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Articles |

1 Department of Geography and Geology, University of Copenhagen, Østervoldgade 10, DK–1350 Copenhagen, Denmark
2 Department of Material Research & Physics, University of Salzburg, Hellbrunnerstrasse 34, A–5020 Salzburg, Austria
E-mail address: emilm{at}geol.ku.dk
| ABSTRACT |
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ianka Sb deposit, Low Tatra Mountains, Slovakia. Unit-cell dimensions are a 48.293(15), b 4.1107(13), c 34.223(11) Å, β 106.168(5)°, space group C2/m. There are 11 independent lead sites, 13 antimony sites, and five mixed (Pb, Sb) sites, 36 sulfur positions, and a single, approximately half-occupied oxygen site. Some coordination polyhedra of antimony exhibit split Sb sites, with positional parameters refined independently. Because of the intergrowth, the final R1 value remained at 23.5%. It does not reflect visibly upon positional parameters, but has an adverse influence on the occupancy of mixed positions. Until further occurrences are documented, it remains an unnamed mineral. It is a typical sulfosalt representative of the category of boxwork structures. Other structures of this category comprise pellouxite, marrucciite, vurroite, neyite, and several synthetic sulfosalts. Sulfosalts with a boxwork structure are formed by a combination of three types of structural modules: continuous walls with a complex structure of rod-layer type; these walls are interconnected by partitions, and the resulting boxlike channels are filled by another type of structure rods. In its entirety, this group demonstrates a number of types for each of these kinds of module. The "core" group of Pb–Sb sulfosalts, scainiite, pillaite, pellouxite, rouxelite, a synthetic Mn–Pb sulfosalt, and Pb15–2xSb14+2xS36Ox described in this study, depend on the presence of minor amounts of oxygen in the structures. Oxygen forms a part of a kermesite-like configuration that generates a pronounced change of the local structural arrangement and, in this way, makes the boxwork framework possible. Several REE sulfides form boxwork structures as well.
Keywords: boxwork structures, sulfosalts, unnamed Pb–Sb oxysulfosalt, crystal structure, Kla
ianka deposit, Low Tatra Mountains, Slovakia.
| INTRODUCTION |
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The structures of this category can be understood as an extension of the principle of rod-based structures (rod layers, rod chessboards, etc.), which was worked out by Makovicky (1993, 1997) for less complex families of sulfosalts and then applied to a number of new structures. This principle was also applied to several Pb–Sb–S–O sulfosalts (such as scainiite and pillaite) by the Nantes – Pisa research group but, starting with their study of scainiite, they favored an alternative approach to modular analysis of the Pb–Sb sulfosalts that is based primarily on the kinship with cyclically twinned sulfosalt structures. Spurred by a discovery of a new Pb–Sb sulfosalt, Pb15–2xSb14+2xS36Ox, the boxwork structure of which is documented here, we have summarized the boxwork structures known today and made some generalizations that can be obtained by considering the boxwork approach, including the observations presented by the Nantes–Pisa group. We expect that the conclusions obtainable by the cyclic approach (see listing in Moëlo et al. 2008) will one day complete the understanding of the dual nature of this group. Our boxwork approach also differs from the approach of "couches gaufrées" (or palisade-like layers) developed by Moëlo et al. (2000) and Doussier et al.(2007), respectively, and discussed in more detail below.
| THE OCCURRENCE OF PB15–2xSB14+2xS36Ox |
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ianka in the old antimony mining region on the northern slopes of the Low Tatra Mountains, Slovakia. A single fragment of quartz matrix with aggregates of needle-like sulfosalt crystals yielded crystals of boulangerite, jamesonite, dadsonite and the hitherto unknown sulfosalt. We found it as a single tiny grain with domains in two orientations and in intimate intergrowth with other phases, while looking for a suitable crystal of dadsonite (Makovicky et al. 2006). Fundamental features of the new crystal structure were determined in 2003. Since then, neither examination of concentrates nor electron-microprobe examination of the material collected in Kla
ianka gave an indication of more material of the same kind. Therefore, the structure determination was carried out to its possible limits and the results are presented here. | EXPERIMENTAL DATA |
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(Uiso) found to be large as well. Fluctuation of occupancy of the mixed sites in different cycles of least-squares refinement is of the order of 1–2
, whereas their positional coordinate values, and those of all other cations and sulfur atoms, vary insignificantly, within the limits of their low
values. In terms of electrons per site, the differences between different results for the occupancy of the oxygen position are minute, compared to the Z values of Pb and Sb. Tables 2 and 3 contain the structural information, whereas a comparison with other related phases is made in Table 4.
