Spiridonovite, (Cu_1-xAg_x)₂Te (x ≈ 0.4), a New Telluride from the Good Hope Mine, Vulcan, Colorado (U.S.A.)

Abstract

Here we describe a new mineral in the Cu-Ag-Te system, spiridonovite. The specimen was discovered in a fragment from the cameronite [ideally, Cu_5-x(Cu,Ag)_3+xTe₁₀] holotype material from the Good Hope mine, Vulcan, Colorado (U.S.A.). It occurs as black grains of subhedral to anhedral morphology, with a maximum size up to 65 μm, and shows black streaks. No cleavage is observed and the Vickers hardness (VHN₁₀₀) is 158 kg·mm⁻². Reflectance percentages in air for R_min and R_max are 38.1, 38.9 (471.1 nm), 36.5, 37.3 (548.3 nm), 35.8, 36.5 (586.6 nm), 34.7, 35.4 (652.3 nm). Spiridonovite has formula (Cu_1.24Ag_0.75)_Σ1.99Te_1.01, ideally (Cu_1-xAg_x)₂Te (x ≈ 0.4). The mineral is trigonal and belongs to the space group P-3c1, with the following unit-cell parameters: a = 4.630(2) Å, c = 22.551(9) Å, V = 418.7(4) Å ³, and Z = 6. The crystal structure has been solved and refined to R1 = 0.0256. It can be described as a rhombohedrally-compressed antifluorite structure, with a rough ccp arrangement of Te atoms. It consists of two Te sites and three M (metal) sites, occupied by Cu and Ag, and is characterized by the presence of edge-sharing tetrahedra, where the four-fold coordinated M atoms lie. The mineral and its name have been approved by the Commission of New Minerals, Nomenclature and Classification of the International Mineralogical Association (No. 2018-136).

1. Introduction

Spiridonovite is a new member of the Cu-Ag-Te system, together with rickardite [1], (Cu_3-xTe₂), vulcanite (CuTe) [2], weissite (Cu_2-xTe) [3], cameronite [Cu_5-x(Cu,Ag)_3+xTe₁₀] [4], and henryite [(Cu,Ag)_3+xTe₂] [5]. The new mineral species was discovered in a fragment from the cameronite holotype material, sample R-934, from the Good Hope mine (38° 20’ 35’’ N, 107° 0’ 26’’ W), Vulcan, Colorado (U.S.A.) obtained in 1974 by the late William W. Pinch on exchange from the Smithsonian Institution, Washington D.C. (U.S.A.) [4].

The Good Hope mine was active from 1898 to 1904, and intermittently through 1930. The mineralization is hosted in mafic intrusive rock, schist and felsic volcanic rock [6]. Precious metals and tellurides are localized in quartz veins and successive supergene alteration of tellurides (altaite, galena, and goldfieldite) formed native Te and Cu-tellurides (e.g., rickardite, vulcanite, weissite), like spiridonovite.

The new mineral has been named after Ernst M. Spiridonov (b. 1938), Professor at the Department of Mineralogy, Moscow State University, Russia. He studied gold deposits of the Urals, Transbaikalia, Kamchatka, Uzbekistan, Armenia, and Bulgaria in the last fifty years and discovered 20 new mineral species, most of them ore minerals. The new mineral and mineral name have been approved by the Commission on New Minerals, Nomenclature and Classification of the International Mineralogical Association (No. 2018-136). The holotype material is deposited in the collections of the Museo di Storia Naturale, Università degli Studi di Firenze, Via La Pira 4, I-50121, Firenze, Italy, catalogue number 3295/I.

2. Description and Physical Properties

Spiridonovite occurs as very rare crystals closely associated to rickardite, vulcanite, cameronite and native tellurium (Figure 1); its maximum grain size is about 65 μm. The mineral shows a subhedral to anhedral grain morphology without inclusions or intergrowths with other minerals.

Spiridonovite crystals are black, show metallic luster and black streak, and are not fluorescent. Mohs hardness, estimated from the Vickers measurements, is ~3. Micro-indentation measurements, carried out with a CORE micro-indentation system, give a mean value of 158 kg·mm⁻² (range 145–170). Tenacity is brittle, and cleavage is not observed. Parting is not observed, and fractures are irregular. The density could not be determined due to the small grain size. The calculated density is 4.6 g·cm⁻³, using the empirical formula and X-ray single-crystal data (see below).

