Synthesis and characterization of hollandite-type material intended for the specific containment of radioactive cesium

The hollandite Ba₁Cs_0.28Fe_0.82Al_1.46Ti_5.72O₁₆, which has been proposed for the cesium-specific conditioning, can be synthesized either by an alcoxyde or a dry route. In both cases, a two-step protocol is applied, i.e., a calcination at 1000 °C followed by a sintering at 1200 °C. After sintering, both synthetic processes lead to a tetragonal form. According to the X-ray diffraction (XRD) patterns collected at the barium and the cesium K absorption edges, the different positions of these two elements have been evidenced with a more centered position in the oxygen cubic site of the tunnel for Ba than for Cs. On the contrary, after calcination, the two synthetic routes yield different products. The alcoxyde route gives rise to a mixture of the aforementioned Cs- and Ba-containing tetragonal I4/m hollandite, a Cs-only-containing monoclinic I2/m hollandite and an unidentified phase with a weak coherence length containing only Ba. The dry route yields a single tetragonal hollandite material containing Ba and Cs slightly different in composition from the targeted compound.     

Phase relations in NaxCrxTi8−xO16 at 1350 °C and crystal structure of hollandite-like Na2Cr2Ti6O16

Phase relations of rutile, freudenbergite, and hollandite structures were examined in the pseudobinary system NaCrO₂-TiO₂ (i.e., Na_xCr_xTi_8−xO₁₆) at 1350 °C. The hollandite structure was obtained in the composition range 1.7?x?2.0. The symmetry of the samples at room temperature was tetragonal for x=1.7 and 1.75, and monoclinic for x=1.8 and above. Single crystals of monoclinic hollandite Na₂Cr₂Ti₆O₁₆ were grown and the structure refinement has been carried out using an X-ray diffraction technique. The space group was I2/m and cell parameters were a=10.2385(11), b=2.9559(9), c=9.9097(11)Å, and β=90.545(9)° with Z=1. The Na ion distribution in the tunnel was markedly deformed from that in the tetragonal form. It was suggested that Cr/Ti ratios were different between the two framework metal sites.     

A universally applicable composite modulated structure approach to ordered BaxMyTi8−yO16 hollandite-type solid solutions

A wide range of barium titanate hollandites of the form (M=Zn, Co, Mg, Fe and Mn) and (M=Fe) with nominal x ranging from 1.0 to 1.4 have been synthesized and examined to investigate the solid solution range and the nature of the ordering of the Ba ions. Electron diffraction studies confirm that the barium titanate hollandites are composite modulated single phase solid solutions made up of mutually incommensurable (along b) framework and Ba ion sub-structures. The overall superspace group symmetry was found to be I′2/m(0,,0)1. The symbol I′ here refers to the superspace centering operation (see below). Both the framework and the Ba sub-structures have the same I2/m average structure space group symmetry. The solid solution ranges for the hollandites were calculated from the positions of well-defined superlattice peaks in X-ray diffraction patterns. The effect of cooling rate on Ba ion ordering is also examined.     

Investigation of Fe-based oxyhydroxy-fluoride with hollandite-type structure

Well crystallized Fe-based oxyhydroxy-fluoride with the FeO(OH_0.2F_0.8)·0.2H₂O chemical composition has been prepared from hydrolysis of Fe trifluoride under supercritical CO₂ conditions. Investigation by Mössbauer spectroscopy and neutron diffraction show that this compound crystallize in the monoclinic symmetry (SG: I2/m, a = 10.447(7) Å, b = 3.028(2) Å, c = 10.445(4) Å, β = 90.00(3)°). Taking into account the Fe-O(F) bond distances, F⁻ anions are mainly located on the common vertices of Fe octahedra whereas OH⁻ groups occupy mainly the shared edges of the Fe octahedra. Two various highly distorted octahedral sites have been identified with Fe-O/F bond distances varying from 1.90 Å to 2.31 Å. One Fe site is more distorted than in FeO_0.8OH_1.2·0.2Cl akaganeite because of the random distribution of F⁻/OH⁻/O²⁻ in the vicinity of this Fe cation.     

Titanate-based ceramics for separated long-lived radionuclides

Studies have been conducted in France to minimize the potential long-term impact of nuclear waste by enhanced chemical separation of the minor actinides (Np, Am, Cm) and some long-lived fission products (I, Cs, Tc). Two options may be considered following this work: (i) the initial reference option is transmutation by neutron bombardment in nuclear facilities, (ii) the second option would be to incorporate the separated elements into an inorganic matrix ensuring long-term stability. In the case of specific conditioning, zirconolite and hollandite are the potential host phases for the minor actinides and caesium, respectively. Both of these matrices have shown strong potential: (i) for incorporating the respective radioelement in the crystalline structure, (ii) for fabricating the ceramic by natural sintering in air, (iii) for chemical durability with a very low initial alteration rate (about 10^–2 g m^–2 d^–1 at 100 °C), then very rapidly reach alteration rates more than four orders of magnitude lower. In the case of zirconolite ceramics, the high chemical durability is conserved even after amorphization of the crystalline structure by external irradiation with heavy ions or by self-irradiation in natural zirconolites 550 million years old. To cite this article: C. Fillet et al., C. R. Chimie 7 (2004).

