Published 2008 | Version v1
Miscellaneous

Vacancy defects in UO2 and their thermal evolution

  • 1. Centre d'Etudes et de Recherches par Irradiation, 3A rue de la Ferollerie 45071 Orleans (France)
  • 2. Laboratoire des Solides Irradies, Ecole polytechnique, 91128, Palaiseau (France)
  • 3. CEA, CE de Cadarache, DEN/DEC/SESC/LLCC Bat 151, 13108 Saint Paul Lez Durance (France)

Description

Full text of publication follows: The understanding of the behaviour of fission nuclear fuel under irradiation is of first importance to foresee the state of the fuel in reactors and also if it is used as a nuclear waste storage matrix. Uranium dioxide is a major component of nuclear fission fuel and is used as a model material to study the behaviour of the nuclear fuel. The behaviour of UO2 under irradiation has been extensively studied by using different techniques such as Channeling Rutherford Backscattering, RX diffraction and so on (see reference [1] for a review), but only very few studies have been focused on the direct observation of point defects and the determination of their properties. Positron annihilation spectroscopy is a useful and powerful method to study the vacancy defects. In this work, we have used positron annihilation lifetime spectrometry (PALS) to characterize the vacancy defects induced by irradiation in UO2 and to determine their thermal properties. Vacancy defects induced in UO2 disks by irradiation with electrons and alpha particles have been characterized by using 22Na based positron lifetime spectroscopy (PALS). Several UO2 disks have been irradiated in different conditions: with electrons at two energies, 1 MeV and 2.5 MeV, with alpha particles at 45 MeV. These results indicate that the vacancy defects detected are formed only when displacement in the U sub-lattice occurs. The annihilation characteristics have been measured in the irradiated UO2 disks after annealing at temperature in the range from 400 to 1300 deg. C during 1 hour in Ar/H2 atmosphere. Their evolution shows that the vacancy defects distribution evolves with temperature. One annealing stage appears at about 800 deg. C. We will discuss the phenomena that could explain these annealing stage. [1] Hj. Matzke, Radiat. Eff. 64, 3 (1982); Nucl. Instr. Meth. B 32, 455 (1988). [2] W.J. Weber, Journal Nucl. Mater. 114 (1983) 213. (authors)

Availability note (English)

Available in abstract form only, full text entered in this record

Additional details

Publishing Information

Imprint Pagination
1 p.
Report number
INIS-FR--09-0005

Conference

Title
Atalante 2008 - Nuclear fuel cycle for a sustainable future
Dates
19-23 May 2008
Place
Montpellier (France)

INIS

Country of Publication
France
Country of Input or Organization
France
INIS RN
40012473
Subject category
S36: MATERIALS SCIENCE;
Resource subtype / Literary indicator
Conference, Non-conventional Literature
Descriptors DEI
PHYSICAL RADIATION EFFECTS; POINT DEFECTS; TEMPERATURE DEPENDENCE; TEMPERATURE RANGE 0400-1000 K; TEMPERATURE RANGE 1000-4000 K; URANIUM DIOXIDE
Descriptors DEC
ACTINIDE COMPOUNDS; CHALCOGENIDES; CRYSTAL DEFECTS; CRYSTAL STRUCTURE; OXIDES; OXYGEN COMPOUNDS; RADIATION EFFECTS; TEMPERATURE RANGE; URANIUM COMPOUNDS; URANIUM OXIDES

Optional Information

Notes
2 refs.