heavy-ion fusion and fission study at jaea · heavy-ion fusion and fission study at jaea katsuhisa...
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![Page 1: Heavy-ion Fusion and Fission Study at JAEA · Heavy-ion Fusion and Fission Study at JAEA Katsuhisa Nishio Advanced Science Research Center Japan Atomic Energy Agency Tokai, JAPAN](https://reader035.vdocument.in/reader035/viewer/2022070402/5fd0beca33d245440065edc8/html5/thumbnails/1.jpg)
Heavy-ion Fusion and Fission Study at JAEA
Katsuhisa Nishio
Advanced Science Research Center
Japan Atomic Energy Agency
Tokai, JAPAN
IWM-EC, 2014, Catania, Italy
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K. Nishio, H. Ikezoe, S. Mitsuoka, I. Nishinaka, H. Makii, Y. Wakabayashi, K. Hirose, K. Tsukada, M. Asai, Y. Nagame, A. Kimura, H. Harada
S. Hofmann, D. Ackermann, F.P. Heßberger, S. Heinz, J. Khuyagbaatar, B. Kindler, V.F.Comas J.A. Heredia, I. Kojouharov, B. Lommel, R. Mann, B. Sulignano, Ch.E. Düllmann, M.Schädel
S. Antalic, S. Saro
T. Ohtsuki, K. Hagino
A.G. Popeko, A.V. Yeremin, A. Svirikhin
Y. Watanabe
A. Yakushev, A. Gorshkov, R. Graeger, A. Türler
Y. Aritomo
A. Andreyev, D. Jenkins
S. Chiba
S. Yan N. Tamura, S. Goto
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Tokai Campus, JAEA Tokyo
Tandem facility
J-PARC
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Experimental Nuclear Physics Program at JAEA
◆ Fusion-Fission Study for Heavy-element Synthesis
◆ Multi-nucleon transfer-induced Fission and Surrogate Reaction
◆ Structure study for nuclei around 100Sn using JAEA Recoil Mass
Separator
◆ Neutron TOF measurement for fission and neutron-capture study
Tandem Facility
J-PARC
Contribution to Fukushima Issues
◆ New surveillance detector for criticality of melted fuel at
Fukushima power plant.
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JAEA Tandem facility
20 MV Tandem accelerator (20UR) Super-conducting Booster Liniac ECR Ion Source on the terminal
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Magnetic Spectrometer
Booster Liniac Recoil Mass Separator
Ge-detector array
ISOL ( p + 238U)
Radioactive target materials can be used Th, U, Np, Pu, Np, Am, Cm, Cf
Scattering Chamber
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Fusion-Fission Study for Heavy Element
Synthesis
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Super-heavy Nuclei
中性子数 N
DbSg
BhHs
Mt
Rg
118
陽子数 Z
Ds
Cn113
150 155 160 165 170 175 180 185
100
105
110
115
120
184
162
108
114
Cold Fusion (GSI,RIKEN)
Pb, Bi Targets
α
sf
EC
β-
Deformed Shell
120 48Ca + Actinide Target Nuclei
(FLNR)
Spherical Shell
Understanding for fusion using actinide target nuclei are
important to explore SHN
Neutron Number
Pro
ton
Nu
mb
er
Heavier Element
Using Radioactive Nuclei
Missing Region
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14 92 108 108 0 34S + 238U 272Hs* 268Hs + 4 1n
