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Preparation of Self Preparation of Self - - supporting Nickel Targets supporting Nickel Targets for for 58 58 Ni, Ni, 60 60 Ni and Ni and 61 61 Ni Ni Bettina Lommel, Willi Hartmann, Annett Huebner, Birgit Kindler and Jutta Steiner

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Preparation of SelfPreparation of Self--supporting Nickel Targets supporting Nickel Targets for for 5858Ni, Ni, 6060Ni and Ni and 6161NiNi

Bettina Lommel, Willi Hartmann, Annett Huebner, Birgit Kindler and Jutta Steiner

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Table of ContentsTable of Contents

• Introduction• Motivation• Self-supporting Nickel• Backing• Electron-beam Evaporation

• 58Ni• 60Ni

• Extracted Ion-beam Evaporation• 61Ni

• Dissolving the Backing• Results

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Targetlaboratory @ GSITargetlaboratory @ GSI

At the Targetlaboratory at GSI we• prepare out of solid materials

– targets– stripper foils– TOF foils– degrader

• prepare for – people from GSI for an experiment at GSI– people from outside for an experiment at GSI– people from GSI for an outside experiment

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Targetlaboratory @ GSITargetlaboratory @ GSI

• provide enriched material for the ion sources• convert material

– from oxide in compound for easier evaporation– from metal in compound for longer lifetime in the beam– from oxide in metal for application in the ion source– .– .– .

• contact person for questions concerning materials• analytics

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Targetlaboratory @ GSITargetlaboratory @ GSI

We produce targets over a wide thickness range• 10 nm -- ~ µm by

– resistive heating– thermal evaporation– e-beam gun evaporation– DC magnetron sputtering– HF magnetron sputtering– extracted ion beam sputtering

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Targetlaboratory @ GSITargetlaboratory @ GSI

• 0.5 µm -- ~ 1 mm– by cold rolling– between stainless steel sheets– from foil or molten down bead– in air– in argon glove box

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Targetlaboratory @ GSITargetlaboratory @ GSI

• 1 mm – several cm– by parallel cutting– by lapping– by polishing

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MotivationMotivation

• investigation of the distribution of the fusion-barrier height by heavy-ion collisions

• first measurements with 20Ne on 90Zr and 92Zr [1] indicate certain fusion barrier height structure which can be attributed to energy level density

• interesting for self-supporting targets• interesting for Ni, choosing the double magic nuclei 58Ni and

other isotopes

• well known thickness• well known homogeneity • increases the accuracy of the measurement

[1] E.Piasecki et al., Phys. Rev. C80 (2009)

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SelfSelf--supporting Nickelsupporting Nickel

• request for self-supporting nickel from a collaboration between the ‘Nuclear Reaction’ group at GSI and the University of Warsaw

• request for 58Ni, 60Ni and 61Ni• thickness 80 µg/cm² - 100 µg/cm² wanted• opening of the target frame ø = 15 mm

• starting material:– 58Ni enriched 99.92 % bought from Chemotrade

• natural abundance: 68.08 %– 60Ni enriched 99.79 % bought from ornl

• natural abundance: 26.22 %– 61Ni enriched 92.92 % bought from ornl

• natural abundance: 1.14 %

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BackingBacking

• copper foil• 8 µm - 10 µm from Goodfellow®

• purity 99.9 %• annealed between copper electrodes• ~ 500 °C – 600 °C• cleaning of the surface• stress reduction• softening

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5858NiNi

• coating system Balzers BA510®

• electron-beam gun Leyboldt KA6®

– max. acceleration voltage: 12 kV– max. power: 6 kW

• online thickness measurement by quartz gauge• water-cooled copper crucible• distance crucible – backing: 150 mm• starting material > 150 mg• ~ 100 µg/cm² 90 sec• size of the backing 100 mm x 100 mm • target thickness ± 10 µg/cm²• yield ~ 15 %

[2] Judith C. Gursky and John A O’Rourke, Nuclear Instruments and Methods, 53, (1967), 357-358

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6060NiNi

• box coater Edwards AUTO 306®

• electron beam gun EB3– max. acceleration voltage: 5 kV– max. power: 3 kW

• online thickness measurement by quartz gauge• water-cooled copper crucible• distance crucible – backing: 50 mm; • rotating backing• starting material > 50 mg• ~ 100 µg/cm² 180 sec• target homogeneity limited by weight measurement• weight measurement of foil + frame• thickness homogeneity < 5 %• yield ~ 45 %

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6161NiNi

• extracted ion-beam sputtering with Gatan Precision Etching Coating System Model 682®

• sputter voltage 6 keV• online thickness measurement by quartz gauge• rate 0,4 Å / sec.• 61Nickel foil on sputter target holder• distance sputter target – backing: 40 mm• rotating backing• ~ 100 µg/cm² 3000 sec• target homogeneity limited by weight measurement• weight measurement of foil + frame• thickness homogeneity < 5 %• yield ~ 10 %

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Dissolving the BackingDissolving the Backing

• dissolving the copper foil• in ammoniacal trichloroacetic acid• no gas formation!

Cu + 4NH4OH + 2CCl3COOH [Cu(NH3)4 · 2H2O](CCl3COO)2+4H2O

• 10 – 15 % trichloroacetic acid• adding of ammoniac until pH-value of 12• copper precipitates• solution gets ink blue

O2

copper ammoniac trichloroacetic acid copper tetraamine chloridic acetate

[3] G. T. J. Arnison, Nucl. Instr. Meth. 53 (1967)

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ResultsResults

• 58Ni: 95, 100 and 115 µg/cm²• 60Ni: 70 and 95 µg/cm²• 61Ni: 90 and 105 µg/cm²

• thickness measurement by weighing• confirmed by alpha-measurement ~ ± 5µg/cm²

• for expensive nickel isotopes the electron-beam evaporation with small distances and rotating backing is the most efficient method

• comparison of the homogeneity should come from the experiment

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AcknowledgementAcknowledgement

Photos by Gabi Otto and Karolin Back, GSI

Alpha-measurement by Agnieszka Trzcinska, Warsaw University