Carlos Vivo-Vilches , Esad Hrnjic , Martin Martschini , Kyra Altindag , Lee W. Packer , Robin Golser , Karin Hain
{"title":"对熔合环境中产生的91Nb、94Nb和93Mo的AMS测量","authors":"Carlos Vivo-Vilches , Esad Hrnjic , Martin Martschini , Kyra Altindag , Lee W. Packer , Robin Golser , Karin Hain","doi":"10.1016/j.nimb.2025.165847","DOIUrl":null,"url":null,"abstract":"<div><div>Long-lived radionuclides, such as <sup>91</sup>Nb, <sup>94</sup>Nb and <sup>93</sup>Mo, are expected to be produced in nuclear fusion reactors by reactions of high-energy neutrons with the structural material. Accurate predictions of waste categorization require experimental validation of simulation codes like FISPACT-II. This work explores the use of Ion-Laser InterAction Mass Spectrometry (ILIAMS) at the Vienna Environmental Research Accelerator (VERA) to measure these three radionuclides by accelerator mass spectrometry (AMS). The ILIAMS setup employs laser photodetachment to suppress their respective stable isobars: <sup>91</sup>Zr, <sup>94</sup>Zr and <sup>94</sup>Mo, and <sup>93</sup>Nb.</div><div>For <sup>91,94</sup>Nb measurements, NbO<sub>3</sub><sup>−</sup> is selected, with interferences from ZrO<sub>3</sub><sup>−</sup> suppressed by collisions with the He buffer gas in the ion cooler. The suppression can be enhanced by overlapping a 355 nm laser with the ion beam. The lower limit for the suppression factor is 37000. In that way, we reach <sup>91</sup>Zr/<sup>93</sup>Nb and <sup>94</sup>Zr/<sup>93</sup>Nb levels of 1.2 × 10<sup>−14</sup> and 1.8 × 10<sup>−14</sup>, respectively, in targets prepared from commercial Nb<sub>2</sub>O<sub>5</sub>. MoO<sub>3</sub><sup>−</sup> is suppressed by a factor of 4360, leading to a <sup>94</sup>Mo/<sup>93</sup>Nb interference of 1.28 × 10<sup>−10</sup> in the same targets.</div><div>For <sup>93</sup>Mo measurements, MoO<sub>2</sub><sup>−</sup> is selected, with interference from NbO<sub>2</sub><sup>−</sup> suppressed by 637 nm photons by a factor of 5.5 × 10<sup>6</sup>. This results in a <sup>93</sup>Nb/<sup>nat</sup>Mo level of 1.3 × 10<sup>−13</sup> in targets prepared from commercial MoO<sub>3</sub>.</div><div>Suppression factors as high as this are not achieved by isobar suppression techniques based on differences in energy loss, not even by AMS facilities with terminal voltages above 8.5 MV.</div></div>","PeriodicalId":19380,"journal":{"name":"Nuclear Instruments & Methods in Physics Research Section B-beam Interactions With Materials and Atoms","volume":"568 ","pages":"Article 165847"},"PeriodicalIF":1.4000,"publicationDate":"2025-08-29","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Towards AMS measurements of 91Nb, 94Nb and 93Mo produced in fusion environment\",\"authors\":\"Carlos Vivo-Vilches , Esad Hrnjic , Martin Martschini , Kyra Altindag , Lee W. Packer , Robin Golser , Karin Hain\",\"doi\":\"10.1016/j.nimb.2025.165847\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><div>Long-lived radionuclides, such as <sup>91</sup>Nb, <sup>94</sup>Nb and <sup>93</sup>Mo, are expected to be produced in nuclear fusion reactors by reactions of high-energy neutrons with the structural material. Accurate predictions of waste categorization require experimental validation of simulation codes like FISPACT-II. This work explores the use of Ion-Laser InterAction Mass Spectrometry (ILIAMS) at the Vienna Environmental Research Accelerator (VERA) to measure these three radionuclides by accelerator mass spectrometry (AMS). The ILIAMS setup employs laser photodetachment to suppress their respective stable isobars: <sup>91</sup>Zr, <sup>94</sup>Zr and <sup>94</sup>Mo, and <sup>93</sup>Nb.</div><div>For <sup>91,94</sup>Nb measurements, NbO<sub>3</sub><sup>−</sup> is selected, with interferences from ZrO<sub>3</sub><sup>−</sup> suppressed by collisions with the He buffer gas in the ion cooler. The suppression can be enhanced by overlapping a 355 nm laser with the ion beam. The lower limit for the suppression factor is 37000. In that way, we reach <sup>91</sup>Zr/<sup>93</sup>Nb and <sup>94</sup>Zr/<sup>93</sup>Nb levels of 1.2 × 10<sup>−14</sup> and 1.8 × 10<sup>−14</sup>, respectively, in targets prepared from commercial Nb<sub>2</sub>O<sub>5</sub>. MoO<sub>3</sub><sup>−</sup> is suppressed by a factor of 4360, leading to a <sup>94</sup>Mo/<sup>93</sup>Nb interference of 1.28 × 10<sup>−10</sup> in the same targets.