Quasifission Fusion- Fission
1 atom
~ 3×1011
3.0×1011 6.6×1012
6.3×1012
(3) Evaporation (2) Fusion CN (1) Contact
Three steps for heavy-element synthesis
Fusion probability
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Actinide Pb,Bi
z
A. Iwamoto, Nucl.Phys.A, 596 (1996) 329.
Orientation effects of target nucleus
Equatorial
High energy (above barrier)
Polar
Low energy (sub-barrier)
Effects of Nuclear Deformation on Fusion
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Neutron
132Sn
238U
Pro
ton
Fusion-fission and Quasi-fission
78Ni
208Pb
274Hs (Z=108)
0
1
2
3
-150
-100
-50
0
50
-0.5
0.0
0.5
Pote
ntial E
ne
rgy 238U
Quasi-fission
36S
0
+
-
Fusion
Compund
Nucleus
Potential by Y. Aritomo
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In-Beam Fission Measurement
Multi-Wire Proportional Counter
MWPC2 MWPC1
238U
Fission Fragment 1
Fission Fragment 2
238U target
200 mm
120 mm
5 mm
30Si, 31P, 36,34S, 40Ar, 40,48Ca Beams
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Elab=179.0 MeV
100
101
102
103
Elab=173.4 MeV
100
101
102
103
Elab=167.8 MeV
100
101
102
103
Elab=162.2 MeV
100
101
102
103
Elab=156.5 MeV
100
101
102
103
Elab=150.9 MeV
100
101
102
103
Elab=145.3 MeV
100
101
102
103
Elab=140.8 MeV
fold (deg)
Eve
nts
100 110 120 130 140 150 160 170 180 190 20010
010
110
210
3
30Si + 238U
Folding Angle Distribution
Folding angle, θfold
Events
Nucleon-transfer Induced Fission Beam
FF 1 FF 2
Beam-like
θfold 238U-like
Full Momentum Transfer Fission Beam
FF 1 FF 2
θfold 268Sg
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Orientation effects on fragment mass distributions in 36S + 238U
K. Nishio et al., Phys. Rev. C, 77 (2008) 064607.
Quasifission One-dimensional
Model
Deformation of 238U
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Fission Fragment Mass Distributions
Low Incident Energy
High Incident Energy
238U
Fragment Mass Excitation Energy of CN
Cro
ss s
ection t
o p
roduce f
ragm
ents
(m
b)
Quasifission K. Nishio et al., Phys. Rev. C, 77, 064607 (2008).
K. Nishio et al., Phys. Rev. C, 82, 044604 (2010).
78 200 90 178
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0
1
2
3
-150
-100
-50
0
50
-0.5
0.0
0.5
Dynamical calculation of nuclear shape – Fluctuation dissipation model -
Pote
ntia
l Energ
y (M
eV
)
272Hs
Quasifission
Fusion 238U
34S
CN
Fission Two center shell model
( 3 dimension )
V. Zagreabev, J. Phys. G, 31, 825 (2005).
Y. Aritomo et al., Nucl.Phys. A753, 152 (2005).
Y. Aritomo, Phys.Rev.C, 80, 064604 (2009).
Langevin Equation
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Quasifission and Deep-quasifission
36S + 238U → 274Hs ( E*=35.5 MeV)
Charge Center Distance; Z
Mass
Asy
mm
etry
; α
Entrance Entrance
Fusion-fission Fusion-fission
Qiasifission Qiasifission
Deep quasifission Deep quasifission
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Shape evolution (polar collision)
0 – 5 5 –10 10 –30 30 –50 > 50 Time (×10-21 s )
30Si + 238U
36S + 238U
CN
CN
Y. Aritomo et al., Phys. Rev. C 85, 044614 (2012).
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Fusion probability
30Si + 238U 34S + 238U
Mass Mass
Cro
ss s
ectio
n (
mb
/2u
)
c.m. Energy (MeV)
29 %
33 %
37 %
41 %
46 % 15 %
11 %
7.5 %
4.9 %
3.6 %
Fusion Probability
All Fission Fragments
Fusion-Fission
Experimental Data
Histogram
Filled Area 264Sg
263Sg
268Hs
267Hs
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Timing detector
Silicon strip detector
238U Targets
34S beams (2.0 – 2.5 pμA) in 2009
SHIP S. Hofmann and G.Münzenberg,
Rev. Mod. Phys. 72, 733 (2000).
Measurement of evaporation residue (ER)
cross sections at GSI
30Si + 238U = 268Sg*
30Si beams (1.0 pμA) in 2006
34S + 238U = 272Hs*
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Hs isotopes produced in 34S + 238U
Ec.m.= 152 MeV
E* = 40 MeV
0.54 pb +1.3 - 0.45
1.8 pb +4.2 - 1.5
Ec.m. = 163 MeV
E* = 51 MeV
Yu.A Lazarev et al., 267Hs ( 2.5 pb ),
PRL75(1995) 1903.