In plane-polarize incident light, the mineral is dark bluish black, with moderate bireflectance (slightly higher than cameronite) and very weak pleochroism from light grey to a slightly greenish grey. Under crossed polars, spiridonovite shows very weak anisotropism with greyish to light-blue rotation tint. Internal reflections are absent, and there is no optical evidence of growth zonation. Reflectance values were measured in air using a MPM-200 Zeiss microphotometer equipped with a MSP-20 system processor on a Zeiss Axioplan ore microscope (Zeiss, Jena, Germany). The filament temperature was approximately 3350 K. An interference filter was adjusted, in turn, to select four wavelengths for measurement (471.1, 548.3, 586.6, and 652.3 nm). Readings were taken for specimen and standard (SiC) maintained under the same focus conditions. The diameter of the circular measuring area was 0.05 mm. Reflectance values are reported in

Table 1. Reflectance values for spiridonovite.

Rmax	Rmin	λ (nm)
38.9	38.1	471.1
37.3	36.5	548.3
36.5	35.8	586.6
35.4	34.7	652.3

.

3. Chemical Data

A preliminary chemical analysis using EDS performed on the crystal fragment used for the structural study did not indicate the presence of elements (Z > 9) other than Cu, Ag and Te. However, given the minor elements found in cameronite [4], we analyzed also Bi, Pb, Zn, Fe, Sb, As, S, Se at the electron microprobe. Analyses (n = 5) were carried out using a JEOL 8200 microprobe (WDS mode, 25 kV, 20 nA, 1 μm beam size, counting times 20 s for peak and 10 s for background. JEOL, Tokyo, Japan). For the WDS analyzes the following lines were used: SKα, FeKα, CuKα, ZnKα, AsLα, SeLα, AgLα, SbLβ, TeLα, PbMα, BiMβ. The crystal fragment was found to be homogeneous within analytical error. Analytical data are given in

Table 2. Analytical data in wt.% for spiridonovite.

Constituent	Mean	Range	Stand. dev. (σ)	Standard
Ag	27.83	25.88–28.09	0.19	Ag metal
Cu	27.12	26.02–27.94	0.16	Cu metal
Bi	0.01	0.00–0.03	0.03	synthetic Bi2S3
Pb	0.02	0.00–0.03	0.02	galena
Zn	0.01	0.00–0.02	0.02	synthetic ZnS
Fe	0.02	0.00–0.04	0.04	pyrite
Sb	0.01	0.00–0.02	0.02	synthetic Sb2Te3
As	0.02	0.00–0.03	0.03	synthetic As2S3
S	0.01	0.00–0.02	0.02	pyrite
Se	0.02	0.00–0.04	0.03	synthetic PtSe2
Te	44.35	42.63–45.81	0.29	synthetic Sb2Te3
Total	99.42	99.15–100.55

.

The empirical formula based on 3 atoms per formula unit is (Cu_1.24Ag_0.75)_Σ1.99Te_1.01, which is in excellent agreement with that derived from the structure refinement, i.e. (Cu_1.19Ag_0.81)_Σ2.00Te. The simplified formula is (Cu,Ag)₂Te. The ideal formula is (Cu_1-xAg_x)₂Te (x ≈ 0.4). (Cu_0.6Ag_0.4)₂Te requires Cu 26.28, Ag 29.74, Te 43.98, Total 100. Silver is an essential constituent in spiridonovite with the intrinsic role to stabilize the crystal structure.

4. X-ray Crystallography

X-ray powder diffraction data (

Table 3. Analytical data in wt.% for spiridonovite. 1 = observed diffraction pattern; 2 = calculated diffraction pattern obtained with the atom coordinates and occupancies reported in Table 5 (only reflections with I_rel ≥ 4 are listed).

