Lecture 4

Search for Superheavy element and
Role of Fission Dynamics
 Z>92
(Heaviest Element in Nature) and upto Z=100-101
achieved by n irradiation or p, a, and d bombardment in
Cyclotron (1940-1955) (LBL)
 Z=102-106 by Light or Heavy-ion induced Fusion
-evaporation using heavy element targets (1958-1974)
Z=107-112 Heavy ion inuced fusion 208Pb,209Bi targets
(GSI)
Identified by recoil separation technique and connecting
to known daughter decay after implanting into Si strip
detectors.

Z=112-116 48Ca+Pu,Am,Cm,Cf (JINR, Dubna)
Identified
by gas filled separators
and Si strip setectors 1
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Cross-section data and extrapolated values for cold-fusion
Reactions (1n -evaporation channel)
Cross-section increases with increasing isospin
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E*~33 MeV
E*~34-38 MeV
48Ca+242Pu->287
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114+3n
48Ca+244Pu->288
114+4n
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48Ca+244Pu->289
114+3n
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Yury Ts. OganessianPure Appl. Chem., Vol. 76, No. 9,
pp. 1715–1734,
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48Ca+244Pu
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The flight time of the reaction products through SHIP is 2 ms.
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∙
Cold Fusion 208Pb and 209Bi targets bombarded by the following projectiles:
48Ca, 50Ti, 54Cr,58Fe, 62Ni, 64Ni, 70Zn, 76Ge, 82Se, and 86Kr.
∎
Hot Fusion 48Ca projectiles bombarded targets of 238U, 244Pu, 243Am,
245
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Cm, 248Cm, and 249Cf,
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BLDf gradually disappears
Spherical
Deformed
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Fission barrier calculations of Smolanzuk et al.
106Sg
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has highest barrier with half life of 3 hrs
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For Z1Z2>1000 to 1650 depending
on the value of the charge
asymmetry, Zp/ZT.
Extra push energies
Swiatecki
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No hindrance
Onset of fusion limitation
Due to Extra push energies
Effective fissility : weighted mean of mono-nuclear and binary
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Injection direction
Difference in energy
Between touching
Point and saddle point
Small due to shell structure
Of Ca and Pb
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Fusion area inside
Saddle point
All trajectories reaches fusion
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Quasi-fission is
dominant
Extra pocket in mass
Symmetric region
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Deep
Quasifission
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
Evgeni A. Cherepanov
Brazilian Journal of
Physics, vol. 34, no. 3A,
September, 2004
The curve V (Z,L = 0) (for the value of R corresponding to
the pocket) has a few local minima, which reflect the shell
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structure in the
interacting nuclei.
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Mass asymm fluctuates
around 0.5 and then
relaxes quickly and
Trajectory move to main
pocket
48Ca+208Pb
EX=50 MeV
Aritomo and Ohta
Pre-print
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Nuclear Physics A 744 (2004) 3–14
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Critical stage
For FF mass
Asymmetries
large
Turning stage
For QF neck develops
and speeds up fission
keeping mass asymm.
For deep QF mass asymm
Relaxed in sub-pocket
At TS
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48Ca+244Pu
Ex=50 MeV
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The smaller formation probability due to inhibition of fusion
by competing mechanism:DIC,QF,FF,PEF
Asymmetric channels: higher E* and unfavourable for survival
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Transition from
FF to QF
Mass distribution for
FF is asymmetric in shape
With peak around 132
QF
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Measurements at LNL,Legnaro (Italy)
470-630 MeV
80Se
+ 208Pb
288
116
372 MeV
56Fe+232Th
470-630 MeV
80Se
+ 232Th
312124
Measurement of fragment mass and kinetic energy
and neutron correlations
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Schematics of the setup for Se+Pb,Th experiment
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80Se+208Pb
80Se+232Th
470 MeV
470 MeV
DIC dominates but significant events around symmetry
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Se+Pb more asymmetric compared to Se+Th
QF is expected to be more for Se+Th
80Se+208Pb
80Se+232Th
470 MeV
103
103
470 MeV
510 MeV
550 MeV
630 MeV
Z = 50 N = 82
Z = 50 N = 82
d/dM (arb. units)
470 MeV
102
102
101
100
101
50
100
150
200
250
10-1
50
Mass (amu)
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100
150
200
250
Mass (amu)
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8000
cross sectionsXEcm (arb. units)
80
Se+208Pb (gated region)
80
Se+232Th (gated region)
Fit to Se+Pb data
Fit to Se+Th data
6000
higher extra-push energy
in the case of 80Se+232Th
4000
2000
0
0
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40
60
80
100
120
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B (MeV)
140
160
180
200
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80Se+208Pb
288116
50
40
30
tot
80Se+232Th
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50
20
40
10
30
tot
0
20
0
50
100
CN
Ex
150
200
250
10
(MeV)
0
ν sf tot =10±2 for Se+Pb
0
50
100
CN
Ex
150
200
(MeV)
12±1 for Fe+Th
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=17±2 for Se+Th
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250
on average of about 0.6 neutron per unit Z
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an increase of about 0.54 neutron per unit Z
excitation energy gained by the system in its transition from the saddle to the
scission point (the term ΔEx by Hilscher) that is known to show a strong mass
and Z dependence.
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JINR,Dubna
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41 detectors of DEMON at Dubna
T. Materna et al. Nuclear Physics A734
(2004) 184-l 87
208±20
QF
FF
A/2±30
The pre-scission neutron multiplicity distribution simulated
using backtracing procedure show two components for Ca+Pu
Whereas for Ca+Pb only one component is seen
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??
Self-consistent
Connectecd with
known species
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Change from
Hot fusion to
Cold fusion
For higher N-Z
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Survival probability
Depends on fission delay
And speed of cooling
Mainly by neutron
evaporation
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Expected intensities s-1 for neutron-rich
radioactive beams
SPIRAL
HI based
PIAFE
Reactor based
24Ne
44Ar
78Zn
84Ge
94Kr
7 x 107
5 x 107
108
2 x 108
2 x 109
Region beyond Z= 114 needs beam intensities in
excess of 1014 s-1.
With MAFF and spallation facility with 100μA proton of 1GeV
Intensities may go up by 3 to 4 orders of magnitude
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