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| DESCRIPTION OF COORDINATION POLYHEDRA IN PB15–2xSB14+2xS36Ox |
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The coordination polyhedra of lead are mono- and bicapped trigonal coordination prisms, positioned typically on the outer surfaces of Pb–Sb rods (i.e., acting as envelopes of lone-electron-pair micelles of Sb); they are intermeshed with the coordination pyramids of antimony, which are concentrated in the rod interior. Eight of them are "standing prisms" with the (approximate) three-fold axes parallel to the rods (i.e., b axis), and three are "lying-down prisms" with three-fold axes at 90° to the rod elongation. A three-fold group of bicapped coordination prisms, Pb2–Pb4–Pb5, and the only tricapped trigonal prismatic Pb site, Pb 7, respectively, bind together three adjacent rods (micelles) at two different points of the structure. The Pb–S distances are recorded in Table 3.
The coordination polyhedra of antimony are square coordination pyramids completed by two additional S atoms under the base to monocapped trigonal prisms. The Sb atom is situated in the prism wall, and the lone electron-pair of Sb, in the volume of the prism. The distance of the additional S from Sb may exceed 4 Å, but the shape of the prism is only rarely distorted: this happens for Sb8 and Sb11 by a partial closure of the lone-electron-pair micelle, and especially for Sb10, which faces the Sb14 site (Figs. 1, 2). The Sb14 atom is bound to oxygen and has an entirely reorganized scheme of Sb–S bonds. An even distribution between "standing" and "lying-down" coordination prisms of Sb is observed.
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As already stated, anisotropic displacement parameters indicate that Sb16 and, to a lesser degree, also Sb14 and Sb5, might be positions split along the 4 Å b axis. In the case of Sb14, this might be connected with bond formation to oxygen because, with a lack of visible superstructure, Sb14 might be bonding randomly to the ligand below, or above, its level. The bond-length scheme (Table 3) suggests a similar disorder along the b direction for Sb19 as well.
The mixed sites are concentrated in a rod of SnS-like structure, which fills the box-like void of the boxwork structure (Fig. 2). Three such sites, Sb1–Pb1, Sb2–Pb3 and Sb17–Pb15, were refined as split sites, with every fractional atom having its own coordinates and a label. Two more sites, Sb3 and Sb20, could only be refined as unsplit sites in which Sb and Pb have the same set of coordinates. In all cases, complete occupancy of a coordination polyhedron was assumed. The Pb atoms protrude from the base of the pyramid and, for well-split cases, the relevant bond-distances approximate those of pure Pb and Sb (not forgetting, however, that their ligands represent mixed positions in such a case). All mixed sites form standing, monocapped trigonal coordination prisms.
The Sb14 site is a specific antimony site of decisive importance for oxysulfosalts of Pb and Sb (Moëlo et al. 2000). The three nearly perpendicular short Sb–anion bonds are: (1) Sb14–S25 (2.464 Å) to the vertex of the configuration, which remained from the "reduction" of the coordination pyramid SbS5, analogous to those of the Sb neighbors, (2) Sb14–S22 (2.499 Å) to a new S position with the same y height as Sb14, and (3) S14–O (2.128 Å), which is oriented along +y or –y with equal probability. Two additional distances, Sb14–S21, are 3.264 Å. The Sb–O distance is an average distance because both Sb14 and O display a pronounced (oriented) displacement parallel to [010]. The half-occupied O site suggests that each Sb14 atom has only one oxygen neighbor. Doussier et al.(2007) modeled this coordination as a mean of 2.02 Å for the Sb–O bond and 2.36 Å for the Sb–vacancy distance; these differences are obtained by displacements of Sb toward oxygen and away from vacant sites, similar to our displacements. Doussier et al.(2007) assumed a half-filled oxygen site in the synthetic Mn sulfosalt they studied, similar to our direct refinement results. The oxygen positions in scainiite (Moëlo et al. 2000) were refined as two full and one half-occupied site, in pillaite (Meerschaut et al. 2001) and pellouxite (Palvadeau et al. 2004) as a half-occupied site, and in rouxelite (Orlandi et al. 2005) as a ~2/3 occupied position.
| MODULAR DESCRIPTION AND AFFINITIES |
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Boxwork structures: definition and architecture
Boxwork structures are the most complex modular category of structures of sulfosalts and other complex sulfides known to date. Their name (Makovicky et al. 2001) comes from the arrangement of structural elements into a framework of walls interconnected by partitions, which together delimit large quadrilateral channels filled by structural elements that are crystal-chemically similar to, although not identical with, the elements that constitute the channel walls. The boxwork structures thus are not a category of micro- or mesoporous structures, in which the channel fill is profoundly different from the structure framework and even may be exchanged under certain conditions (Makovicky 2005).