</div><div>For <sup>93</sup>Mo measurements, MoO<sub>2</sub><sup>−</sup> is selected, with interference from NbO<sub>2</sub><sup>−</sup> suppressed by 637 nm photons by a factor of 5.5 × 10<sup>6</sup>. This results in a <sup>93</sup>Nb/<sup>nat</sup>Mo level of 1.3 × 10<sup>−13</sup> in targets prepared from commercial MoO<sub>3</sub>.</div><div>Suppression factors as high as this are not achieved by isobar suppression techniques based on differences in energy loss, not even by AMS facilities with terminal voltages above 8.5 MV.</div></div>\",\"PeriodicalId\":19380,\"journal\":{\"name\":\"Nuclear Instruments & Methods in Physics Research Section B-beam Interactions With Materials and Atoms\",\"volume\":\"568 \",\"pages\":\"Article 165847\"},\"PeriodicalIF\":1.4000,\"publicationDate\":\"2025-08-29\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Nuclear Instruments & Methods in Physics Research Section B-beam Interactions With Materials and Atoms\",\"FirstCategoryId\":\"101\",\"ListUrlMain\":\"https://www.sciencedirect.com/science/article/pii/S0168583X2500237X\",\"RegionNum\":3,\"RegionCategory\":\"物理与天体物理\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q3\",\"JCRName\":\"INSTRUMENTS & INSTRUMENTATION\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Nuclear Instruments & Methods in Physics Research Section B-beam Interactions With Materials and Atoms","FirstCategoryId":"101","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S0168583X2500237X","RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q3","JCRName":"INSTRUMENTS & INSTRUMENTATION","Score":null,"Total":0}
Towards AMS measurements of 91Nb, 94Nb and 93Mo produced in fusion environment
Long-lived radionuclides, such as 91Nb, 94Nb and 93Mo, are expected to be produced in nuclear fusion reactors by reactions of high-energy neutrons with the structural material. Accurate predictions of waste categorization require experimental validation of simulation codes like FISPACT-II. This work explores the use of Ion-Laser InterAction Mass Spectrometry (ILIAMS) at the Vienna Environmental Research Accelerator (VERA) to measure these three radionuclides by accelerator mass spectrometry (AMS). The ILIAMS setup employs laser photodetachment to suppress their respective stable isobars: 91Zr, 94Zr and 94Mo, and 93Nb.
For 91,94Nb measurements, NbO3− is selected, with interferences from ZrO3− suppressed by collisions with the He buffer gas in the ion cooler. The suppression can be enhanced by overlapping a 355 nm laser with the ion beam. The lower limit for the suppression factor is 37000. In that way, we reach 91Zr/93Nb and 94Zr/93Nb levels of 1.2 × 10−14 and 1.8 × 10−14, respectively, in targets prepared from commercial Nb2O5. MoO3− is suppressed by a factor of 4360, leading to a 94Mo/93Nb interference of 1.28 × 10−10 in the same targets.
For 93Mo measurements, MoO2− is selected, with interference from NbO2− suppressed by 637 nm photons by a factor of 5.5 × 106. This results in a 93Nb/natMo level of 1.3 × 10−13 in targets prepared from commercial MoO3.
Suppression factors as high as this are not achieved by isobar suppression techniques based on differences in energy loss, not even by AMS facilities with terminal voltages above 8.5 MV.
期刊介绍:
Section B of Nuclear Instruments and Methods in Physics Research covers all aspects of the interaction of energetic beams with atoms, molecules and aggregate forms of matter. This includes ion beam analysis and ion beam modification of materials as well as basic data of importance for these studies. Topics of general interest include: atomic collisions in solids, particle channelling, all aspects of collision cascades, the modification of materials by energetic beams, ion implantation, irradiation - induced changes in materials, the physics and chemistry of beam interactions and the analysis of materials by all forms of energetic radiation. Modification by ion, laser and electron beams for the study of electronic materials, metals, ceramics, insulators, polymers and other important and new materials systems are included. Related studies, such as the application of ion beam analysis to biological, archaeological and geological samples as well as applications to solve problems in planetary science are also welcome. Energetic beams of interest include atomic and molecular ions, neutrons, positrons and muons, plasmas directed at surfaces, electron and photon beams, including laser treated surfaces and studies of solids by photon radiation from rotating anodes, synchrotrons, etc. In addition, the interaction between various forms of radiation and radiation-induced deposition processes are relevant.