The crystal structure of franckeite, Pb21.7Sn9.3Fe4.0Sb8.1S56.9

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The crystal structure of franckeite, Pb21.7Sn9.3Fe4.0Sb8.1S56.9. / Makovicky, Emil; Petricek, Vaclav; Dusek, Michal; Topa, Dan.

In: American Mineralogist, Vol. 96, No. Nov-Dec., 2011, p. 1686-1702.

Research output: Contribution to journalJournal articleResearchpeer-review

Harvard

Makovicky, E, Petricek, V, Dusek, M & Topa, D 2011, 'The crystal structure of franckeite, Pb21.7Sn9.3Fe4.0Sb8.1S56.9', American Mineralogist, vol. 96, no. Nov-Dec., pp. 1686-1702. https://doi.org/10.2138/am.2011.3814

APA

Makovicky, E., Petricek, V., Dusek, M., & Topa, D. (2011). The crystal structure of franckeite, Pb21.7Sn9.3Fe4.0Sb8.1S56.9. American Mineralogist, 96(Nov-Dec.), 1686-1702. https://doi.org/10.2138/am.2011.3814

Vancouver

Makovicky E, Petricek V, Dusek M, Topa D. The crystal structure of franckeite, Pb21.7Sn9.3Fe4.0Sb8.1S56.9. American Mineralogist. 2011;96(Nov-Dec.):1686-1702. https://doi.org/10.2138/am.2011.3814

Author

Makovicky, Emil ; Petricek, Vaclav ; Dusek, Michal ; Topa, Dan. / The crystal structure of franckeite, Pb21.7Sn9.3Fe4.0Sb8.1S56.9. In: American Mineralogist. 2011 ; Vol. 96, No. Nov-Dec. pp. 1686-1702.

Bibtex

@article{f13c3e16ee7c46cf8bce2f1cfa0db9e0,
title = "The crystal structure of franckeite, Pb21.7Sn9.3Fe4.0Sb8.1S56.9",
abstract = "The layer-like crystal structure of franckeite from the mine of San Jos{\'e}, Bolivia, exhibits a pronounced one-dimensional transversal wave-like modulation and a non-commensurate layer match in two dimensions. It consists of alternating pseudohexagonal (H) layers and pseudotetragonal (Q) slabs and forms a homologous pair with cylindrite, which has thinner Q slabs. The Q slabs in franckeite are four atomic layers thick. The two components have their own lattices and a common modulation. The Q slab of the refined franckeite structure, Pb21.74Sn9.34Fe3.95Sb8.08S56.87, is an MS layer (M = Pb2+, Sn2+, Sb3+) four atomic planes thick, with a = 5.805(8), b = 5.856(16) {\AA}, and the layer-stacking vector c = 17.338(5) {\AA}. The lattice angles are a = 94.97(2)°, {\ss} = 88.45(2)°, ¿ = 89.94(2)°; the modulation vector q = –0.00129(8) a* + 0.128436(10) b* – 0.0299(3) c*. The H layer is a single-octahedron MS2 layer (M = Sn4+, Fe2+) with a = 3.665(8), b = 6.2575(16), c = 17.419(5) {\AA}, a = 95.25(2)°, {\ss} = 95.45(2)°, ¿ = 89.97(2)°; the modulation vector is q = –0.00087(8) a* + 0.13725(16) b* – 0.0314(4) c*. The a and b vectors of both subsystems are parallel; the c vectors diverge. (3+2)D superspace refinement was performed in the superspace group C1, using 7397 observed reflections. It resulted in the overall R(obs) value equal to 0.094. The Q slabs are composed of two tightly bonded double-layers, separated by an interspace hosting non-bonding electron pairs. Average composition of cations on the outer surface was refined as Pb0.74(Sn,Sb)0.26, whereas that of cations, which are adjacent to the interspace with lone electron pairs, with a configuration analogous to that observed in orthorhombic SnS, corresponds to (Sn,Sb)0.73Pb0.27. Iron is dispersed over the octahedral Sn4+ sites in the H layer. Transversal modulation of the Q slab is achieved by local variations in the Pb:(Sn,Sb) ratios at its surface and interior. Its purpose is to re-establish a one-dimensional commensurate contact along [010] between the curved Q and H surfaces to the greatest extent possible. Layer-stacking disorder and divergence of the Q and H stacking directions, and the divergence between modulation wave-front and these stacking directions are typical for the composite structures of franckeite and cylindrite. Because of the increased rigidity of the Q component, franckeite usually forms masses of curved crystals rather than cylindrical aggregates. The existence of this family depends critically on the radius ratios of the cations involved, especially those involving (Pb2+, Sn2+) and Sn4+. Their replacement by a Pb2+:Bi3+ combination leads to misfit layer structures of a very different type, typified by cannizzarite.",
author = "Emil Makovicky and Vaclav Petricek and Michal Dusek and Dan Topa",
year = "2011",
doi = "10.2138/am.2011.3814",
language = "English",
volume = "96",
pages = "1686--1702",
journal = "American Mineralogist",
issn = "0003-004X",
publisher = "Mineralogical Society of America",
number = "Nov-Dec.",