This definition allows for a variety of principles in wall and partition construction as well as in the box fill, but the majority of sulfosalt structures known to date, those determined chiefly by the members of the Nantes–Pisa research group, follow a rather narrow set of principles, making possible a unified description of this "principal" Pb–Sb subgroup of (primarily) oxysulfosalts. The "aberrant" cases can generally be interpreted as related to definite groups of sulfosalts lying outside the boxwork category. Prominent cases of boxwork structures also exist among the chalcogenides of rare-earth elements.
As already mentioned, the category of boxwork structures overlaps partly with another large category of complex sulfides, the derivatives of the cyclically twinned structures, known among sulfosalts and other complex sulfides (Moëlo et al. 2000, 2008). Thus, several important boxwork sulfosalts, e.g., pillaite, scainiite and the present sulfosalt, can be described with equal validity as structures derived from cyclically twinned sulfosalt structures of zinckenite or barium– bismuth sulfide type (Makovicky 1985); they were classified as such by Moëlo et al.(2008). The duality of description is the best expression of the dual nature of these structures. However, not all important cases of the boxwork category are "cyclic derivatives", e.g., neyite (Makovicky et al. 2001) and La10Er9S27 (Carré & Laruelle 1973, Makovicky 1992), whereas structures like (Mn1–xPbx)Pb10–ySb12–yS26–yCl4+yO (Doussier et al. 2007) are a boundary case. Besides the boxwork structures, the derivatives of cyclically twinned structures encompass other important groups of sulfosalts, such as the kobellite-type structures in the broadest sense. Treatment of the cyclic aspect of complex sulfosalts will not be taken up here, except for a short mention of its application to our new compound.
The structural elements of boxwork structures
The continuous walls in "typical" boxwork structures (drawn vertically in all figures) can be based on the SnS archetype, in a smaller number of cases on the PbS archetype or, being just a double layer, the archetype remains ambiguous (Makovicky 1997). In most cases, they represent an alternation of two types or rods along the layer. They are interconnected by a double layer (100)SnS; this layer-building principle corresponds in principle to "Layer Type 1" observed in boulangerite (Makovicky 1993). In neyite, based on the PbS principle, the interconnection proceeds via a triple layer (100)PbS.
The double layers discernible in the wall structures based on SnS archetype take part in two adjacent rods. They are sinuous, as is also the layer in neyite, and start on one side of the wall, ending on its opposite side. Sinuosity is materialized via insertion of modified "kermesite-like fragments"(Moëlo et al. 2000) (in scainiite, Fig. 3), or by insertion of Hg (in marrucciite, Fig. 4), and by insertion of Pb [in pillaite (Fig. 5), which has three types of rods, although these layers (in "walls") can also be interpreted as Layer-type 11 of Makovicky (1993) with an extended "interconnecting" region between two adjacent rods, as well as in the present structure (Fig. 2)]. Finally, sinuosity can also be produced by the presence of slightly inflated lone-electron- pair micelles (in pellouxite, Fig. 6; for all references see Table 4). These sinuous double layers may have two types of termination: either both terminations end in Sb, which is coordinated to S and O in a "kermesite-type" arrangement defined by Moëlo et al.(2000) (see below), or they have one termination by a SbS5 pyramid and another one of the "kermesite type". Each structure has only one type of double layers.
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The configuration of the partitions between the walls varies much less. In most cases, they are lozenge-shaped rods based on the SnS archetype, four atomic layers thick and with [001]SnS as the rod axis. The maximum width observed involves four pseudotetragonal subcells (pyramids) (pillaite); more common are three pyramids (e.g., scainiite and the present compound), and a two-pyramid width is observed in the synthetic Mn sulfosalt. Their pseudohexagonal, anion-lined surfaces face the walls just described, the pseudotetragonal surfaces face the "fill" of the channels. The only other type observed are partitions in marrucciite; these are based on the PbS archetype and can be interpreted as truncated, with an additional Pb atom at the corner of the partition.
