Cubic crystal system explained

In crystallography, the cubic (or isometric) crystal system is a crystal system where the unit cell is in the shape of a cube. This is one of the most common and simplest shapes found in crystals and minerals.

There are three main varieties of these crystals:

Note: the term fcc is often used in synonym for the cubic close-packed or ccp structure occurring in metals. However, fcc stands for a face-centered-cubic Bravais lattice, which is not necessarily close-packed when a motif is set onto the lattice points. E.g. the diamond and the zincblende lattices are fcc but not close-packed.Each is subdivided into other variants listed below. Although the unit cells in these crystals are conventionally taken to be cubes, the primitive unit cells often are not.

Bravais lattices

The three Bravais latices in the cubic crystal system are:

The primitive cubic lattice (cP) consists of one lattice point on each corner of the cube; this means each simple cubic unit cell has in total one lattice point. Each atom at a lattice point is then shared equally between eight adjacent cubes, and the unit cell therefore contains in total one atom ( × 8).[1]

The body-centered cubic lattice (cI) has one lattice point in the center of the unit cell in addition to the eight corner points. It has a net total of two lattice points per unit cell ( × 8 + 1).

The face-centered cubic lattice (cF) has lattice points on the faces of the cube, that each gives exactly one half contribution, in addition to the corner lattice points, giving a total of 4 lattice points per unit cell ( × 8 from the corners plus  × 6 from the faces).

The face-centered cubic lattice is closely related to the hexagonal close packed (hcp) system, where two systems differ only in the relative placements of their hexagonal layers. The [111] plane of a face-centered cubic lattice is a hexagonal grid.

Attempting to create a base-centered cubic lattice (i.e., putting an extra lattice point in the center of each horizontal face) results in a simple tetragonal Bravais lattice.

Coordination number (CN) is the number of nearest neighbors of a central atom in the structure. Each sphere in a cP lattice has coordination number 6, in a cI lattice 8, and in a cF lattice 12.

Atomic packing factor (APF) is the fraction of volume that is occupied by atoms. The cP lattice has an APF of about 0.524, the cI lattice an APF of about 0.680, and the cF lattice an APF of about 0.740.

Crystal classes

The isometric crystal system class names, point groups (in Schönflies notation, Hermann–Mauguin notation, orbifold, and Coxeter notation), type, examples, international tables for crystallography space group number,[2] and space groups are listed in the table below. There are a total 36 cubic space groups.

No.Point groupTypeExampleSpace groups
Name[3] Schön.IntlOrb.Cox.PrimitiveFace-centeredBody-centered
195–197TetartoidalT23332[3,3]+enantiomorphicUllmannite, Sodium chlorateP23F23I23
198–199P213I213
200–204DiploidalTh2/m
(m)
3*2[3<sup>+</sup>,4]centrosymmetricPyritePm, PnFm, FdI
205–206PaIa
207–211GyroidalO432432[3,4]+enantiomorphicPetziteP432, P4232F432, F4132I432
212–214P4332, P4132I4132
215–217HextetrahedralTd3m
  • 332
[3,3]SphaleriteP3mF3mI3m
218–220P3nF3cI3d
221–230HexoctahedralOh4/m2/m
(mm)
  • 432
[3,4]centrosymmetricGalena, HalitePmm, Pnn, Pmn, PnmFmm, Fmc, Fdm, FdcImm, Iad

Other terms for hexoctahedral are: normal class, holohedral, ditesseral central class, galena type.

Single element structures

See also: Periodic table (crystal structure). As a rule, since atoms in a solid attract each other, the more tightly packed arrangements of atoms tend to be more common. (Loosely packed arrangements do occur, though, for example if the orbital hybridization demands certain bond angles.) Accordingly, the primitive cubic structure, with especially low atomic packing factor, is rare in nature, but is found in polonium.[4] The bcc and fcc, with their higher densities, are both quite common in nature. Examples of bcc include iron, chromium, tungsten, and niobium. Examples of fcc include aluminium, copper, gold and silver.

Another important cubic crystal structure is the diamond cubic structure, which can appear in carbon, silicon, germanium, and tin. Unlike fcc and bcc, this structure is not a lattice, since it contains multiple atoms in its primitive cell. Other cubic elemental structures include the A15 structure found in tungsten, and the extremely complicated structure of manganese.

Multi-element structures

Compounds that consist of more than one element (e.g. binary compounds) often have crystal structures based on the cubic crystal system. Some of the more common ones are listed here. These structures can be viewed as two or more interpenetrating sublattices where each sublattice occupies the interstitial sites of the others.

Caesium chloride structure

One structure is the "interpenetrating primitive cubic" structure, also called a "caesium chloride" or B2 structure. This structure is often confused for a body-centered cubic structure because the arrangement of atoms is the same. However, the caesium chloride structure has a basis composed of two different atomic species. In a body-centered cubic structure, there would be translational symmetry along the [111] direction. In the caesium chloride structure, translation along the [111] direction results in a change of species. The structure can also be thought of as two separate simple cubic structures, one of each species, that are superimposed within each other. The corner of the chloride cube is the center of the caesium cube, and vice versa.[5]

It works the same way for the NaCl structure described in the next section.  If you take out the Cl atoms, the leftover Na atoms still form an FCC structure, not a simple cubic structure.

In the unit cell of CsCl, each ion is at the center of a cube of ions of the opposite kind, so the coordination number is eight. The central cation is coordinated to 8 anions on the corners of a cube as shown, and similarly, the central anion is coordinated to 8 cations on the corners of a cube. Alternately, one could view this lattice as a simple cubic structure with a secondary atom in its cubic void.