Résumé

Pour réduire l'impact potentiel à long terme des déchets nucléaires, des études sont conduites en France sur la séparation chimique poussée des actinides mineurs (Np, Am, Cm) et de certains produits de fission à vie longue (I, Cs, Tc). À l'issue de cette étape, deux options sont envisageables : (i) la transmutation par bombardement neutronique dans des systèmes nucléaires est la première option de référence, (ii) la seconde option consisterait à incorporer les éléments séparés des autres déchets nucléaires dans une matrice minérale stable à long terme. Dans le cadre d'un conditionnement spécifique, la zirconolite et la hollandite sont des phases hôtes potentielles respectivement pour les actinides mineurs et le césium. Ces deux matrices ont montré une potentialité élevée (i) d'incorporation du radioélément considéré dans la structure cristalline, (ii) d'élaboration de la céramique par des procédés de frittage naturel sous air, (iii) de durabilité chimique, avec une vitesse initiale d'altération très faible (de l'ordre de 10^–2 g m^–2 j^–1 à 100 °C), puis très rapidement des diminutions des vitesses d'altération de plus de quatre ordres de grandeur. Pour la céramique zirconolite, cette propriété de durabilité chimique élevée reste conservée, même après amorphisation de la structure cristalline par irradiation externe aux ions lourds ou par auto-irradiation sur des zirconolite naturelles âgées de 550 millions d'années. Pour citer cet article : C. Fillet et al., C. R. Chimie 7 (2004).     

Superstructure of hollandite KxMg(8+x)/3Sb(16−x)/3O16 (x≈1.76)

Single crystals of K_xMg_(8+x)/3Sb_(16−x)/3O₁₆ (x≈1.76) with a hollandite superstructure were grown. Ordering schemes for guest ions (K) and the host structure were confirmed by the structure refinement using X-ray diffraction intensities. The space group is I4/m and cell parameters are a=10.3256(6), c=9.2526(17)Å with Z=3. Superlattice formation is primarily attributed to the Mg/Sb occupational modulation in the host structure. Mg/Sb ratios at two nonequivalent metal sites are 0.8977/0.1023 and 0.1612/0.8388. Two types of the cavity are seen in the tunnel, where parts of K ions deviate from the cavity center along the tunnel direction. Probability densities for K ions in the two cavities are different from each other, which seems to have arisen from the Mg/Sb modulation.     

A new ordered triple Hollandite: Ba1.33Sb2.66Al5.33O16

Ba_1.33Sb_2.66Al_5.33O₁₆ is a triple Hollandite, which crystallizes in a tetragonal cell (I4/m no. 87) with a=b=9.86090(5) Å and c=8.77612(6) Å. Its crystal structure was characterized using electron diffraction and X-ray powder diffraction; it is isotypic to K_1.33Mg_3.11Sb_4.89O₁₆, K_1.76Mg_3.25Sb_4.75O₁₆ and to K_1.8Li_2.45Sb_5.55O₁₆. In the rutile chains of Ba_1.33Sb_2.66Al_5.33O₁₆, the ordering of Al and Sb atoms into unmixed sites induces the tripling of the c parameter compared to a ‘single’ Hollandite structure. The Ba²⁺ cations are dispersed along c, in the largest tunnels on non-split and fully occupied sites. They lie into Ba-Ba pairs separated by vacancies. Their regular arrangement has been confirmed by high resolution electron microscopy. Electrochemical experiments have also been performed in Li-ion cell but no Li insertion was detected.     

Local structures and transport properties of K ions in a hollandite superstructure KxMg(8 + x)/3Sb(16 − x)/3O16

Possible local structures of K ions in the tunnel of a hollandite superstructure K_xMg_(8 + x)/3Sb_{(16 − x)/3}O₁₆ (x ≈ 1.76) were presented, and the validity of the models was confirmed by the structure refinement using single-crystal X-ray diffraction data. Additional constraint conditions were introduced in refinements so that the average structure obtained from the refinement is consistent with assumed microscopic pictures. Joint-probability density functions were calculated for specific K ions concerning the hopping process between neighboring cavities, and converted to the one-particle potentials. Three types of the energy barrier for the hopping process were seen, which were uniformly reduced applying the anharmonic atomic displacement parameters.