			1		2
h	k	l	dobs	Iest	dcalc	Icalc
0	1	2	3.78	60	3.778	67
0	0	6	3.76	20	3.759	23
1	0	4	-	-	3.268	8
1	1	0	2.317	100	2.3150	100
0	1	8	2.305	85	2.3060	99
2	0	2	-	-	1.9739	10
1	1	6	1.973	15	1.9711	21
1	0	10	-	-	1.9656	9
2	0	8	1.635	30	1.6338	30
1	2	2	-	-	1.5020	8
0	1	14	-	-	1.4947	4
3	0	0	1.338	10	1.3366	14
1	2	8	1.333	25	1.3348	27
1	0	16	1.328	10	1.3297	13
2	2	0	-	-	1.1575	8
0	2	16	-	-	1.1530	8
3	1	8	1.033	5	1.0345	11
2	1	16	-	-	1.0321	11
0	4	8	-	-	0.9445	5
1	3	16	-	-	0.8730	9
1	1	24	-	-	0.8706	10

) were collected on a fragment handpicked from the polished section with an Oxford Diffraction Excalibur PX Ultra diffractometer fitted with a 165 mm diagonal Onyx CCD detector and using copper radiation (CuKα, λ = 1.54138 Å).

Single-crystal X-ray studies were carried out using an Oxford Diffraction Xcalibur diffractometer equipped with an Oxford Diffraction CCD detector, with graphite-monochromatized MoKα radiation (λ = 0.71073 Å). Crystal data and details of the intensity data collection and refinement are reported in

Table 4. Crystal and experimental data for spiridonovite.

Crystal size (mm)	0.040 × 0.050 × 0.060
Cell setting	Trigonal
Space group	P-3c1 (#165)
a, c (Å)	4.630(2), 22.550(10)
V (Å3)	418.7(4)
Z	6
Temperature (K)	293(2)
2θmax (°)	64.30
Measured reflections	2155
Unique reflections	435
Reflections with Fo > 4σ(Fo)	103
Rint	0.0312
Rσ	0.0270
Range of h, k, l	−5–5; −6–6; −32–32
R1 [Fo > 4σ(Fo)]	0.0256
R1 (all data)	0.0304
wR (on F2)	0.0696
GooF	0.991
No. least-squares parameters	18
Max. and min. resid. peak (e Å−3)	0.38; −0.24

.

Single-crystal X-ray diffraction intensity data were integrated and corrected for standard Lorentz polarization factors with the CrysAlis^Pro package (Oxford Diffraction, Oxford, UK [7]). The program ABSPACK in CrysAlis RED [8] was used for the absorption correction. A total of 435 unique reflections were collected. Systematic absences were consistent with the space groups P-3c1 and P3c1. The statistical tests on the distribution of |E| values (|E²-1| = 0.977) indicated the presence of an inversion center and so the P-3c1 space group was chosen. The structure was solved and refined using the program Shelx-97 [9]. The site occupation factor (s.o.f.) at the cation sites was allowed to vary (Cu vs. Ag for the M positions and Te vs. structural vacancy for the anionic positions) using scattering curves for neutral atoms taken from the International Tables for X-ray Crystallography [10]. The Te sites were found fully occupied by tellurium and then fixed in the subsequent refinement cycles. Final atomic coordinates and equivalent isotropic displacement parameters are given in

Table 5. Atoms, site-occupancy factors (s.o.f.), Wyckoff positions, atom coordinates and isotropic displacement parameters (Ų) for spiridonovite.

Atom	s.o.f	Wyckoff	x/a	y/b	z/c	Ueq
M1	Cu0.60(1)Ag0.40	4c	0	0	0.37419(7)	0.0623(5)
M2	Cu0.64(1)Ag0.36	4d	⅓	⅔	0.79165(7)	0.0628(4)
M3	Cu0.55(1)Ag0.45	4d	⅓	⅔	0.04146(7)	0.0634(4)
Te1	Te1.00	2b	0	0	0	0.0646(5)
Te2	Te1.00	4d	⅓	⅔	0.66635(3)	0.0699(5)

, whereas selected bond distances are shown in

Table 6. Selected bond distances (Å) for spiridonovite.

M1-	Te1	2.837(2)		M2-	Te2	2.826(2)		M3-	Te2	2.816(2)
	Te2	2.825(1)	(×3)		Te2	2.836(1)	(×3)		Te1	2.832(1)	(×3)

. The CIF is available as Supplementary Material.

5. Results and Discussion

From a chemical point of view, spiridonovite is close to weissite (Cu_2-xTe). However, while weissite can be Ag-free, the presence of Ag in spiridonovite enlarges the coordination polyhedra, creating a different topology with respect to that of weissite, and stabilizing the structure. Indeed, spiridonovite can be seen as a rhombohedrally-compressed antifluorite structure, with a rough ccp arrangement of Te atoms, which exhibit a cubic arrangement. On the contrary, Te atoms exhibit a highly distorted hcp arrangement in weissite, thus producing short Cu-Cu distances and partially occupied Cu sites. Weissite has a complex structure with 24 independent Cu and 12 Te atoms showing significantly different crystal-chemical environments [3], while the crystal structure of spiridonovite is far simpler and comprises two Te sites and three M sites, which are occupied by Cu and minor Ag, as reported in Table 5.

