RUSSOITE, Nh4clas 2O3(H2O)0.5, a NEW PHYLLOARSENITE MINERAL from SOLFATARA DI POZZUOLI, NAPOLI, ITALY
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3+ RUSSOITE, NH4ClAs 2O3(H2O)0.5, A NEW PHYLLOARSENITE MINERAL FROM SOLFATARA DI POZZUOLI, NAPOLI, ITALY ITALO CAMPOSTRINI, FRANCESCO DEMARTIN, AND MARCO SCAVINI Università degli Studi di Milano, Dipartimento di Chimica, via Golgi 19, I-20133 Milano, Italy. E-mail: [email protected] [Received 8 August 2017; Accepted 23 November 2017; Associate Editor: Charles Geiger] ABSTRACT 3+ The new mineral russoite (IMA 2015-105), NH4ClAs 2O3(H2O)0.5, was found at the Solfatara di Pozzuoli, Pozzuoli, Napoli, Italy, as a fumarolic phase associated with alacranite, dimorphite, realgar, mascagnite, salammoniac and an amorphous arsenic sulfide. It occurs as hexagonal plates up to about 300 μm in diameter and 15 μm thick, in rosette-like intergrowths. On the basis of PXRD measurements and chemical analysis, the mineral was recognized to be identical to the corresponding synthetic phase NH4ClAs2O3(H2O)0.5. Crystals are transparent and colorless, with vitreous lustre and white streak. Tenacity is brittle and fracture is irregular. Cleavage is perfect on {001}. The measured density is 2.89(1) g/cm3, the calculated density is 2.911 g/cm3. The empirical formula, (based on 4.5 anions pfu) is [(NH4)0.94,K0.06]Σ1.00(Cl0.91,Br0.01)Σ0.92As2.02O3(H2O)0.5. Russoite is hexagonal, space group P622, with a = 5.2411(7), c = 12.5948(25) Å, V = 299.62(8) Å3 and Z = 2. The eight strongest X-ray powder diffraction lines are [dobs Å(I)(hkl)]: 12.63(19)(001), 6.32(100)(002), 4.547(75)(100), 4.218(47)(003), 3.094(45)(103), 2.627(46)(110), 2.428(31)(112) and 1.820(28)(115). The structure, was refined to R =0.0518 for 311 reflections with I >2(I) and shows a different location of the ammonium cation and water molecules with respect to that reported for the synthetic analogue. The This is a 'preproof' accepted article for Mineralogical Magazine. This version may be subject to change during the production process. DOI: 10.1180/minmag.2017.081.097. mineral belongs to a small group of phylloarsenite minerals (lucabindiite, torrecillasite, gajardoite). It contains electrically neutral As2O3 layers, topologically identical to those found in lucabindiite and gajardoite between which are ammonium cations and outside of which Cl- anions. Water molecules and additional ammonium cations are located in a layer between two levels of chloride anions. Keywords: russoite; new mineral; arsenite; lucabindiite; torrecillasite; gajardoite. INTRODUCTION The Solfatara di Pozzuoli is one of about 40 volcanoes in the Campi Flegrei area and is located three kilometers from the center of the town of Pozzuoli, Napoli, Italy. Solfatara formed during the third Flegrean eruptive period and dates to about 3700-3900 years ago. Inside the Solfatara some active fumaroles are present, the most important of which is called "Bocca Grande" and has a temperature of about 160 °C. During a research campaign carried out in 2011, a few samples of the new mineral 3+ russoite, NH4ClAs 2O3(H2O)0.5, were collected at the “Bocca Grande” fumarole, where this phase formed as a sublimate product. XRPD measurements and chemical analysis, showed the mineral to be identical to the corresponding synthetic phase NH4ClAs2O3(H2O)0.5 (Edstrand and Blomqvist, 1955). In lack of single crystal suitable for an accurate X-ray structure refinement on the natural product, the XRPD data and the analytical results, perfectly matching those of the synthetic phase, were considered to be sufficient for a positive identification of the new mineral species, which was approved by the IMA Commission on New Minerals, Nomenclature and Classification (IMA. 2015- 105). Its name was chosen to honour Dr. Massimo Russo (b. 1960, –), researcher at Osservatorio Vesuviano, Istituto Nazionale di Geofisica e Vulcanologia, Napoli. His work has been mainly devoted to the mineralogy of Italian volcanoes and he is author of several books and articles on this topic. Holotype material is deposited in the Reference Collection of the DCSSI, Università degli Studi di Milano, catalogue number 2015-01. The recent availability of new material allowed us to obtain more accurate single-crystal intensity data for structure refinement. These data showed a location of the ammonium cation and water molecule 2 different from that proposed by Edstrand and Blomqvist (1955). OCCURRENCE, CHEMICAL DATA AND PHYSICAL PROPERTIES The new mineral russoite was found as a fumarolic phase associated with alacranite, dimorphite, mascagnite, realgar, salammoniac and an amorphous arsenic sulfide. In the same fumarole other interesting and rare minerals are found: adranosite, adranosite-(Fe), efremovite, huizingite-(Al) and godovikovite. Russoite occurs as rosette-like intergrowths or subparallel aggregates formed by hexagonal plates flattened on {001} and bounded by {100} up to about 300 μm in diameter and 15 μm thick, (Figures 