In neyite (Fig. 8) and in La10Er9S27, dealt with in detail below, the partitions are pseudotetragonal layers, two atomic layers thick. In neyite, they contain a unique lateral offset in the form of a column of empty octahedra flanked by tetrahedrally coordinated Cu sites, fully analogous to the configurations observed in the sheared-layer structures of proudite-group minerals.
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The SnS-based "fill elements" are [001]SnS rods in most structures. In neyite (Makovicky et al. 2001), the synthetic Pb–La–Bi sulfosalt (Iordanidis & Kanatzidis 2001, Doussier et al. 2007) and the synthetic Mn sulfosalt (Doussier et al. 2007), as well as vurroite (Pinto et al. 2008) (the latter two examples contain single-octahedron rods), they are [011]PbS. Because of different cross-sections, comparison of the size of fill elements in different structures can be best performed counting the number of cations and anions per cross-section in the projections illustrated. They start with MS4 for single-octahedron columns and end with M18S26 for the present compound. For scainiite, the fill is M9S14, whereas in pillaite, the complete "fill" represents M6S10Cl2, because chlorine completes the lozenge-shaped fill-rod. The same stoichiometry, M6S12, occurs in the PbS-like fragments, terminated by trigonal prisms, in Pb2LaxBi8–xS14 (Iordanidis & Kanatzidis 2001, Doussier et al. 2007). In terms of an SnS-like arrangement, the rods of Sb sulfosalts contain between two fragments and four fragments of tightly bonded double layers, respectively seen in scainiite and in the new structure.
The different types of rods described here were already defined and illustrated by Moëlo et al.(2000) and Palvadeau et al.(2004) as rods A (defined as partitions in the present contribution), B (channel fill) and C1–C2 rods (Moëlo et al. 2000) or type-C ribbon layers (Palvadeau et al. 2004) (our walls). In the paper on marrucciite, Orlandi et al.(2007) altered the assignment of the A, B, C notation to the three rod types mentioned, and in the paper by Doussier et al. (2007), this notation was abandoned in favor of "palisade-like layers" discussed further below. A brief discussion of boxwork structures and illustration of the rods involved was also given by Ferraris et al.(2004) and Makovicky (2006).
Modular character of Pb15–2xSb14+2xS36Ox
The structure of Pb15–2xSb14+2xS36Ox is a typical rod-based structure of a Pb–Sb boxwork type, broadly similar to those of pillaite or pellouxite, with the largest channels or "boxes" and most voluminous channel fill known to this day (Table 4). Typically, rods of the box walls and partitions are primarily rods with extensive pseudotetragonal surfaces. Sheared pseudohexagonal surfaces 33.42 form only portions of rod terminations. Correspondingly, the box contents consist of an enclosed rod with all surfaces of a sheared pseudohexagonal type, with only single-corner pyramids as intervals of pseudotetragonal type (Fig. 2).
The combined (100) walls in Pb15–2xSb14+2xS36Ox consist of two alternating types of rods arranged en échelon in a way similar to the rod-layers in boulangerite: (1) smaller rods, with four combined layers of cations–anions that are three coordination pyramids wide [these are pseudotetragonal pyramids that have also been described as Q subcells by Makovicky (1993)]. They are interconnected with (2) larger rods via tightly bonded double-layers. The latter rods are 3
pyramids wide, 4 atomic layers thick, and they end in "kermesite-like portions", instead of the classical 33.42 (101)SnS endings [a mathematical notation for surfaces in which three triangular and two quadratic configurations of sulfur atoms meet in every S atom, defined as sheared pseudohexagonal anionic surfaces by Makovicky (1993)], seen in the classical rod-based sulfosalts (Makovicky 1993). In this "kermesite-like" configuration, the horizontal, outwardly oriented short Sb–S bond and that to the vertex of the pyramid are accompanied by a short bond to oxygen above or below the Sb atom.
The partition (quoted as rod category 3 below) is a rod that is three pseudotetragonal coordination pyramids wide; it has a regular rod aspect and a lozenge-like cross-section. The encapsulated "fill" rods (category 4) are eight atomic layers thick, and in their principal portions, they are three pyramids wide, with terminal double-layers reduced to a width of two, and finally only one coordination pyramid (Fig. 2). The anionic surfaces are of the 33.42 configuration; the rod is truncated in two opposing corners by pseudotetragonal intervals only one Pb pyramid wide.
