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Collins SM, Köster U, Robinson AP, Ivanov P, Cocolios TE, Russell B, Fenwick AJ, Bernerd C, Stegemann S, Johnston K, Gerami AM, Chrysalidis K, Mohamud H, Ramirez N, Bhaisare A, Mewburn-Crook J, Cullen DM, Pietras B, Pells S, Dockx K, Stucki N, Regan PH. Determination of the Terbium-152 half-life from mass-separated samples from CERN-ISOLDE and assessment of the radionuclide purity. Appl Radiat Isot 2023; 202:111044. [PMID: 37797447 DOI: 10.1016/j.apradiso.2023.111044] [Citation(s) in RCA: 2] [Impact Index Per Article: 2.0] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 07/28/2023] [Revised: 09/15/2023] [Accepted: 09/22/2023] [Indexed: 10/07/2023]
Abstract
Terbium-152 is one of four terbium radioisotopes that together form a potential theranostic toolbox for the personalised treatment of tumours. As 152 Tb decay by positron emission it can be utilised for diagnostics by positron emission tomography. For use in radiopharmaceuticals and for activity measurements by an activity calibrator a high radionuclide purity of the material and an accurate and precise knowledge of the half-life is required. Mass-separation and radiochemical purification provide a production route of high purity 152Tb. In the current work, two mass-separated samples from the CERN-ISOLDE facility have been assayed at the National Physical Laboratory to investigate the radionuclide purity. These samples have been used to perform four measurements of the half-life by three independent techniques: high-purity germanium gamma-ray spectrometry, ionisation chamber measurements and liquid scintillation counting. From the four measurement campaigns a half-life of 17.8784(95) h has been determined. The reported half-life shows a significant difference to the currently evaluated half-life (ζ-score = 3.77), with a relative difference of 2.2 % and an order of magnitude improvement in the precision. This work also shows that under controlled conditions the combination of mass-separation and radiochemical separation can provide high-purity 152Tb.
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Affiliation(s)
- S M Collins
- National Physical Laboratory, Hampton Road, Teddington, TW11 0LW, UK; School of Mathematics and Physics, University of Surrey, Guildford, GU2 7XH, UK.
| | - U Köster
- Institut Laue-Langevin, 38042, Grenoble, France
| | - A P Robinson
- National Physical Laboratory, Hampton Road, Teddington, TW11 0LW, UK; Christie Medical Physics and Engineering (CMPE), The Christie NHS Foundation Trust, Manchester, M20 4BX, UK; The University of Manchester, Manchester, M13 9PL, UK
| | - P Ivanov
- National Physical Laboratory, Hampton Road, Teddington, TW11 0LW, UK
| | - T E Cocolios
- KU Leuven, Institute for Nuclear and Radiation Physics, Celestijnenlaan 200D, 3001, Leuven, Belgium
| | - B Russell
- National Physical Laboratory, Hampton Road, Teddington, TW11 0LW, UK
| | - A J Fenwick
- National Physical Laboratory, Hampton Road, Teddington, TW11 0LW, UK
| | - C Bernerd
- KU Leuven, Institute for Nuclear and Radiation Physics, Celestijnenlaan 200D, 3001, Leuven, Belgium; CERN - European Organization for Nuclear Research, Esplanade des Particules 1, 1217, Meyrin, Switzerland
| | - S Stegemann
- KU Leuven, Institute for Nuclear and Radiation Physics, Celestijnenlaan 200D, 3001, Leuven, Belgium
| | - K Johnston
- CERN - European Organization for Nuclear Research, Esplanade des Particules 1, 1217, Meyrin, Switzerland
| | - A M Gerami
- CERN - European Organization for Nuclear Research, Esplanade des Particules 1, 1217, Meyrin, Switzerland
| | - K Chrysalidis
- CERN - European Organization for Nuclear Research, Esplanade des Particules 1, 1217, Meyrin, Switzerland
| | - H Mohamud
- National Physical Laboratory, Hampton Road, Teddington, TW11 0LW, UK
| | - N Ramirez
- National Physical Laboratory, Hampton Road, Teddington, TW11 0LW, UK
| | - A Bhaisare
- National Physical Laboratory, Hampton Road, Teddington, TW11 0LW, UK
| | - J Mewburn-Crook
- National Physical Laboratory, Hampton Road, Teddington, TW11 0LW, UK
| | - D M Cullen
- The University of Manchester, Manchester, M13 9PL, UK
| | - B Pietras
- The University of Manchester, Manchester, M13 9PL, UK
| | - S Pells
- The University of Manchester, Manchester, M13 9PL, UK
| | - K Dockx
- KU Leuven, Institute for Nuclear and Radiation Physics, Celestijnenlaan 200D, 3001, Leuven, Belgium
| | - N Stucki
- HEPIA, HES-SO, University of Applied Sciences and Arts Western Switzerland, Rue de la Prairie 4, 1202, Geneva, Switzerland
| | - P H Regan
- National Physical Laboratory, Hampton Road, Teddington, TW11 0LW, UK; School of Mathematics and Physics, University of Surrey, Guildford, GU2 7XH, UK
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Mantovan R, Fallica R, Mokhles Gerami A, Mølholt TE, Wiemer C, Longo M, Gunnlaugsson HP, Johnston K, Masenda H, Naidoo D, Ncube M, Bharuth-Ram K, Fanciulli M, Gislason HP, Langouche G, Ólafsson S, Weyer G. Atomic-scale study of the amorphous-to-crystalline phase transition mechanism in GeTe thin films. Sci Rep 2017; 7:8234. [PMID: 28811632 PMCID: PMC5558007 DOI: 10.1038/s41598-017-08275-5] [Citation(s) in RCA: 11] [Impact Index Per Article: 1.6] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Download PDF] [Figures] [Journal Information] [Subscribe] [Scholar Register] [Received: 04/05/2017] [Accepted: 07/10/2017] [Indexed: 11/25/2022] Open
Abstract
The underlying mechanism driving the structural amorphous-to-crystalline transition in Group VI chalcogenides is still a matter of debate even in the simplest GeTe system. We exploit the extreme sensitivity of 57Fe emission Mössbauer spectroscopy, following dilute implantation of 57Mn (T½ = 1.5 min) at ISOLDE/CERN, to study the electronic charge distribution in the immediate vicinity of the 57Fe probe substituting Ge (FeGe), and to interrogate the local environment of FeGe over the amorphous-crystalline phase transition in GeTe thin films. Our results show that the local structure of as-sputtered amorphous GeTe is a combination of tetrahedral and defect-octahedral sites. The main effect of the crystallization is the conversion from tetrahedral to defect-free octahedral sites. We discover that only the tetrahedral fraction in amorphous GeTe participates to the change of the FeGe-Te chemical bonds, with a net electronic charge density transfer of ~ 1.6 e/a0 between FeGe and neighboring Te atoms. This charge transfer accounts for a lowering of the covalent character during crystallization. The results are corroborated by theoretical calculations within the framework of density functional theory. The observed atomic-scale chemical-structural changes are directly connected to the macroscopic phase transition and resistivity switch of GeTe thin films.
