Introduction
Uranyl-sulfate minerals are widespread phases found in nearly all sandstone-hosted uranium–vanadium deposits in the southwestern United States, and worldwide. In Red Canyon, Utah, sulfates dominate the secondary uranyl mineralisation occurring on mine walls; in fact, many of the deposits in this region were first located by prospectors who noticed bright yellow and green encrustations on the uranium-bearing layers exposed at the surface. In the decades since mining ceased in Red Canyon, the remaining exposed (and unexposed) ore has undergone numerous periods of dissolution, crystallisation, and fluctuations in humidity and pH, which have led to an explosion in the diversity of uranyl species found underground.
Zincorietveldite, the new mineral described herein, is the 25th new mineral to be first described from the Blue Lizard mine in southeast Utah, USA, all within the last 10 years (see, for instance, Plášil et al., Reference Plášil, Kampf, Ma and Desor2023; Kampf et al., Reference Kampf, Plášil, Olds, Ma and Marty2023a). Zincorietveldite is named as the zinc analogue of rietveldite with Zn dominant in each of the two octahedrally coordinated cation sites. The new mineral and name (symbol Zrvd) were approved by the Commission on New Minerals, Nomenclature and Classification of the International Mineralogical Association (IMA2022-070, Kampf et al., Reference Kampf, Olds, Plášil and Marty2023b). The description is based on five cotype specimens, all micromounts, deposited in the collections of the Natural History Museum of Los Angeles County, 900 Exposition Boulevard, Los Angeles, CA 90007, USA, catalogue numbers 76262, 76264, 76265, 76266 and 76267. Specimen 76267 is also a cotype for libbyite (Kampf et al., Reference Kampf, Olds, Plášil, Nash and Marty2023c).
Occurrence
Zincorietveldite was found by two of the authors (ARK and JM) in efflorescent crusts on mine walls underground in the Blue Lizard mine (37°33'26"N, 110°17'44"W), Red Canyon, White Canyon District, San Juan County, Utah, USA. The mine is ~72 km west of the town of Blanding, Utah, and ~22 km southeast of Good Hope Bay on Lake Powell. Detailed historical and geological information on the Blue Lizard mine is described elsewhere (e.g. Kampf et al., Reference Kampf, Plášil, Kasatkin and Marty2015a), and is primarily derived from a report by Chenoweth (Reference Chenoweth1993). Abundant secondary uranium mineralisation in Red Canyon is associated with post-mining oxidation of asphaltite-rich sandstone beds laced with uraninite and sulfides in the damp underground environment. Zincorietveldite is a relatively rare mineral found in association with bobcookite, coquimbite, halotrichite, libbyite, metavoltine, rhomboclase, römerite, tamarugite, voltaite and other potentially new minerals on matrix comprised mostly of subhedral to euhedral, equant quartz crystals that are recrystallised counterparts of the original grains of the sandstone.
We have also confirmed the occurrence of zincorietveldite at the Widowmaker mine, on Fry Mesa, also in the White Canyon district; however, our description of the species is based solely on material from the Blue Lizard mine. The Widowmaker mine should not be considered a cotype locality.
Morphology, physical properties and optical properties
Zincorietveldite occurs as subparallel groups of yellow to orange–yellow blades up to ~1 mm in length (Fig. 1). Blades are elongate on [001], flattened on {010} and exhibit the forms {100}, {010}, {110}, {011}, {01$\bar{1}$}, {101}, {$\bar{1}$0$\bar{1}$}, {111} and {11$\bar{1}$} (Fig. 2). No twinning was observed, but merohedral twinning is likely because of the noncentrosymmetric space group. The streak is very pale yellow and the mineral is nonfluorescent. Crystals are transparent with a vitreous lustre. The tenacity is brittle and the fracture is curved. The Mohs hardness is ~2½ based on scratch tests. There are three cleavages: excellent on {010}, good on {100} and fair on {001}. Crystals sink very slowly in pure methylene iodide (3.32 g⋅cm–3). The mineral is soluble in Clerici solution, so the density could not be measured. The calculated density based upon the empirical formula is 3.376 g⋅cm–3. The mineral is easily soluble in room-temperature H2O. Zincorietveldite is optically biaxial (+) with α = 1.568(2), β = 1.577(2) and γ = 1.595(2) measured in white light. The 2V measured directly on a spindle stage is 70(1)°; the calculated 2V is 71.2°. Dispersion is strong, r > v. The optical orientation is X = b, Y = a and Z = c. The mineral is pleochroic with X = yellow, Y = colourless and Z = light yellow; Y < Z < X. The Gladstone–Dale compatibility (Mandarino, Reference Mandarino2007) 1 – (K p/K c) is –0.002 (superior) based on the empirical formula using k(UO3) = 0.118, as provided by Mandarino (Reference Mandarino1976).
