Redox Response of Actinide Materials to Highly Ionizing Radiation

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Redox Response of Actinide Materials to Highly Ionizing Radiation ARTICLE Received 9 Jul 2014 | Accepted 18 Dec 2014 | Published 27 Jan 2015 DOI: 10.1038/ncomms7133 Redox response of actinide materials to highly ionizing radiation Cameron L. Tracy1, Maik Lang2, John M. Pray3, Fuxiang Zhang3, Dmitry Popov4, Changyong Park4, Christina Trautmann5,6, Markus Bender5, Daniel Severin5, Vladimir A. Skuratov7 & Rodney C. Ewing8 Energetic radiation can cause dramatic changes in the physical and chemical properties of actinide materials, degrading their performance in fission-based energy systems. As advanced nuclear fuels and wasteforms are developed, fundamental understanding of the processes controlling radiation damage accumulation is necessary. Here we report oxidation state reduction of actinide and analogue elements caused by high-energy, heavy ion irradiation and demonstrate coupling of this redox behaviour with structural modifications. ThO2, in which thorium is stable only in a tetravalent state, exhibits damage accumulation 3 þ 4 þ processes distinct from those of multivalent cation compounds CeO2 (Ce and Ce ) and 4 þ 5 þ 6 þ UO3 (U ,U and U ). The radiation tolerance of these materials depends on the efficiency of this redox reaction, such that damage can be inhibited by altering grain size and cation valence variability. Thus, the redox behaviour of actinide materials is important for the design of nuclear fuels and the prediction of their performance. 1 Department of Materials Science and Engineering, University of Michigan, Ann Arbor, Michigan 48109, USA. 2 Department of Nuclear Engineering, University of Tennessee, Knoxville, Tennessee 37996, USA. 3 Department of Earth and Environmental Sciences, University of Michigan, Ann Arbor, Michigan 48109, USA. 4 High Pressure Collaborative Access Team (HPCAT), Geophysical Laboratory, Carnegie Institution of Washington, Argonne, Illinois 60439, USA. 5 GSI Helmholtzzentrum fu¨r Schwerionenforschung, 64291 Darmstadt, Germany. 6 Technische Universita¨t Darmstadt, 64287 Darmstadt, Germany. 7 Flerov Laboratory of Nuclear Reactions, Joint Institute for Nuclear Research, 141980 Dubna, Russia. 8 Department of Geological and Environmental Sciences, Stanford University, Stanford, California 94305, USA. Correspondence and requests for materials should be addressed to R.C.E. (email: [email protected]). NATURE COMMUNICATIONS | 6:6133 | DOI: 10.1038/ncomms7133 | www.nature.com/naturecommunications 1 & 2015 Macmillan Publishers Limited. All rights reserved. ARTICLE NATURE COMMUNICATIONS | DOI: 10.1038/ncomms7133 nsulating materials exhibit diverse responses to radiation, partially delocalized 5f orbitals cause significant variation in the ranging from isolated point defect formation and disordering accessible stable electronic configurations across this series21. Ito phase transformations and amorphization1. Substantial Motivated by the potential influence of their complex effort has been devoted to understanding the influence of crystal chemistry on the radiation response of actinide materials, we structure and chemistry on radiation damage accumulation2,3. have systematically irradiated f-block oxides with 167 MeV 132Xe The radiation tolerance of actinide materials, which refers to their ions, similar in mass and energy to fission fragments, and ability to retain their atomic structures and properties during 950 MeV 197Au ions. Fission rates are highest, and fission irradiation, is of primary concern for the design of nuclear fuels fragment damage most prevalent, in the relatively cool rim region with long operating lifetimes and adequate performance in of nuclear fuel pellets, where temperatures are typically between reactor accident scenarios4. A variety of criteria have been 500 and 700 °C, and thermal activation is generally negligible22. proposed as predictors of radiation tolerance, including bond Thus, these irradiations were performed at room temperature to covalency5, susceptibility to disordering2, thermodynamic avoid radiation-induced heating of the materials above fuel pellet stability6 and grain size7. However, relating trends in radiation rim temperatures. Complementary synchrotron-based structural tolerance to the dynamic process of radiation damage and chemical probes, X-ray diffraction (XRD) and X-ray accumulation is difficult due to the complex nature of defect absorption spectroscopy (XAS) were used to characterize the production and recovery, both of which occur at nanometric resulting atomic-scale modifications. Thorium and cerium are length scales, femto- and picosecond timescales, and extremely both nominally one f-electron elements and possess dioxides high energy densities8. In addition, the conditions under which a isostructural with those of the light actinides, all of