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Affiliation(s)
- R Mantovan
- Laboratorio MDM, IMM-CNR, Via Olivetti 2, 20864, Agrate Brianza (MB), Italy.
| | - R Fallica
- Laboratorio MDM, IMM-CNR, Via Olivetti 2, 20864, Agrate Brianza (MB), Italy.,Laboratory for Micro- and Nanotechnology, Paul Scherrer Institute, 5232, Villigen PSI, Switzerland
| | - A Mokhles Gerami
- Physics Department, ISOLDE/CERN, Geneva 23, Switzerland.,Dept. of Physics, K. N. Toosi University of Technology, P.O. Box 15875-4416, Tehran, Iran
| | - T E Mølholt
- Physics Department, ISOLDE/CERN, Geneva 23, Switzerland
| | - C Wiemer
- Laboratorio MDM, IMM-CNR, Via Olivetti 2, 20864, Agrate Brianza (MB), Italy
| | - M Longo
- Laboratorio MDM, IMM-CNR, Via Olivetti 2, 20864, Agrate Brianza (MB), Italy.
| | - H P Gunnlaugsson
- Science Institute, University of Iceland, Dunhaga 3, 107 Reykjavík, Iceland
| | - K Johnston
- Physics Department, ISOLDE/CERN, Geneva 23, Switzerland
| | - H Masenda
- School of Physics, University of the Witwatersrand, Johannesburg, 2050, South Africa
| | - D Naidoo
- School of Physics, University of the Witwatersrand, Johannesburg, 2050, South Africa
| | - M Ncube
- School of Physics, University of the Witwatersrand, Johannesburg, 2050, South Africa
| | - K Bharuth-Ram
- Durban University of Technology, Durban, 4000, South Africa.,School of Chemistry and Physics, University of KwaZulu-Natal, Durban, 4000, South Africa
| | - M Fanciulli
- Laboratorio MDM, IMM-CNR, Via Olivetti 2, 20864, Agrate Brianza (MB), Italy.,Dipartimento di Scienza dei Materiali, Università di Milano Bicocca, Milano, Italy
| | - H P Gislason
- Science Institute, University of Iceland, Dunhaga 3, 107 Reykjavík, Iceland
| | - G Langouche
- KU Leuven, Instituut voor Kern-en Stralings Fysika, B-3001, Leuven, Belgium
| | - S Ólafsson
- Science Institute, University of Iceland, Dunhaga 3, 107 Reykjavík, Iceland
| | - G Weyer
- Department of Physics and Astronomy, Aarhus University, Aarhus C, Denmark
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Mølholt TE, Gunnlaugsson HP, Johnston K, Mantovan R, Röder J, Adoons V, Mokhles Gerami A, Masenda H, Matveyev YA, Ncube M, Unzueta I, Bharuth-Ram K, Gislason HP, Krastev P, Langouche G, Naidoo D, Ólafsson S, Zenkevich A. Charge states and lattice sites of dilute implanted Sn in ZnO. J Phys Condens Matter 2017; 29:155701. [PMID: 28165333 DOI: 10.1088/1361-648x/aa5e95] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 06/06/2023]
Abstract
The common charge states of Sn are 2+ and 4+. While charge neutrality considerations favour 2+ to be the natural charge state of Sn in ZnO, there are several reports suggesting the 4+ state instead. In order to investigate the charge states, lattice sites, and the effect of the ion implantation process of dilute Sn atoms in ZnO, we have performed 119Sn emission Mössbauer spectroscopy on ZnO single crystal samples following ion implantation of radioactive 119In (T ½ = 2.4 min) at temperatures between 96 K and 762 K. Complementary perturbed angular correlation measurements on 111mCd implanted ZnO were also conducted. Our results show that the 2+ state is the natural charge state for Sn in defect free ZnO and that the 4+ charge state is stabilized by acceptor defects created in the implantation process.
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Affiliation(s)
- T E Mølholt
- EP Department, ISOLDE/CERN, 1211 Geneva 23, Switzerland
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