Raman spectroscopy
Raman spectroscopy was done on a Horiba XploRA PLUS micro-Raman spectrometer using an incident wavelength of 532 nm, laser slit of 100 μm, 1800 gr/mm diffraction grating and a 100× (0.9 NA) objective. The spectrum, recorded from 4000 to 60 cm–1, is shown in Fig. 3.
The spectrum of zincorietveldite is very similar to that of rietveldite and the band assignments indicated in Fig. 3 are the same as those previously proposed for rietveldite (Kampf et al., Reference Kampf, Sejkora, Witzke, Plášil, Čejka, Nash and Marty2017). Using the empirically derived equation of Libowitzky (Reference Libowitzky1999), the sharp band at 3540 cm–1 is consistent with hydrogen bond O⋅⋅⋅O distances of ~2.96 Å. This value matches well with our proposed hydrogen bonding scheme for which 14 of the 18 O⋅⋅⋅O distances are in the range 2.92 to 3.00 Å (see Table 4). According to the empirical relationship of Bartlett and Cooney (Reference Bartlett and Cooney1989), the ν1 UO22+ band at 860 cm–1 corresponds to a U–OUr bond length of ~1.75 Å, in excellent agreement with U–OUr bond lengths from the X-ray data: 1.750(6) and 1.766(6) Å.
Chemical composition
Electron probe microanalyses (6 points) were done using a JEOL JXA-8230 electron microprobe operating in wavelength dispersive spectroscopy mode using Probe for EPMA software (https://www.probesoftware.com). Analytical conditions were 15 kV accelerating voltage, 1 nA beam current and a beam diameter of 10 μm. Because insufficient material is available for a direct determination of H2O, it has been calculated based upon the structure determination (S = 2 and O = 15 atoms per formula unit). The analytical results are given in Table 1.
* Based on structure
S.D. – standard deviation
The empirical formula (based on 15 O apfu) is (Zn0.675Mg0.102Fe0.085Mn0.043Co0.033)Σ0.938(U1.028O2)(SO4)2(H1.991O)5. Adjusting for full occupancy of the Zn and U sites, the empirical formula is (Zn0.720Mg0.109Fe0.091Mn0.046Co0.035)Σ1.00(UO2)(SO4)2(H2O)5. The simplified formula is (Zn,Mg,Fe,Mn,Co)(UO2)(SO4)2(H2O)5. The ideal formula is Zn(UO2)(SO4)2(H2O)5, which requires ZnO 13.18, UO3 46.31, SO3 25.93, H2O 14.58, total 100 wt.%.
X-ray crystallography
Powder X-ray diffraction (PXRD) data were recorded using a Rigaku R-Axis Rapid II curved imaging plate microdiffractometer with monochromatised MoKα radiation. A Gandolfi-like motion on the φ and ω axes was used to randomise the sample. Observed d values and intensities were derived by profile fitting using JADE Pro software (Materials Data, Inc.). The powder data are presented in Supplementary Table S1 (see below). The unit-cell parameters refined from the powder data using JADE Pro with whole pattern fitting are a = 12.871(3), b = 8.343(2), c = 11.314(2) Å and V = 1214.9(4) Å3.
The single-crystal structure data were collected at room temperature using the same diffractometer and radiation noted above. The Rigaku CrystalClear software package was used for processing the structure data, including the application of an empirical absorption correction using the multi-scan method with ABSCOR (Higashi, Reference Higashi2001). The structure was solved using the intrinsic-phasing algorithm of SHELXT (Sheldrick, Reference Sheldrick2015a). SHELXL-2016 (Sheldrick, Reference Sheldrick2015b) was used for the refinement of the structure. The structure solution located all non-hydrogen atoms, which were refined with anisotropic displacement parameters. The Zn1 and Zn2 sites were refined with joint occupancies by Zn and Mg yielding Zn0.875Mg0.125(14) and Zn0.856Mg0.144(13), respectively. These correspond to site scattering values of 55.500 and 54.816, respectively, for a total site scattering of 110.316. For comparison, the total site-scattering value corresponding to full site occupancies with the cation ratios indicated by the electron probe microanalyses is 109.476. The H atoms locations could not be found in the difference-Fourier maps. The two largest electron density residuals, 4.44 and 3.55 e –, located 0.89 and 0.87 Å from the U site, respectively, are presumed to be ripple effects. Data collection and refinement details are given in Table 2, atom coordinates and displacement parameters in Table 3, selected bond distances in Table 4 and a bond-valence analysis in Table 5. The crystallographic information file has been deposited with the Principal Editor of Mineralogical Magazine and is available as Supplementary material (see below).
