Wei-ping Liu 柳卫平 [email protected] China Institute of Atomic Energy, CIAE ...
description
Transcript of Wei-ping Liu 柳卫平 [email protected] China Institute of Atomic Energy, CIAE ...
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Nuclear astrophysical reactions by unstable beams andProgress of BRIF and BRIFIIWei-ping Liu [email protected] China Institute of Atomic Energy, CIAE 6th China Japan Joint Nuclear Physics Symposium May 16-20, 2006Shanghai
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Study of some key nuclear astrophysical reactions by unstable nuclear beams
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Interplay between astrophysics and nuclear physicsNuclear processMain energy of star to balance gravitational collapseMechanism of isotope synthesis apart from HydrogenRule the evolution process from the first few minutes after big bang to just before the end of star lifeNuclear astrophysicsUsing nuclear physics to explain the energy production and element synthesis in star and cosmos
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Nuclear astrophysics and physics of unstable nucleiprimordial and super novae high temperature and density environment, large amount of unstable nuclear involved into nuclear burningRIKEN RIBF proposal
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Nuclear astrophysics LabB. Pfeiffer, et al., Z. Physik A357, 253 (1997)
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Reaction networkCross sectionDecay half-life
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Challenge to experiment11C(p,)12NGamow windowExtremely low energyVanishing low cross section
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Our solution: indirect methodRIB productionW.P. Liu, NIM B204(2003)62(d,n) or (d,p) measurementANC or Spec factorAstrophysical reaction ratesW.P. Liu, PRL77(1996)611
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Direct capture process of 11C(p,g)Key reaction in hot pp chainDominated by direct captureN. C. Shu,, W. P. Liu et al., Nucl. Phys. A 758 (2005) 419cW. P. Liu et al., NPA728(2003)275
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First measurement of primordial 8Li(n,g)9Li reaction rateDestroy reaction of 8Li: 8Li(n,g)9Li, 8Li(d,p)9Li in inhomogeneous big bangAPJ429(1994)499Half-life of 8Li: 0.83 sdirect (n,g) exp. impossibleZ. H. Li, W.P. Liu et al.PRC 71, 052801(R) (2005)
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Comment on our resultsThe paper presents excellent experimental work and removes a longstanding debate about the absolute cross section of 8Li(n,g) As far as I know, so far, no results have been published to determine a neutron capture rate of astrophysical importance
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13N(d,n)14O 13N(p,g)14OPRC, submitted
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Summary of reaction studied9C12N18Ne17F14O
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Opportunities from BRIF and BRIF IIBRIF: Beijing Radioactive Ion Facility
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Physics : why BRIFIntensity 1-109, energy 100 keV-10 MeV/u, RIA proposal
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The current Tandem labBeam type, only stable, no noble gasEnergy range, less than 14 MeV/qInstrumentation, no RMS, no ISOLBeam time: 100 % overdue
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BRIF100 MeV 200 mA compact proton cyclotron20000 mass resolution ISOL, 2 MeV/q super-conducting LINAC
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BRIF energy and mass resolution