The M atoms have four-fold coordination, creating an arrangement of edge-sharing tetrahedra on (110), similarly to what reported for the crystal structure of empressite (AgTe), that shows sheets of edge-sharing AgTe₄ tetrahedra [11]. The main difference between the two structures is the environment of tellurium atoms: in empressite there are Te₃ groups, a rare feature in mineral crystal structures, so far reported only in empressite and krennerite [12]. The spiridonovite structure is shown in Figure 2. The presence of Ag affects the bond distances (in the range 2.82-2.84 Å; Table 6) that are larger than those reported for Cu tellurides, such as vulcanite (CuTe) [13], rickardite (Cu_3-xTe₂) [14], cameronite (Cu_5-x(Cu,Ag)_3+xTe₁₀ [4]), weissite (Cu_2-xTe) [3], and henryite ((Cu,Ag)_3+xTe₂) [5]. Conversely, they are smaller than those observed in Ag-tellurides, such as empressite (AgTe) [11] and hessite (Ag₂Te) [15]. No short metal-metal contacts are observed. Bond valence sums (

Table 7. Bond valence sums (v.u.) for spiridonovite.

Atom	M1	M2	M3	ΣTe
Te1	0.265×2→		0.277×3↓×6→	2.192
Te2	0.274×3↓×3→	0.267 0.260×3↓×4→	0.286	2.148
	1.087	1.047	1.117

), calculated according to the parameters given by Brese and O’Keeffe [16], and taking into account the refined occupancies (Table 5), confirm the validity of the structural model.

All the minerals belonging to the Cu-Ag-Te system are shown in

Table 8. Minerals belonging to the Cu-Ag-Te system.

Mineral [ref]	Formula	Space Group	Cell Values (Å)	V(Å3)	Z
cameronite [4]	Cu5-x(Cu,Ag)3+xTe10 (x = 0.43)	C2/c	a = 17.906(1) b = 17.927(1) c = 21.230(2) β = 98.081(8)°	6747.2(8)	14
empressite [11]	AgTe	Pmnb	a = 8.882(1) b = 20.100(5) c = 4.614(1)	823.7(3)	16
henryite [5]	(Cu,Ag)3+xTe2 (x = 0.40)	Fd-3c	a = 12.1987(5)	1815.3(2)	16
hessite [15]	Ag2Te	P21/c	a = 8.164(1) b = 4.468(1) c = 8.977(1) β = 124.16(1)°	271.0(1)	4
krennerite [12]	(Au1-xAgx)Te2 (x = 0.2)	Pma2	a = 16.58(3) b = 8.849(3) c = 4.464(3)	654(1)	8
rickardite [14]	Cu3-xTe2	Pmmn	a = 3.9727(4) b = 4.0020(5) c = 6.1066(3)	97.1(1)	2
vulcanite [13]	CuTe	Pmmn	a = 3.155(1) b = 4.092(1) c = 6.956(1)	89.80(3)	2
weissite [3]	Cu2-xTe (x = 0.21)	P3m1	a = 8.3124(7) c = 21.546(1)	1289.3(2)	24

, together with some crystallographic detail.

If we consider a tripled a parameter for spiridonovite, we get the cell: a = 13.89 and c = 22.55 Å. Such a metric has some analogy with that of the β^III synthetic compound of the Cu-Te system [17], which exhibits a hexagonal symmetry and a = 12.54 and c = 21.71 Å. The cell enlargement observed for spiridonovite could be due to the presence of Ag replacing Cu.

However, as demonstrated by [18], the β^III synthetic phase is actually an intermetallic compound, with short Cu-Cu and Te-Te contacts, and thus different from spiridonovite. Cameronite (Cu_5-x(Cu,Ag)_3+xTe₁₀ [4]) and weissite (Cu_2-xTe) [3] have a similar intermetallic nature, showing short bond distances between the metals, characterized by the presence of typical “interpenetrated tetrahedra” due to the short Cu-Cu, Te-Te, and Cu-Te distances.