}

RIS

TY - JOUR

T1 - The crystal structure of franckeite, Pb21.7Sn9.3Fe4.0Sb8.1S56.9

AU - Makovicky, Emil

AU - Petricek, Vaclav

AU - Dusek, Michal

AU - Topa, Dan

PY - 2011

Y1 - 2011

N2 - The layer-like crystal structure of franckeite from the mine of San José, Bolivia, exhibits a pronounced one-dimensional transversal wave-like modulation and a non-commensurate layer match in two dimensions. It consists of alternating pseudohexagonal (H) layers and pseudotetragonal (Q) slabs and forms a homologous pair with cylindrite, which has thinner Q slabs. The Q slabs in franckeite are four atomic layers thick. The two components have their own lattices and a common modulation. The Q slab of the refined franckeite structure, Pb21.74Sn9.34Fe3.95Sb8.08S56.87, is an MS layer (M = Pb2+, Sn2+, Sb3+) four atomic planes thick, with a = 5.805(8), b = 5.856(16) Å, and the layer-stacking vector c = 17.338(5) Å. The lattice angles are a = 94.97(2)°, ß = 88.45(2)°, ¿ = 89.94(2)°; the modulation vector q = –0.00129(8) a* + 0.128436(10) b* – 0.0299(3) c*. The H layer is a single-octahedron MS2 layer (M = Sn4+, Fe2+) with a = 3.665(8), b = 6.2575(16), c = 17.419(5) Å, a = 95.25(2)°, ß = 95.45(2)°, ¿ = 89.97(2)°; the modulation vector is q = –0.00087(8) a* + 0.13725(16) b* – 0.0314(4) c*. The a and b vectors of both subsystems are parallel; the c vectors diverge. (3+2)D superspace refinement was performed in the superspace group C1, using 7397 observed reflections. It resulted in the overall R(obs) value equal to 0.094. The Q slabs are composed of two tightly bonded double-layers, separated by an interspace hosting non-bonding electron pairs. Average composition of cations on the outer surface was refined as Pb0.74(Sn,Sb)0.26, whereas that of cations, which are adjacent to the interspace with lone electron pairs, with a configuration analogous to that observed in orthorhombic SnS, corresponds to (Sn,Sb)0.73Pb0.27. Iron is dispersed over the octahedral Sn4+ sites in the H layer. Transversal modulation of the Q slab is achieved by local variations in the Pb:(Sn,Sb) ratios at its surface and interior. Its purpose is to re-establish a one-dimensional commensurate contact along [010] between the curved Q and H surfaces to the greatest extent possible. Layer-stacking disorder and divergence of the Q and H stacking directions, and the divergence between modulation wave-front and these stacking directions are typical for the composite structures of franckeite and cylindrite. Because of the increased rigidity of the Q component, franckeite usually forms masses of curved crystals rather than cylindrical aggregates. The existence of this family depends critically on the radius ratios of the cations involved, especially those involving (Pb2+, Sn2+) and Sn4+. Their replacement by a Pb2+:Bi3+ combination leads to misfit layer structures of a very different type, typified by cannizzarite.

AB - The layer-like crystal structure of franckeite from the mine of San José, Bolivia, exhibits a pronounced one-dimensional transversal wave-like modulation and a non-commensurate layer match in two dimensions. It consists of alternating pseudohexagonal (H) layers and pseudotetragonal (Q) slabs and forms a homologous pair with cylindrite, which has thinner Q slabs. The Q slabs in franckeite are four atomic layers thick. The two components have their own lattices and a common modulation. The Q slab of the refined franckeite structure, Pb21.74Sn9.34Fe3.95Sb8.08S56.87, is an MS layer (M = Pb2+, Sn2+, Sb3+) four atomic planes thick, with a = 5.805(8), b = 5.856(16) Å, and the layer-stacking vector c = 17.338(5) Å. The lattice angles are a = 94.97(2)°, ß = 88.45(2)°, ¿ = 89.94(2)°; the modulation vector q = –0.00129(8) a* + 0.128436(10) b* – 0.0299(3) c*. The H layer is a single-octahedron MS2 layer (M = Sn4+, Fe2+) with a = 3.665(8), b = 6.2575(16), c = 17.419(5) Å, a = 95.25(2)°, ß = 95.45(2)°, ¿ = 89.97(2)°; the modulation vector is q = –0.00087(8) a* + 0.13725(16) b* – 0.0314(4) c*. The a and b vectors of both subsystems are parallel; the c vectors diverge. (3+2)D superspace refinement was performed in the superspace group C1, using 7397 observed reflections. It resulted in the overall R(obs) value equal to 0.094. The Q slabs are composed of two tightly bonded double-layers, separated by an interspace hosting non-bonding electron pairs. Average composition of cations on the outer surface was refined as Pb0.74(Sn,Sb)0.26, whereas that of cations, which are adjacent to the interspace with lone electron pairs, with a configuration analogous to that observed in orthorhombic SnS, corresponds to (Sn,Sb)0.73Pb0.27. Iron is dispersed over the octahedral Sn4+ sites in the H layer. Transversal modulation of the Q slab is achieved by local variations in the Pb:(Sn,Sb) ratios at its surface and interior. Its purpose is to re-establish a one-dimensional commensurate contact along [010] between the curved Q and H surfaces to the greatest extent possible. Layer-stacking disorder and divergence of the Q and H stacking directions, and the divergence between modulation wave-front and these stacking directions are typical for the composite structures of franckeite and cylindrite. Because of the increased rigidity of the Q component, franckeite usually forms masses of curved crystals rather than cylindrical aggregates. The existence of this family depends critically on the radius ratios of the cations involved, especially those involving (Pb2+, Sn2+) and Sn4+. Their replacement by a Pb2+:Bi3+ combination leads to misfit layer structures of a very different type, typified by cannizzarite.

U2 - 10.2138/am.2011.3814

DO - 10.2138/am.2011.3814

M3 - Journal article

VL - 96

SP - 1686

EP - 1702

JO - American Mineralogist

JF - American Mineralogist

SN - 0003-004X

IS - Nov-Dec.

ER -

ID: 36091026