In situ resistivity measurements of RAFM base alloys at cryogenic temperatures: The effect of proton irradiation

dc.contributor.authorGómez-Ferrer, Begoña
dc.contributor.authorVila, Rafael
dc.contributor.authorJiménez-Rey, David
dc.contributor.authorOrtiz, Christophe
dc.contributor.authorMota, Fernando
dc.contributor.authorGarcía, Juan Manuel
dc.contributor.authorRodriguez, Antonio
dc.date.accessioned2024-02-07T17:08:03Z
dc.date.available2024-02-07T17:08:03Z
dc.date.issued2014
dc.description.abstractA four-probe technique for measurement of electrical resistance on low-temperature ion-irradiated metallic sheets is described. The design, temperature control system, preparation method of samples and the resistivity measurements are described in detail. The resistivity recovery (RR) curve has been measured on a Fe-5%Cr model alloy irradiated with 5 MeV protons. The procedure to obtain the RR derivative curve is outlined and experimental errors are identified and quantified. Special care has been taken to use a sample with very low impurity content and low dislocation density (1.2 × 10 8 cm-2). Thus, effects in recovery spectrum of the Fe-5%Cr alloy are only due to the presence of Cr and irradiation defects, which will be mainly Frenkel Pairs (FPs) given that the mean energy of the Primary Knock-on Atoms (PKA) is close to 0.35 keV. The results obtained for the Fe-5%Cr under 5 MeV proton irradiation are found to be in overall agreement with previous experimental measurements performed under electron irradiation although some differences appear probably due to the different spatial distribution of the created defects and the higher temperature resolution of annealing steps. The RR spectrum obtained reveals the appearance of the structure of stages I and II and also a partial suppression of the stage III peak with respect to previous results obtained after electron irradiation. The stage III suppression is explained as a superposition of vacancy recombination effects and short-range ordering (SRO) effects which are apparently dependent on the spatial distribution of defects created during irradiation. Moreover, recombination phenomena are observed beyond stage III up to 500 K.es_ES
dc.description.sponsorship- Comisión Europea a través del programa EFDA – MATREMEV WP (JCI-2009-05681) - TECHNOFUSION (S2009/ENE-1679)es_ES
dc.identifier.citationJournal of Nuclear Materials, Vol 447, Issue 1-3, p. 225-232 (2014)es_ES
dc.identifier.doihttp://dx.doi.org/10.1016/j.jnucmat.2014.01.016
dc.identifier.issn223115
dc.identifier.urihttps://hdl.handle.net/20.500.14855/2403
dc.language.isoenges_ES
dc.publisherELSEVIERes_ES
dc.rights.accessRightsembargoed accesses_ES
dc.subjectResistivityes_ES
dc.subjectRadiationes_ES
dc.subjectSteelses_ES
dc.subjectIon irradiationes_ES
dc.subjectModellinges_ES
dc.subjectIrones_ES
dc.subjectTechniquees_ES
dc.titleIn situ resistivity measurements of RAFM base alloys at cryogenic temperatures: The effect of proton irradiationes_ES
dc.typejournal articlees_ES

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