IFEG   20353
INSTITUTO DE FISICA ENRIQUE GAVIOLA
Unidad Ejecutora - UE
congresos y reuniones científicas
Título:
Nitrogen ionization cross section by electron impact
Autor/es:
ANA BERTOL; PABLO PÉREZ; JORGE TRINCAVELLI; GUSTAVO CASTELLANO; RUTH HINRICHS; MARCOS VASCONCELLOS
Lugar:
Gramado - Rio Grande do Sul
Reunión:
Congreso; 13th International Conference on Particle-Induced X-ray Emission; 2013
Institución organizadora:
Laboratório de Implantação Iónica, Instituo de Física, Universidade Federal do Rio Grande do Sul, Sociedade Brasileira de Física, International Atomic Energy Agency
Resumen:
The electron impact ionization cross sections (s) of light elements were recently reviewed [1], however the developed models were based on data from the early nineteen-seventies that had used varied experimental setups, e.g. gaseous samples, or organic films of nucleic acid bases sublimated on thin carbon films mounted on TEM copper grids. More recently the s of heavier elements have been determined with thin mono-elemental films deposited on substrates. It has been shown that the influence of chemical bonding on the s values is negligible [2], so the ionization cross section can also be experimentally determined measuring the characteristic X-ray spectrum emitted by a thin compound film containing the desired element (e.g. nitrides or oxides). In this work the nitrogen ionization cross section was determined using films of AlN, Si N , TiN, and FeN 3 4 with 10 nm thickness, deposited by magnetron sputtering (AJA International model ATC, ORION 8 UHV, LCN, Instituto de Física of Univ. Federal do Rio Grande do Sul, Brasil) on carbon planchets. The mass thicknesses of the films were determined using Rutherford backscattering spectrometry (RBS) in a 3MeV ion accelerator (High Voltage Engineering, Tandetron 3MV in the Laboratório de Implantação Iônica, IFUFRGS, Brasil). Nitrogen X-ray spectra were acquired in an electron microprobe (JEOL JXA 8230 in the Laboratorio de Microscopía Electrónica y Análisis por Rayos X of the Univ. Nacional de Córdoba, Argentina) equipped with a wavelength dispersive spectrometer (WDS) using a synthetic crystal (LDE1) with 2d≈ 60 Å. The spectra were measured at beam energies of 1.0, 1.2, 1.5, 2.0, 3.0, 4.0, and 5.0 keV (see Figure 1).