Microstructure and nanohardness of hafnium diboride after ion irradiations

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Abstract

In order to simulate helium and lithium appearance originating from the 10B (n,α)7Li reaction, that occurs under neutron irradiation in a PWR, hafnium diboride samples have been irradiated with He+ and Li+ ions at 350°C. As implanted and annealed materials have been characterised by TEM observations and nanohardness measurements. In spite of high concentration of implanted helium, no helium bubbles were found whereas the TEM images showed a contrast associated with tiny dislocation loops. Observation on samples annealed at 1600°C allowed a more detailed analysis of loops which exhibit an interstitial nature (resp. vacancy) for a {1 1 2̄ 0} or {1 0 1̄ 0} habit plane (resp. (0 0 0 1)). The organisation of these secondary defects leads to a strongly anisotropic deformation of grains which is thought to cause intergranular microcracking when conflictual stresses are met at grain boundaries.

Introduction

This study concerns materials for control-rod applications in 100% MOX pressurised water reactors (PWR). Hafnium diboride appears to be a promising candidate since it exhibits a high melting point (Tm=3380°C) [1]and a high neutron absorber efficiency, equivalent to that of boron carbide commonly used in the present PWR [2]. Furthermore the new absorber must be able to withhold the corrosion mechanisms of the PWR core environment, i.e. water, with LiOH and H3BO3 in solution, at 350°C and under 155 bars. It has been observed that metal-rich pellets of HfB2 + 10 vol% Hf fulfilled these requirements [3]. All these observations let us think that HfB2 based materials could be appropriate neutron absorbers.

Investigations on neutron irradiated boron carbide and borides of transition metals have been carried out at the Vallecitos Atomic Laboratory of the General Electric Company in the 1960s [4]. The first post-irradiation analysis showed that diborides had swelled less and released few helium compared to B4C. By X-ray diffraction, the authors also demonstrated that the crystalline structure in diborides had collapsed less than that of hexa- and dodecaborides. The better behaviour (helium release, lattice resistance,...) of diborides compared to the others under irradiation is explained by the fact that diborides crystallise in a compact structure with a high bonding strength.

Following these former investigations it seems reasonable to assume that, as it is observed in B4C, HfB2 swelling is the direct consequence of the He and Li appearance and the subsequent bubble formation, resulting from 10B(n,α)7Li reaction. To ascertain this assumption and to determine the specific role of each (n,α) reaction product in the HfB2 structural damaging, He+ and Li+ have been implanted separately on thin TEM samples for further microstructural observations. In addition, nanohardness tests have been carried out on the thin He implanted layer of the HfB2 samples.

Section snippets

Materials

Powders were supplied by CERAC Company. In order to obtain high density pellets (>95% of the theoretical density), HfB2 powder and a mixture of HfB2 + 10 vol.% Hf were hot-pressed at respectively, 2000°C and 1800°C. The MR-HfB2 (metal-rich samples: HfB2 + 10 vol.% Hf) were then annealed 24 h at 1200°C to homogenise the microstructure. Sintering and heat treatment conditions are given in Table 1. Chemical analysis of O and C by infra-red absorption spectrometry and of metallic impurities by

Sample preparation

Diamond impregnated tools were used to cut 250 μm thick slices from the pellets. Samples of 3 mm in diameter are then obtained by ultrasonic grinding.

TEM specimens were electropolished in a TENUPOL apparatus at −30°C under 70 V, in a solution made of 70 vol.% ethanol, 20 vol.% butoxyethanol and 10 vol.% perchloric acid. Conventional TEM observations are carried out at 200 keV in a CM 20 Philips electron microscope. Only the HfB2 matrix is observable in the MR-HfB2 samples since only this phase

As received states

Observations of S-HfB2 specimens before irradiation show featureless grains and triple junction (Fig. 3(a)). The HfB2 grains in MR-HfB2 display 15 nm intragranular voids heterogeneously distributed as well as large cavities associated with precipitates identified by PEELS and microdiffraction as HfO2 (Fig. 3(b)).

Low fluence

The He+-particle injection causes the appearance of numerous black dots (Fig. 4(a)) in the grains of S-HfB2. The apparent density of this secondary defect structure depending on the

Discussion and conclusion

In the early stage of this study, He bubbles were supposed to be responsible for the swelling of HfB2 observed on samples after neutron irradiation [4]. In fact, we referred to the observations on B4C, where He forms pressurised bubbles after He+ irradiation at 750°C [11]. However, no bubbles have been found before annealing, even in foils implanted up to 10 at.%. He bubbles only appear after annealing performed at a high temperature (from 1200°C) in comparison with the temperature of PWR core

Acknowledgements

To Yves Serruys (DTA/CEREM/DECM/SRMP – CEA-Saclay) for the He+ irradiations, to Sylvie Poissonnet (DTA/CEREM/DECM/SRMP – CEA-Saclay) for nanohardness measurements and to Odile Kaı̈tasov (CSNSM-CNRS – Paris XI) for the Li+ irradiations.

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