Calculation of energy-loss straggling of C, Al, Si, and Cu for fast H, He, and Li ions

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We present theoretical calculations of the energy-loss straggling of C, Al, Si, and Cu targets for H, He, and Li ions in the range of intermediate to high energies (0.01-10 MeV u). These calculations have been done by employing the dielectric formalism and by considering the different equilibrium ch...

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Autor principal: Montanari, C.C
Otros Autores: Miraglia, Jorge Esteban, Heredia-Avalos, S., Garcia-Molina, R., Abril, I.
Formato: Capítulo de libro
Lenguaje:Inglés
Publicado: 2007
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Biblioteca Central Dr. Luis F. Leloir (FCEN) de Universidad de Buenos Aires
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100 1 |a Montanari, C.C. 
245 1 0 |a Calculation of energy-loss straggling of C, Al, Si, and Cu for fast H, He, and Li ions 
260 |c 2007 
270 1 0 |m Montanari, C.C.; Instituto de Astronomía y Física del Espacio, Casilla de correo 67, Sucursal 28, 1428 Buenos Aires, Argentina 
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506 |2 openaire  |e Política editorial 
520 3 |a We present theoretical calculations of the energy-loss straggling of C, Al, Si, and Cu targets for H, He, and Li ions in the range of intermediate to high energies (0.01-10 MeV u). These calculations have been done by employing the dielectric formalism and by considering the different equilibrium charge states of the swift ion inside the solid as a function of its energy. Two different models are used: the Mermin energy-loss functions combined with generalized oscillator strengths (MELF-GOS) and the shellwise application of the local plasma approximation (SLPA). The MELF-GOS describes the target outer-electron excitations through a fitting to experimental data in the optical limit, employing a linear combination of Mermin-type energy-loss functions; the excitations of the inner-shell electrons are taken into account by means of generalized oscillator strengths. The SLPA employs a free-electron-gas model for the target valence electrons and the local density approximation for each shell of target electrons separately by using Hartree-Fock atomic wave functions. The results of the energy-loss straggling obtained by the two independent models show good agreement with the available experimental data. The calculated energy-loss straggling tends at high energies to the Bohr value and takes values below it at intermediate energies. The Bethe-Livingston shoulder (or overshooting) at intermediate energies does not appear in the present calculations. We find that the energy-loss straggling normalized to ZP2 is almost independent of the ion atomic number ZP; therefore, the results for H, He, and Li projectiles in each target can be approximated by a universal curve at high energies. © 2007 The American Physical Society.  |l eng 
593 |a Instituto de Astronomía y Física del Espacio, Casilla de correo 67, Sucursal 28, 1428 Buenos Aires, Argentina 
593 |a Departamento de Física, Facultad de Ciencias Exactas y Naturales, Universidad de Buenos Aires, Argentina 
593 |a Departamento de Física - CIOyN, Universidad de Murcia, Apartado 4021, E-30080 Murcia, Spain 
593 |a Departament de Física Aplicada, Universitat d'Alacant, Apartat 99, E-03080 Alacant, Spain 
650 1 7 |2 spines  |a CARBON 
690 1 0 |a ALUMINUM 
690 1 0 |a DIELECTRIC DEVICES 
690 1 0 |a ELECTRIC CHARGE 
690 1 0 |a IONS 
690 1 0 |a OSCILLATORS (ELECTRONIC) 
690 1 0 |a PLASMA APPLICATIONS 
690 1 0 |a SILICON 
690 1 0 |a BOHR VALUE 
690 1 0 |a DIELECTRIC FORMALISM 
690 1 0 |a MERMIN ENERGY-LOSS FUNCTIONS MODEL 
690 1 0 |a OSCILLATOR STRENGTHS (MELF-GOS) 
690 1 0 |a ATOMIC PHYSICS 
700 1 |a Miraglia, Jorge Esteban 
700 1 |a Heredia-Avalos, S. 
700 1 |a Garcia-Molina, R. 
700 1 |a Abril, I. 
773 0 |d 2007  |g v. 75  |k n. 2  |p Phys Rev A  |x 10502947  |t Physical Review A - Atomic, Molecular, and Optical Physics 
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856 4 0 |u https://doi.org/10.1103/PhysRevA.75.022903  |y DOI 
856 4 0 |u https://hdl.handle.net/20.500.12110/paper_10502947_v75_n2_p_Montanari  |y Handle 
856 4 0 |u https://bibliotecadigital.exactas.uba.ar/collection/paper/document/paper_10502947_v75_n2_p_Montanari  |y Registro en la Biblioteca Digital 
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999 |c 67668 

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