The magnetic hyperfine field at 140Ce in nickel

The hyperfine interaction of140Ce in nickel has been investigated by the time-differential perturbed-angular-correlation technique (TDPAC). The probe was produced by isotope separator implantation of the fission product140Xe, the β- decay chain of which finally populates excited states of140Ce. Diff...

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Autores principales: Bibiloni, Aníbal Guillermo, Caracoche, María Cristina, López García, Alberto Raúl, Martínez, Jorge Alberto, Mendoza Zélis, Luis Alejandro, Mercader, Roberto Carlos, Pasquevich, Alberto Felipe
Formato: Articulo
Lenguaje:Inglés
Publicado: 1977
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Acceso en línea:http://sedici.unlp.edu.ar/handle/10915/133956
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id I19-R120-10915-133956
record_format dspace
institution Universidad Nacional de La Plata
institution_str I-19
repository_str R-120
collection SEDICI (UNLP)
language Inglés
topic Ciencias Exactas
Física
TDPAC
Different spin rotation spectra
nickel
spellingShingle Ciencias Exactas
Física
TDPAC
Different spin rotation spectra
nickel
Bibiloni, Aníbal Guillermo
Caracoche, María Cristina
López García, Alberto Raúl
Martínez, Jorge Alberto
Mendoza Zélis, Luis Alejandro
Mercader, Roberto Carlos
Pasquevich, Alberto Felipe
The magnetic hyperfine field at 140Ce in nickel
topic_facet Ciencias Exactas
Física
TDPAC
Different spin rotation spectra
nickel
description The hyperfine interaction of140Ce in nickel has been investigated by the time-differential perturbed-angular-correlation technique (TDPAC). The probe was produced by isotope separator implantation of the fission product140Xe, the β- decay chain of which finally populates excited states of140Ce. Different spin rotation spectra were observed before and after an 8 h annealing at 415°C. The analysis of the spectra led to the conclusion that the Ce ions were in the diamagnetic 4+ state. The dominant contributions to the hyperfine interaction are two different magnetic hyperfine fields: |H; hf; 1|=385±7 kOe and |H; hf; 2|=276±12 kOe.H; hf; 1 disappears after annealing. The fraction of nuclei which observeH; hf; 2 is increased by the annealing procedure from 16% to 75%. It is assumed thatH; hf; 1 is the hyperfine field of CeNi in an unperturbed substitutional site andH; hf; 2 is attributed to Ce ions which have trapped a single vacancy.
format Articulo
Articulo
author Bibiloni, Aníbal Guillermo
Caracoche, María Cristina
López García, Alberto Raúl
Martínez, Jorge Alberto
Mendoza Zélis, Luis Alejandro
Mercader, Roberto Carlos
Pasquevich, Alberto Felipe
author_facet Bibiloni, Aníbal Guillermo
Caracoche, María Cristina
López García, Alberto Raúl
Martínez, Jorge Alberto
Mendoza Zélis, Luis Alejandro
Mercader, Roberto Carlos
Pasquevich, Alberto Felipe
author_sort Bibiloni, Aníbal Guillermo
title The magnetic hyperfine field at 140Ce in nickel
title_short The magnetic hyperfine field at 140Ce in nickel
title_full The magnetic hyperfine field at 140Ce in nickel
title_fullStr The magnetic hyperfine field at 140Ce in nickel
title_full_unstemmed The magnetic hyperfine field at 140Ce in nickel
title_sort magnetic hyperfine field at 140ce in nickel
publishDate 1977
url http://sedici.unlp.edu.ar/handle/10915/133956
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