R int = Σ|F o2–F o2(mean)|/Σ[F o2]. GoF = S = {Σ[w(F o2–F c2)2]/(n–p)}½. R 1 = Σ||F o|–|F c||/Σ|F o|. wR 2 = {Σ[w(F o2–F c2)2]/Σ[w(F o2)2]}½; w = 1/[σ2(F o2)+(aP)2+bP] where a is 0.0325, b is 0.5911 and P is [2F c2+Max(F o2,0)]/3.
* Refined occupancies: Zn1 = Zn0.875(14)Mg0.125(14); Zn2 = Zn0.856(13)Mg0.144(13)
U+6–O and S+6–O bond-valence parameters from Gagné and Hawthorne (Reference Gagné and Hawthorne2015). Hydrogen-bond strengths based on O–O bond lengths from Ferraris and Ivaldi (Reference Ferraris and Ivaldi1988). Negative values indicate donated hydrogen-bond contributions.
Description of the structure
Zincorietveldite is isostructural with rietveldite. The U site in the structure is surrounded by seven O atoms forming a squat UO7 pentagonal bipyramid. This is the most typical coordination for U6+, particularly in uranyl sulfates, where the two short apical bonds of the bipyramid constitute the uranyl group. Four of the five equatorial O atoms of the UO7 bipyramid participate in SO4 tetrahedra; the other is an H2O group. The linkages of pentagonal bipyramids and tetrahedra form an infinite [(UO2)(SO4)2(H2O)]2– chain along [001] (Fig. 4). The chains are linked in the [100] direction by Zn1O2(H2O)4 and Zn2O2(H2O)4 octahedra, which share O vertices with SO4 tetrahedra in the chains (Fig. 5). A heteropolyhedral sheet parallel to {010} is thereby formed. Adjacent sheets are linked only by hydrogen bonding (Fig. 4).
The [(UO2)(SO4)2(H2O)]2– chain in the structures of rietveldite and zincorietveldite is also found in the structures of bobcookite, Na(H2O)2Al(H2O)6[(UO2)2(SO4)4(H2O)2]⋅8H2O (Kampf et al. Reference Kampf, Plášil, Kasatkin and Marty2015a), oldsite, K2Fe[(UO2)(SO4)2]2⋅8H2O (Plášil et al., Reference Plášil, Kampf, Ma and Desor2023), oppenheimerite, Na2(H2O)2[(UO2)(SO4)2(H2O)] (Kampf et al. Reference Kampf, Plášil, Kasatkin, Marty and Čejka2015b), svornostite, K2Mg[(UO2)(SO4)2]2⋅8H2O (Plášil et al., Reference Plášil, Hloušek, Kasatkin, Novák, Čejka and Lapčák2015), synthetic K2[(UO2)(SO4)2(H2O)](H2O) (Ling et al., Reference Ling, Sigmon, Ward, Roback and Burns2010) and synthetic Mn(UO2)(SO4)2(H2O)5 (Tabachenko et al., Reference Tabachenko, Serezhkin, Serezhkina and Kovba1979). The chains in bobcookite and oppenheimerite are geometrical isomers of the chain in the structures of oldsite, rietveldite and zincorietveldite.
Studies of the synthetic phases of general formula M(UO2)(SO4)2(H2O)5, in which M = Mg, Mn, Fe, Co, Ni, Cu, Zn or Cd (Kornyakov et al., Reference Kornyakov, Tyumentseva, Krivovichev, Tananaev and Gurzhiy2021; Serezhkin and Serezhkina, Reference Serezhkin and Serezhkina1978; Soares Rocha, Reference Soares Rocha1960; Tabachenko et al., Reference Tabachenko, Serezhkin, Serezhkina and Kovba1979), show that these phases occur in two polytypes (Table 6). Rietveldite and zincorietveldite are isostructural with the synthetic phases with space group Pmn21 and have double the a cell parameter of the phases with space group P21.
Acknowledgements
Structures Editor Peter Leverett and an anonymous reviewer are thanked for their constructive comments on the manuscript. We are grateful to retired miner Dan Shumway of Blanding, Utah, for advice and assistance in our collecting efforts in Red Canyon. This study was funded, in part, by the John Jago Trelawney Endowment to the Mineral Sciences Department of the Natural History Museum of Los Angeles County. JP acknowledges the support of the Czech Science Foundation (GACR 20-11949S).
Supplementary material
The supplementary material for this article can be found at https://doi.org/10.1180/mgm.2023.14.
Competing interests
The authors declare none.