Lucian Mathes, Maximilian Suhr, Vassily V. Burwitz, Danny R. Russell, Sebastian Vohburger, Christoph Hugenschmidt
{"title":"极低正电子能量下的表面和近表面正电子湮灭光谱学","authors":"Lucian Mathes, Maximilian Suhr, Vassily V. Burwitz, Danny R. Russell, Sebastian Vohburger, Christoph Hugenschmidt","doi":"arxiv-2409.07952","DOIUrl":null,"url":null,"abstract":"We present a monoenergetic positron beam specifically tailored to the needs\nof (near-) surface positron annihilation spectroscopy. The Setup for LOw-energy\nPositron Experiments (SLOPE) comprises a high-activity 22Na source, a tungsten\nmoderator, electrostatic extraction and acceleration, magnetic beam guidance,\nas well as an analysis chamber with a movable sample holder and a {\\gamma}-ray\ndetection system. The tungsten moderator foil, biased between 0 and 30 V, in\ncombination with the HV-biasable sample holder, enables positron implantation\nenergies between 3 eV and 40 keV. At low energies (<20 eV), the count rate\ntypically amounts to 4400 counts per second, and the beam diameter is smaller\nthan 12 +/- 3 mm. We conduct phase space simulations of the positron beam using\nCOMSOL Multiphysics (c) to characterize the beam properties and compare the\nfindings with the experimentally determined energy-dependent beam diameter. To\nshowcase the capabilities of SLOPE, we perform studies of positronium (Ps)\nformation on boehmite and depth-resolved coincidence Doppler-broadening\nspectroscopy (CDBS) of copper. In particular, the Ps formation at the\nhydrogen-terminated surface of boehmite is found to be maximum at a positron\nimplantation energy of 10 eV. The range of positron energies for which we\nobserve Ps formation agrees with the hydrogen ionization energy.","PeriodicalId":501374,"journal":{"name":"arXiv - PHYS - Instrumentation and Detectors","volume":"48 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-09-12","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Surface and Near-Surface Positron Annihilation Spectroscopy at Very Low Positron Energy\",\"authors\":\"Lucian Mathes, Maximilian Suhr, Vassily V. Burwitz, Danny R. Russell, Sebastian Vohburger, Christoph Hugenschmidt\",\"doi\":\"arxiv-2409.07952\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"We present a monoenergetic positron beam specifically tailored to the needs\\nof (near-) surface positron annihilation spectroscopy. The Setup for LOw-energy\\nPositron Experiments (SLOPE) comprises a high-activity 22Na source, a tungsten\\nmoderator, electrostatic extraction and acceleration, magnetic beam guidance,\\nas well as an analysis chamber with a movable sample holder and a {\\\\gamma}-ray\\ndetection system. The tungsten moderator foil, biased between 0 and 30 V, in\\ncombination with the HV-biasable sample holder, enables positron implantation\\nenergies between 3 eV and 40 keV. At low energies (<20 eV), the count rate\\ntypically amounts to 4400 counts per second, and the beam diameter is smaller\\nthan 12 +/- 3 mm. We conduct phase space simulations of the positron beam using\\nCOMSOL Multiphysics (c) to characterize the beam properties and compare the\\nfindings with the experimentally determined energy-dependent beam diameter. To\\nshowcase the capabilities of SLOPE, we perform studies of positronium (Ps)\\nformation on boehmite and depth-resolved coincidence Doppler-broadening\\nspectroscopy (CDBS) of copper. In particular, the Ps formation at the\\nhydrogen-terminated surface of boehmite is found to be maximum at a positron\\nimplantation energy of 10 eV. The range of positron energies for which we\\nobserve Ps formation agrees with the hydrogen ionization energy.\",\"PeriodicalId\":501374,\"journal\":{\"name\":\"arXiv - PHYS - Instrumentation and Detectors\",\"volume\":\"48 1\",\"pages\":\"\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2024-09-12\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"arXiv - PHYS - Instrumentation and Detectors\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/arxiv-2409.07952\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"arXiv - PHYS - Instrumentation and Detectors","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/arxiv-2409.07952","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Surface and Near-Surface Positron Annihilation Spectroscopy at Very Low Positron Energy
We present a monoenergetic positron beam specifically tailored to the needs
of (near-) surface positron annihilation spectroscopy. The Setup for LOw-energy
Positron Experiments (SLOPE) comprises a high-activity 22Na source, a tungsten
moderator, electrostatic extraction and acceleration, magnetic beam guidance,
as well as an analysis chamber with a movable sample holder and a {\gamma}-ray
detection system. The tungsten moderator foil, biased between 0 and 30 V, in
combination with the HV-biasable sample holder, enables positron implantation
energies between 3 eV and 40 keV. At low energies (<20 eV), the count rate
typically amounts to 4400 counts per second, and the beam diameter is smaller
than 12 +/- 3 mm. We conduct phase space simulations of the positron beam using
COMSOL Multiphysics (c) to characterize the beam properties and compare the
findings with the experimentally determined energy-dependent beam diameter. To
showcase the capabilities of SLOPE, we perform studies of positronium (Ps)
formation on boehmite and depth-resolved coincidence Doppler-broadening
spectroscopy (CDBS) of copper. In particular, the Ps formation at the
hydrogen-terminated surface of boehmite is found to be maximum at a positron
implantation energy of 10 eV. The range of positron energies for which we
observe Ps formation agrees with the hydrogen ionization energy.