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BRIF research opportunities and combinations100 MeV, 200 mAProton CyclotronISOLMass Resolution20000RIBStable BeamIon SourceSuperConductingLINACTandemAccelerator15 MVNeutron dataRadiation physicsDecay dataMaterial physicsNuclear dataRadiation physicsNuclear structureReactionAstrophysicsAtomic PhysicsApplicationsRadiation physicsNuclear structureReactionAstrophysicsAtomic PhysicsTandem with unstable beam, proton-rich, fissionheavy ion beam with higher beam energy, 20 MeV/q100 MeV proton and neutron beamsavailable by the year 2010100 MeV neutronISOLcurrent terminalslimitation of instrument and machine time
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More n-rich beam: CARRISOLHorizontal tubeHe-jet + ISOLNeutron flux 1X1014 /cm2/sAvailable in 2007
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Low b RFQ for new injector17 MeV/q super-conducting LINACRMSLarge acceptance spectrometerDecay measurements
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Beam energy
Chart1
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8.6666666667101118.54.8
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13 MV
15 MV
(MeV/u)
200011
1315
H111261304.83030
D2113
He2423924519.211.2522.5
Li3735236033.68.571428571420
Be4946547543.28.333333333318.75
B51146547552.86.818181818218.75
C61257859057.67.518
N714578610567.27.517.5
O816691610576.86.562517.5
F919691712091.26.315789473717.1428571429
Mg122413115.2
Al132713129.6
Si142881179150134.45.357142857116.6666666667
P153113148.8
S163213153.6
Cl173513168
Ca20409130101651924.12516.5
Fe265613268.8
Ni285913283.2
Cu296413307.2
Se347913379.2
Br358013384
Ag4710813518.4
Sn5011913571.2
I5312713609.6
26304.8
13
394519.2
526033.6
657543.2
657552.8
789057.6
7810567.2
9110576.8
9112091.2
13115.2
13129.6
117150134.4
13148.8
13153.6
13168
130165192
MeV
brnbf energy.nb,
3.5 MV 3.5 MV 3.5 MV 13 MV 13 MV 13 MV 13 MV 15 MV 15 MV 15 MV 15 MV 15 MV 15 MV
11177.00012626.00113030.000132321
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16668624.50.148111560.9433111801.084352501.5060239
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brnbf energy.nb, 17 MeV
3.5 MV 3.5 MV 3.5 MV 13 MV 13 MV 13 MV 13 MV 15 MV 15 MV 15 MV 15 MV 15 MV 15 MV
1117.0007126.0026.00113030.0001.0001014.9447471
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115314.0001.2727272727465.005.9154756.8185.000109.46116014.54555
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13 MV 15 MV
1263032474.8
68.6666666667101118.54.8
115.90909090916.81818181827.7272714.54554.8
165.68756.56257.562515.06254.8
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2010.7761194030.89552238811.253733.94034.8
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black and white version
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13 MV
15 MV
(MeV/u)
7263032
1.758.66666666671011
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0.24257425741.41584158421.78217821782.35644
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0.12827225130.81675392670.9424083771.31937
0.1250.79591836730.91836734691.28571
0.12189054730.7761194030.89552238811.25373
0.11893203880.75728155340.87378640781.23301
0.11611374410.73933649290.85308056871.20379
0.11342592590.72222222220.83333333331.17593
0.11085972850.70588235290.8144796381.15837
0.10840707960.69026548670.7964601771.13274
0.10606060610.67532467530.77922077921.10823
0.10381355930.66101694920.76271186441.08475
0.1016597510.64730290460.74688796681.06224
0.09959349590.63414634150.73170731711.04878
0.09760956180.62151394420.71713147411.02789
3.5 MV
13 MV
15 MV
MeV/u
7263032
10.5526066
14657585
17.591105121
21104120138
21104135157
21117150176
21130150180
21130150184
21130165201
21130165205
21143165207
21143165209
24.5143180228
24.5143180230
24.5143180232
24.5143180232
24.5143180234
24.5143180236
24.5143180236
24.5143180238
24.5156180240
24.5143180240
24.5143180240
24.5156180242
24.5156180244
24.5156180246
24.5156180246
24.5156180248
24.5156180248
24.5156180248
24.5156180248
24.5156180250
24.5156180250
24.5156180250
24.5156180250
24.5156180252
24.5156180252
24.5156180252
24.5156180252
24.5156180252
24.5156180254
24.5156180254
24.5156180254
24.5156180256
24.5156180256
24.5156180256