Rods of the categories (1) and (2) are infinite along [010]SnS, whereas the category (3), i.e., the transversal rod (i.e., the partition) and (4) the boxwork infill, are infinite along [001]SnS. In the projection along [010] of the present structure, the cases (1) and (2) exhibit "lying-down" monocapped trigonal coordination prisms, whereas the configurations (3) and (4) are composed of "standing" monocapped trigonal coordination prisms (Fig. 2). The Sb–S–O configuration of rods (2) forms an embayment into which a corner of the transversal rod (3) is inserted.
The degenerate cyclic character (Makovicky 1985, Moëlo et al. 2000) of the structure of Pb15–2x Sb14+2xS36Ox is produced by the arrangement of three distinct rods around a local three-fold axis in each of the acute corners of a "boxwork" channel. On a local scale, they form groups of three edge-sharing bicapped trigonal coordination prisms of Pb. The rods involved are of the category (1) and (3) defined above, both of 3Q type, but with different external connections, as well as the corner portions of the large rod (4). As mentioned above, the rods (1) and (3) display an orientation of the SnS archetype at 90° to that in rod (4). All this limits the size of the region that obeys the local three-fold axis.
Surfaces of the first three types of rods in Pb15–2x Sb14+2xS36Ox are occupied by Pb in standing and lyingdown trigonal coordination prisms, which are mono-, bi-, and tricapped, according to the local match requirement on rod interfaces. The longest match is ~4 Q : 2
H in terms of primitive pseudotetragonal (Q) and centered orthohexagonal (H) subcells (mesh), followed by ~2
Q : 1
H and ~1
Q : 1 H. Rods of category (1) and (2) together compose a (100) rod-layer that approximates the Type-1 rod-layer of Makovicky (1993), although modified by the insertion of a "kermesite-like configuration" at selected edges. The configurations resulting from this arrangement allow insertion of an unmodified transversal 3Q rod (a partition) and a formation of a "box", in which the cation–anion contacts between the walls and "fill" satisfy the coordination requirements of lead.
| STRUCTURAL AFFINITIES OF PB15–2xSB14+2xS36Ox |
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This concept leads to the question of possible homologous series in this group of compounds. All representatives of the Pb–Sb sulfosalts of the "core" oxysulfosalt group, related to zinkenite, have variously large local environments in common, as illustrated in the original descriptions by the Nantes–Pisa research group. However, the misfit between the dimensions of the arrays of pseudotetragonal subcells in the walls and the dimensions of the n x (101)SnS subperiodicity of pseudohexagonal surfaces means that practically all attempts to produce a homologous expansion or contraction are frustrated, demanding excessive concentrations of kermesite-like elements in order to compensate for the lack of fit.
The new sulfosalt, Pb15–2xSb14+2xS36Ox, however, represents a case close to homology. In the structure of pellouxite (Palvadeau et al. 2004), a large complex rod (Fig. 9) can be defined, which also describes large portions of the structure of Pb15–2xSb14+2xS36Ox. The latter structure contains additional elements that form a zig-zag layer cutting diagonally through the walls and the box-fill and displacing the complex rods as well (Fig. 9). In addition, however, when we proceed along the [100] and [001] directions of pellouxite, the adjacent complex rods are invariably displaced by
Q (~2 Å) parallel to [010] in the new compound. Therefore, these two structures are not two homologues in an exact sense but plesiotypes (Makovicky 1997).
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| FROM THE ROD -BASED TO BOXWORK STRUCTURES: THE IMPORTANCE OF THE "KERMESITE -LIKE " CONFIGURATION |
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ík 1967, Bonazzi et al. 1987,
urovi
& Hybler 2006). Details of atom coordinations (bond distances) in the "kermesite-like" configurations of Pb–Sb oxysulfosalts are to be found in Moëlo et al.(2000), Orlandi et al.(2001, 2004) and Doussier et al. (2007). Both the apically or internally situated "kermesite configurations" shorten the pseudotetragonal subperiodicity of cation–anion configurations (and their surfaces) by about a half-width of the coordination pyramid of Sb, in the direction perpendicular to the rod orientation. Thus, the structural element that follows, and is attached into the embayment of the structure wall, can be positioned "earlier", and yield structural configurations not considered possible with the above-mentioned "classical matches" in rod-based sulfosalts. In addition, as already mentioned by Moëlo et al.(2000), the paired "kermesite-like" elements in the centers of double layers in scainiite shift the two portions of the double layer by ~2 Å against one another. For the Pb–Sb sulfosalts, along the wall direction, the position of the next partition thus fits with the dimensions and position of the fill element and can follow after it. It would be situated too far for any contact with the fill element without the intervention of the "kermesite fragment". Furthermore, the "horizontally situated" apical S atom of the "kermesite configuration" becomes a regular corner-component of the partition (Figs. 2, 3), and determines its shift along the rod axis to such a level that the coordinations of Pb atoms on the partition surfaces fit with the heights of S atoms on the pseudohexagonal surfaces of the fill element. All this would not exist without the small islands of "kermesite configuration" in the structure.