which material is irradiated can drastically affect its response. High exhibit the fluorite structure, yet they possess contrasting solid- temperatures, as encountered in the centre of nuclear fuel pellets, state chemistry. ThO2, a proposed nuclear fuel component used can alter the kinetics of radiation-induced defect production, such for the breeding of uranium, cannot be reduced, while the cerium that materials that are tolerant of radiation in one temperature in the actinide analogue CeO2 is easily reduced from the regime can be less so in others9. Moreover, materials tolerant of tetravalent state to the trivalent state, similar to the behaviour low-energy radiation, which produces damage through atomic of UO2 and PuO2. Finally, UO3 and its room-temperature displacement caused by elastic collisions with nuclei, are not hydration products, (UO2)(OH)2 (a-uranyl hydroxide) and necessarily resistant to high-energy radiation, which deposits (UO2)8O2(OH)12(H2O)10 (metaschoepite), feature hexavalent energy in a material primarily through the excitation of uranium that can be reduced multiple steps to the tetravalent electrons10,11. The effects of highly ionizing radiation are oxidation state23. They are common oxidation/hydrolysis generally less well understood than those of displacive products of the nuclear fuel UO2 and are produced by fuel– radiation, but fission fragments, which fall into this high-energy coolant interactions and groundwater exposure of fuel4. regime, are known to significantly degrade the performance of The results of these experiments show evidence of coupling nuclear fuels12. To better understand the physics of damage between radiation-induced redox behaviour and structural production by ionizing radiation, a comprehensive approach, in modifications, with materials that undergo cation valence state which structural modifications are considered alongside coupled changes exhibiting damage accumulation behaviour different electron delocalization and redox processes, is necessary. than those that are resistant to such chemical modification. In We have investigated the effects of highly ionizing radiation on redox-active materials, control of the efficiency of these radiation- actinide materials using heavy ions accelerated to velocities induced redox processes through, for example, grain-size ranging from 5% to 10% the speed of light. At specific energies modification can be used to tailor the susceptibility of a material above B1 MeV per nucleon, these swift heavy ions simulate the to radiation damage. These results are particularly important for effects of the energetic nuclear fragments that form during fission actinide oxides as, due to the partially itinerant nature of their 5f events and the a-particles released in radionuclide decay, both of electrons, they exhibit increasing variability in stable electronic which deposit energy in irradiated materials primarily by configurations across the actinide series (as the 5f orbitals are electronic excitation13. Damage resulting from elastic collisions filled). This results in systematic variation in their radiation is generally minor until the particle end-of-range region, and the tolerance, as demonstrated here via a comparative study of such resulting defects are often distinct from those caused by the materials. These results yield new insight into the mechanisms by electronic interactions14. Electronic stopping results in extensive which highly ionizing radiation produces damage in nuclear fuel local ionization, yielding excitation densities of up to several materials and demonstrate potential for the design of radiation- keV nm À 3 within a nanometric cylinder along the ion tolerant materials through control of their redox behaviour. trajectory15. Although the atomistic modifications that occur following this electron cascade have been extensively studied8,13, the relaxation of these delocalized electrons is complex and Results 16 difficult to relate directly to atomic behaviour . It is generally Defect accumulation in ThO2. Irradiation of ThO2 with swift assumed that electron-hole recombination leads to recovery of the heavy ions induces only minor structural modifications pre-irradiation charge distribution13 but, given the highly non- (Fig. 1a,b), as discussed in detail elsewhere24. XRD patterns equilibrium conditions under which relaxation of the electron corresponding to both irradiation energies display a shift in the cascade occurs, electronic structure modifications are possible. Of fluorite structure diffraction maxima to lower 2y angles, particular interest is the influence of complex f-electron chemistry signifying an increase in the unit cell parameter and broadening on a material’s radiation response, considering previous work17,18 of the peaks due to the accumulation of heterogeneous reporting the reduction
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