24.5156180256
24.5156180256
24.5156180258
24.5156180258
3.5 MV
13 MV
15 MV
15 MV
MeV
BRNBE.XLS
11111
23333
34455
46688
577910
5781112
5891315
5991517
5991719
59101821
59102023
510102125
510102227
610112430
610112532
610112634
610112636
610112738
610112840
610112842
610112944
611113046
610113047
610113049
611113151
611113253
611113355
611113357
611113459
611113461
611113462
611113464
611113566
611113568
611113570
611113571
611113673
611113675
611113677
611113678
611113680
611113782
611113783
611113785
611113887
611113888
611113890
611113892
611113893
611113995
611113997
3.5 MV
13 MV
15 MV
15 MV
BRNBELP.XLC
BEVELACISLBRNBF
10301010629174
1003022010924.4444444444220
100500JHP1422.2857142857312
10500106.51722.0588235294375
10301206.52817.8928571429501
K1200, LISE, RIPSISAC3515.7714285714552
101071.54713.4468085106632
10010601.55511.8649
100100LLN1006.5
10100130.651205.8
1010OREB1505
SIS1013
105805
23851603
2385002202.25HI-13
10500EB8812672
1051013194.421052631684
COULOMB BARRIER401.5283.8571428571108
54.8800.36353.4285714286120
2104.81500.1582.4827586207144
CSR1081.4444444444156
1051331.1729323308156
15052000.78156
150300
10300
105
&F
Page &P
BRNBELP.XLC
0000000000000
000000000000
00000000
00000000
000000
00
00
00
00
0
0
&F
Page &P
BEVALAC
SIS
K1200, LISE, RIPS
CSR
EB88
LLN
ISAC
HI-13
OREB
BRNBF
ISL
COULOMB
BARRIER
JHP
A (amu)
E/A (MeV/amu)
BRNBE.XLC
000
000
00
00
00
00
00
00
00
0
0
HI-13
BRNBF
COULOMB
BARRIER
A (amu)
E/A (MeV/amu)
Beam Energy vs. Mass
BRNBELL.XLC
4.8106.51.50.651313296
4.8106.51.551.524.44444444444.4210526316
30.3622.28571428573.8571428571
2.250.122.05882352943.4285714286
17.89285714292.4827586207
15.77142857141.4444444444
13.44680851061.1729323308
11.80.78
6.5
5.8
5
&F
Page &P
EB88
LLN
ISAC
HI-13
OREB
BRNBF
ISL
COULOMB BARRIER
JHP
A (amu)
E/A (MeV/amu)
30104.8106.51.50.6513130HI-1355
30104.8106.51.551.514.5655
50010030.36134.4210526316300500
5001002.250.111.53.8571428571300500
301010.73.428571428655
8.62.4827586207
8.11.4444444444
6.91.1729323308
5.80.78
5.5
4.9
&F
Page &P
BEVALAC
SIS
K1200, LISE, RIPS
CSR
EB88
LLN
ISAC
HI-13
OREB
BRNBF
ISL
COULOMB BARRIER
JHP
A (amu)
E/A (MeV/amu)
4.8106.51.50.6513130HI-13
4.8106.51.551.514.56
30.36134.4210526316
2.250.111.53.8571428571
10.73.4285714286
8.62.4827586207
8.11.4444444444
6.91.1729323308
5.80.78
5.5
4.9
EB88
LLN
ISAC
HI-13
OREB
BRNBF
ISL
COULOMB BARRIER
JHP
A (amu)
E/A (MeV/amu)
-
RFQ/DTLLow energy normal temp RFQ+ finger type DTL, multi charge heavy ion beam up to the energy accepted by SC LINAC36MHz
-
SC LINACEnergy gain 17 MeV/q36 wave length QWR9 100 L LHe tankQWRLHe tank
-
Large acceptancespectrometerLarge D Q + detectorsMass range 100-200energy 5-10 MeV/uSolid angle 80 mSrP acceptance 10Mass resolution 300 via TOF and tracking
-
RMS
Mass resolution 400solid angle 16 mSr, horizontal and vertical angular width 3.6 degreeacceptation angle 0-10 degreeMain parameters
Name
Magnets
Deflector
Radius, meter
1
5
Bending angle, degree
40
20
Gap, cm
12
12.5
Maximum Field
1.0 Tm
25 MV
-
Gamma array10X BGO+seg. HPGe Eff. 10 % @ 1 MeVresolution 6 keV
-
Research opportunitiesSystematic study of shell evolutionNuclear astrophysicsMechanism of SHE Properties of medium mass neutron rich nucleiNew decay modesGamma array
Recoil mass separator
Large acceptance spectrometer
Decay setup
-
ConclusionBRIF and BRIFII will open up exciting research opportunitiesWith BRIFII: new experimental terminalshigher beam energy of 35 MeV/q100 % more beam time by separate operationLimit: overall instrumentation usageAvailable by the year of 2013Chances are still open, and we welcome contributions, suggestions and new proposalsWe would like to collaborate with major domestic and foreign research groups and world labs to take their full research potential and to do cooperative jobsCall for user communities to build machine and detector and physics task force with more flexible wayA nice play ground in Beijing to connect locations