Systematic analysis of different experimental approaches to measure electronic stopping of very slow hydrogen ions
The electronic stopping cross section (SCS) of Ni for slow H+, H2 +, D+ and D2 + ions has been investigated for different types of targets in two complementary experimental geometries, i.e., in transmission and backscattering. To warrant sample purity, both a high purity nickel sheet and nanometer N...
| Authors: | , , , , , , , , |
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| Format: | article |
| Status: | Published version |
| Publication Date: | 2018 |
| Country: | Argentina |
| Institution: | Consejo Nacional de Investigaciones Científicas y Técnicas |
| Repository: | CONICET Digital (CONICET) |
| Language: | English |
| OAI Identifier: | oai:ri.conicet.gov.ar:11336/181800 |
| Online Access: | http://hdl.handle.net/11336/181800 |
| Access Level: | Open access |
| Keyword: | BACKSCATTERING ELECTRONIC STOPPING LEIS NICKEL PROTONS TRANSMISSION https://purl.org/becyt/ford/1.3 https://purl.org/becyt/ford/1 |
| Summary: | The electronic stopping cross section (SCS) of Ni for slow H+, H2 +, D+ and D2 + ions has been investigated for different types of targets in two complementary experimental geometries, i.e., in transmission and backscattering. To warrant sample purity, both a high purity nickel sheet and nanometer Ni layers were prepared in-situ under ultra-high-vacuum conditions. In an alternative approach, ultra-thin samples were prepared ex-situ as self-supporting foils and as nanometer films on a polished substrate (silicon). Identical SCS results are obtained in backscattering using the in-situ prepared film and the high purity sheet. The ex-situ prepared targets contained considerable concentrations of impurities of low atomic numbers, whose contribution to the SCS can be rectified by applying Bragg's rule using TRIM stopping for the impurities. In this way for the ex-situ targets the accuracy of the resulting SCS data is improved considerably. Concordant stopping cross section data are obtained in both geometries. The achieved accuracy does, however, not permit to spot a possible influence of different impact parameter regimes explored in transmission and in backscattering geometries. |
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