Lisa-Marie Krug , Leon Chryssos , Jürgen Bundesmann , Alina Dittwald , Georgios Kourkafas , Andrea Denker , Christoph Hugenschmidt
{"title":"利用 27Al(p,x)22Na 反应生产基于质子束的正电子发射器","authors":"Lisa-Marie Krug , Leon Chryssos , Jürgen Bundesmann , Alina Dittwald , Georgios Kourkafas , Andrea Denker , Christoph Hugenschmidt","doi":"10.1016/j.nimb.2024.165488","DOIUrl":null,"url":null,"abstract":"<div><p>Positron annihilation experiments on an laboratory scale depend on the supply and the availability of <span><math><msup><mrow><mi>β</mi></mrow><mrow><mo>+</mo></mrow></msup></math></span> emitters. Here we present the production of positron sources based on the <sup>27</sup>Al(p,x)<sup>22</sup>Na reaction by irradiation of Al with a 68<!--> <!-->MeV proton beam. We simulated the energy loss, range and radial scattering of the protons in Al in order to design a simple target consisting of a stack of Al discs. Our approach allows (i) the direct use of the Al discs as positron emitters that inherently avoids wet chemical processes as usually applied in commercial production of carrier-free <sup>22</sup>Na, (ii) the production of multiple positron sources at once, and (iii) the simple measurement of the depth and lateral distribution of <sup>22</sup>Na. We precisely determined the cross section of the <sup>27</sup>Al(p,x)<sup>22</sup>Na reaction which was found to differ from literature values particularly for proton energies between 27 and 40<!--> <!-->MeV. The activity of all nuclides produced (apart from <sup>22</sup>Na) was shown to be negligible 15 days after irradiation. The production of radionuclides such as <sup>48</sup>Sc, <sup>54</sup>Mn and <sup>56</sup>Co can be prevented by using Al of a higher purity. The concept presented here can easily be adapted for the production of stronger <sup>22</sup>Na sources by increasing the proton current or/and the irradiation time.</p></div>","PeriodicalId":19380,"journal":{"name":"Nuclear Instruments & Methods in Physics Research Section B-beam Interactions With Materials and Atoms","volume":"555 ","pages":"Article 165488"},"PeriodicalIF":1.4000,"publicationDate":"2024-08-06","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.sciencedirect.com/science/article/pii/S0168583X24002581/pdfft?md5=c33f68bff05ab5056b1a9bda22da6f17&pid=1-s2.0-S0168583X24002581-main.pdf","citationCount":"0","resultStr":"{\"title\":\"Proton beam based production of positron emitters by exploiting the 27Al(p,x)22Na reaction\",\"authors\":\"Lisa-Marie Krug , Leon Chryssos , Jürgen Bundesmann , Alina Dittwald , Georgios Kourkafas , Andrea Denker , Christoph Hugenschmidt\",\"doi\":\"10.1016/j.nimb.2024.165488\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><p>Positron annihilation experiments on an laboratory scale depend on the supply and the availability of <span><math><msup><mrow><mi>β</mi></mrow><mrow><mo>+</mo></mrow></msup></math></span> emitters. Here we present the production of positron sources based on the <sup>27</sup>Al(p,x)<sup>22</sup>Na reaction by irradiation of Al with a 68<!--> <!-->MeV proton beam. We simulated the energy loss, range and radial scattering of the protons in Al in order to design a simple target consisting of a stack of Al discs. Our approach allows (i) the direct use of the Al discs as positron emitters that inherently avoids wet chemical processes as usually applied in commercial production of carrier-free <sup>22</sup>Na, (ii) the production of multiple positron sources at once, and (iii) the simple measurement of the depth and lateral distribution of <sup>22</sup>Na. We precisely determined the cross section of the <sup>27</sup>Al(p,x)<sup>22</sup>Na reaction which was found to differ from literature values particularly for proton energies between 27 and 40<!--> <!-->MeV. The activity of all nuclides produced (apart from <sup>22</sup>Na) was shown to be negligible 15 days after irradiation. The production of radionuclides such as <sup>48</sup>Sc, <sup>54</sup>Mn and <sup>56</sup>Co can be prevented by using Al of a higher purity. The concept presented here can easily be adapted for the production of stronger <sup>22</sup>Na sources by increasing the proton current or/and the irradiation time.</p></div>\",\"PeriodicalId\":19380,\"journal\":{\"name\":\"Nuclear Instruments & Methods in Physics Research Section B-beam Interactions With Materials and Atoms\",\"volume\":\"555 \",\"pages\":\"Article 165488\"},\"PeriodicalIF\":1.4000,\"publicationDate\":\"2024-08-06\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"https://www.sciencedirect.com/science/article/pii/S0168583X24002581/pdfft?md5=c33f68bff05ab5056b1a9bda22da6f17&pid=1-s2.0-S0168583X24002581-main.pdf\",\"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/S0168583X24002581\",\"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/S0168583X24002581","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}
Proton beam based production of positron emitters by exploiting the 27Al(p,x)22Na reaction
Positron annihilation experiments on an laboratory scale depend on the supply and the availability of emitters. Here we present the production of positron sources based on the 27Al(p,x)22Na reaction by irradiation of Al with a 68 MeV proton beam. We simulated the energy loss, range and radial scattering of the protons in Al in order to design a simple target consisting of a stack of Al discs. Our approach allows (i) the direct use of the Al discs as positron emitters that inherently avoids wet chemical processes as usually applied in commercial production of carrier-free 22Na, (ii) the production of multiple positron sources at once, and (iii) the simple measurement of the depth and lateral distribution of 22Na. We precisely determined the cross section of the 27Al(p,x)22Na reaction which was found to differ from literature values particularly for proton energies between 27 and 40 MeV. The activity of all nuclides produced (apart from 22Na) was shown to be negligible 15 days after irradiation. The production of radionuclides such as 48Sc, 54Mn and 56Co can be prevented by using Al of a higher purity. The concept presented here can easily be adapted for the production of stronger 22Na sources by increasing the proton current or/and the irradiation time.
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.