ± 0.3 MeV
– abundance = 36.9 ± 2.1 % = efficiency
29hours data
941 counts
16O
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Ecm=1.5 MeV experiment• beam: 12C1+, frequency: 3.620MHz
– energy: 6.0MeV, intensity: ~150pnA
• target: 4He gas ~ 15.0 Torr x 3.98 cm• observable: 16O3+, 4.5 ± 0.3 MeV– abundance = 40.9 ± 2.1 % = efficiency
• B.G. were generated from hitting walls of magnet
15 hours data
16O
16O 29 counts
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Cross Section and S-factor
• 2.4MeV–
• 1.5MeV– – need much more statistics– background reduction is not sufficient
bkeV 3.889.0S(2.4) nb, 2.764.6 s
future plan D. Schurmann et al.Eur. Phys. J. A 26, 301-305 (2005)
Our data (2009, 2010)
bkeV 30~S(1.5) nb, 1.0 ~ s
, 2010
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Summary
• Direct 16O measurement via 4He(12C, 16O)g reaction was proposed to determine 12C/16O abundance ratio in stars
• Blow-in type windowless gas target was developed, and thickness of 24 Torr x 3.98 cm was achieved
• Background reduction was performed by using RMS, RF-deflector and movable slits
• Ecm= 2.4 MeV experiment– s= 64.6 nb, S-factor = 89.0 keV b
• Ecm= 1.5 MeV experiment– s~ 1.0 nb, S-factor ~ 30 keV b– need much more statistics, and background reduction
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BACKUP
12
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Charge State Fraction of 16O
0
10
20
30
40
50
60
70
2 4 6 8 10 12 14
Frac
tion
[%]
Energy [MeV]
5+4+3+ 6+2+
7+
Our dataW. Liu et al. / Nucl. Instr. and Meth. A 496 (2003) 198–214
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12C beam• TOF information is needed for background rejection• pulsed beam: buncher, chopper
TOF [ch]
width: 5.43nsefficiency: 33.7 %
12C -
sin wavefrequency: 3.5-6.0MHzvoltage: 2.8kVpp
accel accel
decel decel
slitsin wavefrequency: 3.5-6.0MHzvoltage: 3.0kVpp
Chopper
Buncher
12C beam
12C foil
Si-SSD
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Normal operation of tandem accelerator.
Accel-decel operation of tandem accelerator.
At low acceleration voltage, focusing becomes weak, and beam transmission decreases.
By alternative focus-defocus, Focusing becomes strong, and Beam transmission increases.
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By the accel-decel operation, ・ 10 times higher beam transmission is obtained by strong focusing. ・ 17.5 times more intense beam can be injected, due to higher electric power
necessary for accel-decel operation.By a large aperture (12f) gas stripper, spread in beam energy and angle is
decreased, and beam transport to the target is ~3 times increased.
Totally, beam intensity is 300-500 times increased.
normal operation
accel-deceloperation
Al shorting bars for accel-decel operation
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pass only reaction products (16O) which are spread in time.
f2=3×f1
V2=V1/9f1=6.1MHzV1=±24.7kV
V3=23.7kV
reject BG
pass reaction products
+
Flat-bottom voltage
RF-Deflector (Long Time Chopper)