1-2). This aggregates sometimes are yellowish due to admixed amorphous arsenic sulfide. Crystals are colorless to white, transparent or translucent, with vitreous lustre and white streak. Tenacity is brittle and fracture is irregular. Cleavage is perfect on {001}. The mineral does not fluoresce in long- or short-wave ultraviolet light. No twinning is apparent. The density, measured by flotation in a diiodomethane/benzene solution is 2.89(1) g/cm3, that calculated using the empirical formula and unit-cell data is 2.911 g/cm3. Due to the minute size of the crystals the Mohs hardness could not be determined. Optically russoite is uniaxial (-) with = 1.810(6) and = 1.650(5) (measured in white light). The calculated mean refractive index using the Gladstone-Dale constants of Mandarino (1976, 1981) is 1.757, which is rated as good. The infrared spectrum of russoite (Figure 3) was recorded in a KBr disk, in the range 4000 – 400 cm-1, using a Jasco FTIR-470 Plus spectrometer. It is consistent with the presence of ammonium [bands at -1 -1 (cm ): 3254, 3; 3145, 22; 1403, 4], water [bands at (cm ): 3454, 3; 3398, 1; 1625, 2] and arsenite (bands at 604 and 670 cm-1) (Farmer, 1974; Busigny et al., 2003). The weak absorption at -1 -1 - about 2400 cm is due to atmospheric CO2, that at 1110 cm might be attributed to minor OH , partially replacing the chloride ion. 3 Quantitative chemical analyses (6) were carried out in EDS mode using a JEOL JSM 5500 LV scanning electron microscope equipped with an IXRF EDS 2000 microprobe (20 kV excitation voltage, 10 pA beam current, 2 μm beam diameter). This analytical method was chosen because crystal intergrowths did not take a good polish and was impossible to prepare a flat polished sample; moreover the crystals are severely damaged by using the WDS technique, even with a low voltage and current and a large diameter of the electron beam. In this case, as reported by Ruste (1979) and Acquafredda and Paglionico (2004), the EDS detector gives more accurate analyses of small volumes of investigated sample also with a probe current lower than 1 nA and this method gives good results also when collecting X-rays emitted from a non perfectly flat surface of the specimen. X-ray intensities were converted to wt% by ZAF quantitative analysis software. The standards employed were: synthetic InAs (As) halite (Cl), synthetic KBr (K, Br). Element concentrations were measured using the K lines for Cl, K, and the L line for As and Br. The mean analytical results are reported in Table 1. No amounts of other elements above 0.1 wt% were detected. Water and ammonium contents were not analyzed because the mineral is intimately mixed with mascagnite and realgar and is not possible to obtain a sufficient amount of pure sample suitable for this kind of analysis. The presence of N was also evident in the EDS spectrum made on selected crystals, however the uncertainties of the measurements were considered too large for a quantitative estimation of this element. Therefore the ammonium and water contents were deduced from the NH4ClAs2O3(H2O)0.5 stoichiometry, taking into account the K content, which partly replaces the ammonium ion (K + NH4 = 1 apfu). The empirical formula (based on 4.5 anions pfu) is: [(NH4)0.94,K0.06]Σ1.00(Cl0.91,Br0.01)Σ0.92As2.02O3(H2O)0.5. The simplified formula is NH4ClAs2O3(H2O)0.5. The X-ray powder-diffraction pattern (Table 2), obtained using a conventional Rigaku DMAX II diffractometer, with graphite monochromatized CuK radiation, is in good agreement with that calculated for the synthetic phase (PDF2 – entry 00-076-1366), whose structure was solved by Edstrand and Blomqvist (1955) on the basis of Weissenberg film measurements. Using the same indexing of the synthetic phase and the program UNITCELL (Holland and Redfern, 1997) the 4 following unit-cell parameters a = 5.259(2), c = 12.590(5) Å, V= 301.55(2) Å3 were refined for russoite. They are in good agreement with those reported for the synthetic phase a = 5.254, c = 12.574 Å. SINGLE-CRYSTAL STRUCTURE DETERMINATION A new sampling, carried out in April 2016, after the approval of russoite as a new mineral by the IMA CNMNC, gave the us opportunity to collect additional specimens with larger aggregates of crystals (up to 0.3 mm), from which fragments apparently suitable for single-crystal structure determination could have been obtained. Indeed, all these fragments are not perfect single crystals, as they are made by several small platelets almost stacked in a parallel way, but slightly misaligned. After many attempts, one fragment was found to be composed by two different individuals only, sufficiently misaligned to allow the collection of a complete set of reflections, suitable for a new structure refinement. The diffracted intensities, corresponding to a complete scan of the reciprocal lattice up to 2= 63.60°, were collected at room temperature using a Bruker Apex II diffractometer equipped with a 2K CCD detector and MoK radiation (λ = 0.71073 Å).