New Isotope
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Fusion and ER cross sections
34S + 238U 30Si + 238U
Fusion Cross
Section
×Fusion
Probability
×Survival
Probability
Cross sections for
SHN
(Statistical Model )
Qasifission Quasifission
Capture Cross
Section E Excitation energy Excitation energy
F
issio
n
Cro
ss s
ectio
n (
mb)
Fis
sio
n
cro
ss s
ection (
mb)
Eva
po
ratio
n R
esid
ue
C
ross s
ection (
mb)
Eva
po
ratio
n R
esid
ue
C
ross s
ectio
n (
mb
)
Energy in c.m. (MeV) Energy in c.m. (MeV)
K. Nishio et al., PRC 82, 044604 (2010).
K. Nishio et al., PRC 82, 024611 (2010).
1.8 pb 67 pb 0.54 pb 10 pb
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283,282Cn
Ec.m. (MeV)
Pfu
s
48Ca+238U40Ca+238U
180 200 220 240
10-2
10-1
100
48Ca+238U (MeV)E*
20 30 40 50 60 70 80 90
40Ca+238U40 50 60 70 80 90 100 110
Fusi
on
Pro
bab
ility
Ec.m.
Fusion Probabilities for 48Ca + 238U and 40Ca + 238U
K. Nishio et al., Phys. Rev. C 86, 034608 (2012).
Fragment Mass (u)
Yie
ld (
%)
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48Ca + 238U
S. Hofmann et al., Eur.Phys.J. A 32, 251 (2007).
Yu.Ts. Oganessian et al., Phys.Rev.C 70, 064609 (2004)
Yu.Ts. Oganessian, J.Phys.G 34, R165 (2007).
Capture cross section
Fusion Cross section
282,283Cn cross sections from
Cro
ss S
ection (m
b)
Ec.m. (MeV)
3n2n
4n
E* (MeV)
3n : FLNR4n : FLNR3n : GSI
CaptureFusion
48Ca +238U
170 180 190 200 21010-11
10-10
10-9
10-8
10-7
10-6
10-5
10-4
10-3
10-2
10-1
100
101
102
103 20 30 40 50
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Summary
In beam fission experiment can be used to estimate the fusion
probability for heavy-element synthesis.
Model calculation in heavy-ion induced fission was shown.
Sub-barrier fusion reaction can be used for heavy-element
synthesis.
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Heavy-Ion Program at J-PARC
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J-PARC HI
JPARC HI
Heavy Ion LINAC (35m)
-13 MeV/u, 238U 238U 10-15 GeV/u
Proton 400 MeV 50 GeV
3 GeV
hadron
n, μ
ν
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28
Heavy-Ion Acceleration at J-PARC
28
J-PARC
SPS
ALICE/PHENIX
STAR, energy scan
NICA
FAIR
QCD Phase diagram -search for critical point and
phase boundary-
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New LINAC
RCS
MR
Ion Source
RFQ
• 108MHz
• Einj ~ 50keV
n×IH-DTL
• 108MHz
• 2~3m
• n~7
Short Cavities
• 324MHz
• Energy
tunable
RCS
Multi-turn injection
MR
197Au32+ 197Au79+
12.8MeV/u 188MeV/u 11.5GeV/u
- Laser Ion
Source
- EBIS
- SC-ECR
Full strip Linac
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Three Extreme Region on Chart of Nuclei Z
N
N=Z
50
100
50
100 150 200 28
50 82
126
20 28
50
82
150
184
120 114
N=126
SHE
Search for Heaviest N=Z Nuclei
Search for Super-heavy Nuclei
Search for Heaviest N=126 Nuclei
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Protons
Neu
trons
238U + 248Cm ( 6MeV/u )
238U
248Cm
Search for Super-Heavy Nuclei
by V. Zagrebaev (FLNR)