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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
INTDS 2010 Bettina Lommel 2
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
INTDS 2010 Bettina Lommel 4
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
INTDS 2010 Bettina Lommel 5
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
INTDS 2010 Bettina Lommel 6
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
INTDS 2010 Bettina Lommel 7
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
INTDS 2010 Bettina Lommel 8
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 %
INTDS 2010 Bettina Lommel 20
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