Synthesis of superheavy elements with Z =112-120 in hot fusion reactions

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1 Synthesis of superheavy elements with Z =112-120 in hot fusion reactions Wang Nan College of Physics, SZU Collaborators: S G Zhou, J Q Li, E G Zhao, W. Scheid Huzhou Apr. 13 th 2012

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Synthesis of superheavy elements with Z =112-120 in hot fusion reactions. Wang Nan College of Physics, SZU Collaborators: S G Zhou, J Q Li, E G Zhao, W. Scheid. Huzhou Apr. 13 th 2012. Contents. Introduction Formalism - PowerPoint PPT Presentation

Transcript of Synthesis of superheavy elements with Z =112-120 in hot fusion reactions

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Synthesis of superheavy elements with Z =112-120 in hot fusion reactions

Wang Nan

College of Physics, SZU

Collaborators: S G Zhou, J Q Li, E G Zhao, W. Scheid

Huzhou

Apr. 13th 2012

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Contents

Introduction

Formalism

Results and discussions

Summary

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Periodic Table for Chemistry Elements

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• Experimental achievements: Super-heavy elements up to Z=118 have been synthesized

experimentally.

Z=107-113: cold fusion, 208Pb/209Bi based reactions by evaporating 1 or 2 neutrons (Rev.Mod.Phys.72(2000)733, Rep.Prog.Phys.61(1998)639)

Z=112-118: 48Ca induced fusion reactions, 48Ca bombarding actinide targets

by evaporating 3-5 neutrons (J.Phys.G34(2007)R165, NPA787(2007)343c)

GSI: 107-112 Dubna: 112-118 Riken: 113 IMP: 259Db, 265Bh

Question: How many nucleons can stay together in nucleus?

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Theoretical models for SHN production

Macroscopic dynamical model

S. Bjornholm and W.J. Swiatecki, NPA 391 (1982) 471

Fluctuation-dissipation model

Aritomo et al. PRC 59 (1999) 796, Shen Int. J.Mod. E 17(2008)66 , Liu & Bao Phys.Rev.C 80(2009)034601

Nucleon collectivization model (Zagrebaev et al.PRC65(2001)014607)

Dinuclear system model

Adamian et al. NPA 618(1997) 176

Li, Wang et al. EPL 64 (2003) 750, Eur. Phys. J. A 24, 223 (2005) , J. Phys. G32 (2006) 1143.

Feng et al., NPA 771 (2006) 50

Huang et al, PRC 84 (2011) 064619

Wang, Zhao, Scheid , Zhou 85,041601(R)(2012)

Other model

Wang et al 84, 061601(R) (2011)

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Evaporation residue cross section:

),(),(),()12(2

)( ........

2

.. JEWJEPJETJE

E mcsurmcCNmcJmc

mcER

Schematic picture of the formation of SHNDinuclear system (used to describe deep inelastic collisions of heavy systems): V.V. Volkov, Phys. Rep. 44(1978)93

TP

EN

CN

CF

capture

fusion

evaporation

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Capture of two colliding nuclei

J

mcmc

mcc JETJE

E ),()12(2

)( ....

2

..

dB

JJJR

BEJ

BfJET

Bmc

mc

)1()(2)(

2exp1

1)(),(

2

2

..

..

Transmission probability calculated from barrier distribution:

mm

mm

BBBB

N

BBBB

NBf

,exp1

,exp1

)(2

2

2

1

2/)(

2/)(

02

0

s

sm

BB

BBB

The value of 1 is 2-4 MeV less than the one of 2

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Formation of compound nucleus - Master equation

),()()],(),'()[(),,(

11'1'11

'1

11111tAPttAPdtAPdtW

dt

tEAdP

A

qfAAAAA

BGA

iiCN APP

0

)(

tVtHtH 0

tatattHKKK

K

0

tVtatatutVKK

KKKK

KK

KKKK

'

''

''

'

,,

Hamiltonian

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Dynamical Potential Energy Surface(Dyn-Pes)

Driving potential(Potential Energy Surface)

CNNCPES BrVrVABABV ),,(),,()()( 212121

2

120

222

20111

)(

)(

A

A

C

C

)1( /max

te

2

2,121211int 2

1),,(),,(),( i

iiNC CrVrVAE

Dynamical deformation satisfy

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Dynamical Potential Energy Surface(Dyn-Pes)

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Survival probability of excited compound nucleus

iifin

inx

iCNCNsur JEJE

JEJxEPJxEW

),(),(

),(),,(),,(

**

***

The thermal compound nucleus will decay by evaporating -ray, light particles and fission. The survival probabilities can be written as

2222

42

21

1

3

4)(

GG

GE

EA

NZ

c

e

mcf

a

EBE

rotn

rot

dJEBEJE

RmsJE

1

02

2*

,),(

)12(),(

Vfor

VforVRinv

0

/1)(

2

6.1/ RKZZZV

f

rotf aEBE

rotf

rotff

ff EBE

dJEBE

JEJE

1

0 /2exp1

,

),(2

1),(

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Exp. Yu.Ts. Oganessian, et al., PRC 70 (2004) 064609

Capture and evaporation residue cross sections for Ca48+U238

Results and discussions

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Exp. Yu.Ts. Oganessian et al., PRC 70 (2004) 064609

Evaporation residue cross sections for Ca48+U238, Np237

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Exp. Yu.Ts. Oganessian et al., PRC 70 (2004) 064609

Evaporation residue cross sections for Ca48+Pu242, Pu244

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Exp. Yu.Ts. Oganessian et al., PRC 74.044602

Evaporation residue cross sections for Ca48+Am243, Cm248

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Exp. Yu.Ts. Oganessian et al., PRC 74.044602

Evaporation residue cross sections for Ca48+ Bk249, Cf249

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Exp. Yu.Ts. Oganessian et al., PRC 74.044602

Evaporation residue cross sections for Ca48+U-Cf

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About element Z=120

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Fusion probability for nuclei Z=120

Evp. cross sections for nuclei Z=120

Dash dot: Ti+Cf249 Solid: Cr+Cm248Dashed: Fe+Pu244

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Lifetime for some Cf isotopes

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About element Z=119

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Evp. Cross sections for Cr+ Am and Fe+Np reactions leading to nuclei with Z=119

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Lifetime for some Bk isotopes

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Evp. Cross sections for some Ti+ Bk isotope reactions

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Summary

Some evaporation residue cross sections for 112-118 are studied with dyn-pes DNS model . The calculated results are in good agreements with experimental

Several combinations for Z=119, 120 are calculated . Some reactions are suggested.

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