Is oxygen invariably present? Light (1997) described a structure of "Pb8.67Sb11.33S23", with a nonstoichiometric formula derived from structure determination, with unit-cell dimensions (Table 4) marginally larger than those of pillaite (Meerschaut et al. 2001) and a crystal structure virtually identical with that of pillaite. Light placed an Sb atom (with 5% Pb) into the Cl site of pillaite; all metal and metalloid sites were refined as mixed sites. These crystals are a product of vapor transport with iodine and H2O vapor as a transport medium. Thus, we interpret this "trigonal prismatic Sb position" as the iodine position, the "5% Pb content" being in full agreement with the difference between the atomic numbers of Sb and I. The I–cation distances are 3.514 Å, 3.546 Å, and 3.610 Å, to be compared with the Cl-cation distances in pillaite itself, 3.250 Å, 3.329 Å, and 3.399 Å. The marginal Sb atom in the rods of the continuous walls in Lights structure has a coordination identical to that in the "kermesite configurations" of pillaite, except for the unidentified oxygen.
Our interpretation of the phase synthesized by Light (1997) has been corroborated by the syntheses of Kryukova et al.(2005), who prepared a phase with unit-cell parameters nearly identical with those of pillaite (Table 4), a composition estimated by a combination of WDS and EDS as Cu0.51Pb8.73Sb8.15I1.6S20 (no data on the analysis given; the phase was obtained by vapor transport from a natural, mixed sulfosalt material), and a pillaite-like structure that was verified by HRTEM and comparison of calculated and observed powder-diffraction patterns. Therefore, both sets of investigations describe apparently the same phase, a synthetic "iodo-pillaite", and left some problems unsolved, especially the presence of oxygen in the "kermesite-like fragments", which seems inevitable from the coordination found by Light (1997).
| PALISADE -LIKE LAYERS ("COUCHES GAUFRÉES") |
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The paper by Doussier et al. (2007) contains an attempt to classify boxwork structures according to the complex palisade-like layers in them, distancing them in this way from the large body of rod-based structures of layer, chessboard, and even cyclic types. One of the aims of the present paper is to re-establish this connection, preserving the unity of the family of rod-based structures on a higher level of complexity.
| STRUCTURE TYPES OTHER THAN PB–SB OXYSULFOSALTS RELATED TO ZINKENITE |
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Neyite, Ag2Cu6Pb25Bi26S68 (Makovicky et al. 2001), is a type structure of the boxwork concept (Fig. 8). The clearly outlined box-fill is of the PbS type, with the composition M26S36 and with pseudohexagonal surfaces, disturbed only by two short Q intervals at the acute corners. The boxfill faces the pseudotetragonal surfaces of the sinuous walls, three atomic planes thick, as well as those of the tightly bonded double-layers serving as partitions. In analogy to rouxelite, the straight portions of the sinuous walls are locally extended by insertion of broad, foreshortened Ag octahedra, and the four surrounding polyhedra are rotated and thus fitted to the periodicity of the adjacent pseudohexagonal surface (Fig. 8).
One of the smallest boxwork frameworks among sulfosalts is the structure of Bi2In4S9 (Chapuis et al. 1972). Ribbons with a composition Bi2In2S6 form porous walls; other such ribbons, stabilized in place by In–S bonds, form partitions, and fragments of octahedrally coordinated In layers are the box fill (Fig. 13). The marginal atoms of five-coordinated indium in the latter fragments can be assigned either to the framework or to the fill.
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| CONCLUSIONS |
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| AKNOWLEDGEMENTS |
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| References |
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Received December 11, 2007
,revised manuscript received January 18, 2009
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