Reaction Properties - GSI · 2016-04-20 · See his presentation from the last IRiS workshop ......

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Reaction Properties Working Group report J. Dvorak, H. Gäggeler, D. Hild, J. Kratz, G. Pollarolo, M. Schädel, G. Souliotis, and A. Türler Jan Dvorak Helmholtz Institute Mainz

Transcript of Reaction Properties - GSI · 2016-04-20 · See his presentation from the last IRiS workshop ......

Page 1: Reaction Properties - GSI · 2016-04-20 · See his presentation from the last IRiS workshop ... 10000 100000 Cross sections for 48Ca+248Cm at 209 MeV LAB - Secondary even-odd products

Reaction Properties Working Group report

J. Dvorak, H. Gäggeler, D. Hild, J. Kratz, G. Pollarolo, M. Schädel, G. Souliotis, and A. Türler

Jan DvorakHelmholtz Institute Mainz

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Outline

● Design Reactions

● Reaction channels:

–Elastic scattering–Quasi-elastic and few-nucleon transfer channels–Multi-nucleon transfer channels–Fusion

● Preparatory experiment

Page 3: Reaction Properties - GSI · 2016-04-20 · See his presentation from the last IRiS workshop ... 10000 100000 Cross sections for 48Ca+248Cm at 209 MeV LAB - Secondary even-odd products

Design Reactions

Design reactions chosen at IRiS 10 (Spring) workshop:

–Various projectiles + Actinide targets– 136Xe + 208Pb–Energy < 10 % above the Coulomb Barrier

Reaction ELAB

[MeV]

22Ne + 238U 12540Ar + 238U 22848Ca + 238U 255136Xe + 238U 799238U + 238U 1606

136Xe + 208Pb 789

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Classification of collisions

Loveland, W. D.; Morrissey, D. & Seaborg, G. T. Modern Nuclear Chemistry

Co

mpo

und

Nuc

leus

Fus

ion

Lik

e

Dee

p-I

nel

astic

Qu

asi-e

last

ic

Ela

stic

an

d C

oule

x

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Elastic scattering

Loveland, W. D.; Morrissey, D. & Seaborg, G. T. Modern Nuclear Chemistry

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Elastic scattering – differential cross section

● Up to θgr Rutherford cross section

● ECM

= 1.1VC → θ

gr = 110°

● Below that σel drops

gr=2asin V C2 ECM−V C

R. Bass, Nuclear Reactions With Heavy Elements

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Elastic scattering – differential cross section

dσdθ

Arbitrary scale

238U + 248Cm @ 750 MeV CM (~ VC) 48Ca + 248Cm @ 209 MeV CM (1.07 V

C)

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Inelastic collisions

86Kr+166Er at 8.18 MeV/u

Gobbi, Nuclear Physics A, 1981, 354, 337 - 374

dσ dE dθ

d dE d

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Inelastic collisions – angular distribution

Behavior scales with “modified Sommerfeld parameter” η'

a) Orbiting η' < 150

b) Focusing 250 < η' < 400

c) Coulomb trajectory 500< η'

'=Z 1 . Z 2 . e

2

ℏ . v BVB - relative velocity at interaction barrier

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Angular distribution for design reactions

Reaction ELAB

[MeV] η' Type

22Ne + 238U 125 200 Focusing40Ar + 238U 228 357 Focusing48Ca + 238U 255 418 Focusing136Xe + 238U 799 1071 Coulomb238U + 238U 1606 1700 Coulomb

136Xe + 208Pb 789 802 Coulomb

48Ca and 238U + 238U (248Cm) are representative reactions

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Deep inelastic collisions

Gobbi, Nuclear Physics A, 1981, 354, 337 - 374

86Kr+166Er at 8.18 MeV/u dσ dE dZ

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GRAZING

● Deep-inelastic reactions are complex

● Luckily we have GRAZING

– coupled channels calculations– G. Polarollo

http://personalpages.to.infn.it/~nanni/grazing/

● See his presentation from the last IRiS workshophttp://www-win.gsi.de/iris10/contributions/IRiS10_contribution_Pollarolo.pdf

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GRAZING calculation for 48Ca + 248Cm @ 209 MeV

● dσ/(dE.dθ) for different exit channels

● Reliable for quasi-elastic and few-nucleon transfer channels

– The strongestchannels

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Many-nucleon transfer reactions

● Two detailed theoretical calculations:

– 48Ca + 248Cm @ 209 MeV CM (1.07 VC) by

Adamian and Antonenko

– 238U + 248Cm @ 750 MeV CM (~ VC) by

V. Zagrebaev

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48Ca + 248Cm @ 209 MeV CM (1.07 VC)

● Calculated by Adamian and Antonenko

– Diffusion of dinuclear system in the charge and mass asymmetry coordinates

– Long contact times → isotropic angular distribution

– Excitation energy of the system shared between fragments by their mass

Ref e.g.: Adamian, G. G., Antonenko, N. V., Sargsyan, V. V. & Scheid, W., Phys. Rev. C, 2010, 81, 024604

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48Ca + 248Cm @ 209 MeV CM

140 145 150 155 160 165 170 1750.01

0.1

1

10

100

1000

10000

100000

Cross sections for 48Ca+248Cm at 209 MeV LAB - Secondary even-odd products

CfFmNoRfSgHs

N

Cro

ss s

eci

on

(pb

)

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48Ca + 248Cm @ 209 MeV CM

195 200 205 210 215 220 2250.1

1

10

100

1000

Cross sections 48Ca+248Cm - secondary products

271Sg259No267Db268Db264Lr

Energy in CM (MeV)

cros

s se

ctio

n (p

b)

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238U + 248Cm @ 750 MeV CM (~ VC)

● Calculation by V. Zagrebaev

– Dynamical model based on Langevin-type dynamical equations of motion

– Promising results presented at the last IRiS workshop

http://www-win.gsi.de/iris10/contributions/IRiS10_contribution_Zagrebaev.pdf

– Meanwhile new calculations

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Chart of Nuclides

Zagrebaev & Greiner, Nuclear Physics A, 2010, 834, 366

Transfer reactio

ns

Multi-nucleon transfer reactionsgive access to tens of new n-rich SHE isotopes

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What is missing in the picture?

Design Reactions – concentrate on 48Ca,238U + 248Cm

Reaction kinematics

Reaction channels:

–Elastic scattering

–Quasi-elastic and few-nucleon transfer channels – GRAZING

–Multi-nucleon transfer channels – Calculations by experts

–Fusion – especially fusion-fission● Preparatory experiments

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Fusion-fission

● Fusion-fission – reactions with lighter projectiles

● Rather simple (comparing to other channels)

● Experimental data exist

Itkis at al., Fusion-fission of Superheavy Nuclei,

J. of Nuclear and Radiochemical Sciences, 2002, 3, 57–61

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Preparatory experiments

● Angular distribution of SHE fragments

– The biggest unknown– Critical for separator simulations– Experimental data missing– A simple radiochemical experiment would help

Beam Target

Foil stack

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Thank you for your attention!Thank you for your attention!

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2 body kinematics

● http://nrv.jinr.ru/nrv/webnrv/kinematics/two_body.php

48Ca+238U → 26Ne + 260No at 255 MeV LAB 238U+238U → 216Pb + 260No at 1606 MeV LAB

ΘLAB

(260No) < 32°, 8.7 <ELAB

(260No) < 90 MeV ΘLAB

(260No) < 65°, 3.9 <ELAB

(260No) < 1594 MeV