In addition to caesium chloride itself, the structure also appears in certain other alkali halides when prepared at low temperatures or high pressures.[6] Generally, this structure is more likely to be formed from two elements whose ions are of roughly the same size (for example, ionic radius of Cs+ = 167 pm, and Cl = 181 pm).

The space group of the caesium chloride (CsCl) structure is called Pmm (in Hermann–Mauguin notation), or "221" (in the International Tables for Crystallography). The Strukturbericht designation is "B2".[7]

There are nearly a hundred rare earth intermetallic compounds that crystallize in the CsCl structure, including many binary compounds of rare earths with magnesium,[8] and with elements in groups 11, 12,[9] [10] and 13. Other compounds showing caesium chloride like structure are CsBr, CsI, high-temperature RbCl, AlCo, AgZn, BeCu, MgCe, RuAl and SrTl.

Rock-salt structure

The space group of the rock-salt or halite (sodium chloride) structure is denoted as Fmm (in Hermann–Mauguin notation), or "225" (in the International Tables for Crystallography). The Strukturbericht designation is "B1".[11]

In the rock-salt structure, each of the two atom types forms a separate face-centered cubic lattice, with the two lattices interpenetrating so as to form a 3D checkerboard pattern. The rock-salt structure has octahedral coordination: Each atom's nearest neighbors consist of six atoms of the opposite type, positioned like the six vertices of a regular octahedron. In sodium chloride there is a 1:1 ratio of sodium to chlorine atoms.  The structure can also be described as an FCC lattice of sodium with chlorine occupying each octahedral void or vice versa.

Examples of compounds with this structure include sodium chloride itself, along with almost all other alkali halides, and "many divalent metal oxides, sulfides, selenides, and tellurides".[6] According to the radius ratio rule, this structure is more likely to be formed if the cation is somewhat smaller than the anion (a cation/anion radius ratio of 0.414 to 0.732).

The interatomic distance (distance between cation and anion, or half the unit cell length a) in some rock-salt-structure crystals are: 2.3 Å (2.3 × 10−10 m) for NaF,[12] 2.8 Å for NaCl,[13] and 3.2 Å for SnTe.[14] Most of the alkali metal hydrides and halides have the rock salt structure, though a few have the caesium chloride structure instead.

Alkali metal hydrides and halides with the rock salt structure! scope="col"
HydridesFluoridesChloridesBromidesIodides
LithiumLithium hydrideLithium fluoride[15] Lithium chlorideLithium bromideLithium iodide
SodiumSodium hydrideSodium fluorideSodium chlorideSodium bromideSodium iodide
PotassiumPotassium hydridePotassium fluoridePotassium chloridePotassium bromidePotassium iodide
RubidiumRubidium hydrideRubidium fluorideRubidium chlorideRubidium bromideRubidium iodide
CaesiumCaesium hydrideCaesium fluoride(CsCl structure)
Alkaline earth metal chalcogenides with the rock salt structure! scope="col"
OxidesSulfidesSelenidesTelluridesPolonides
MagnesiumMagnesium oxideMagnesium sulfideMagnesium selenide[16] Magnesium telluride[17] (NiAs structure)
CalciumCalcium oxideCalcium sulfideCalcium selenide[18] Calcium tellurideCalcium polonide[19]
StrontiumStrontium oxideStrontium sulfideStrontium selenideStrontium tellurideStrontium polonide
BariumBarium oxideBarium sulfideBarium selenideBarium tellurideBarium polonide
Rare-earth[20] and actinoid pnictides with the rock salt structure! scope="col"
NitridesPhosphidesArsenidesAntimonidesBismuthides
ScandiumScandium nitrideScandium phosphideScandium arsenide[21] Scandium antimonide[22] Scandium bismuthide[23]
YttriumYttrium nitrideYttrium phosphideYttrium arsenide[24] Yttrium antimonideYttrium bismuthide[25]
LanthanumLanthanum nitride[26] Lanthanum phosphide[27] Lanthanum arsenideLanthanum antimonideLanthanum bismuthide[28]
CeriumCerium nitrideCerium phosphideCerium arsenideCerium antimonideCerium bismuthide
PraseodymiumPraseodymium nitridePraseodymium phosphidePraseodymium arsenidePraseodymium antimonide[29] Praseodymium bismuthide
NeodymiumNeodymium nitrideNeodymium phosphideNeodymium arsenideNeodymium antimonideNeodymium bismuthide
Promethium?????
SamariumSamarium nitrideSamarium phosphideSamarium arsenideSamarium antimonideSamarium bismuthide
EuropiumEuropium nitrideEuropium phosphide(Na2O2 structure)[30] (unstable)[31]
GadoliniumGadolinium nitrideGadolinium phosphideGadolinium arsenideGadolinium antimonideGadolinium bismuthide
TerbiumTerbium nitrideTerbium phosphideTerbium arsenideTerbium antimonideTerbium bismuthide
DysprosiumDysprosium nitrideDysprosium phosphideDysprosium arsenideDysprosium antimonideDysprosium bismuthide
HolmiumHolmium nitrideHolmium phosphideHolmium arsenideHolmium antimonideHolmium bismuthide
ErbiumErbium nitrideErbium phosphideErbium arsenideErbium antimonideErbium bismuthide
ThuliumThulium nitrideThulium phosphideThulium arsenideThulium antimonideThulium bismuthide
YtterbiumYtterbium nitrideYtterbium phosphideYtterbium arsenideYtterbium antimonide(unstable)[32] [33]
LutetiumLutetium nitrideLutetium phosphideLutetium arsenideLutetium antimonideLutetium bismuthide
Actinium?????
ThoriumThorium nitrideThorium phosphideThorium arsenideThorium antimonide(CsCl structure)
Protactinium?????
UraniumUranium nitrideUranium monophosphideUranium arsenideUranium antimonideUranium bismuthide[34]
NeptuniumNeptunium nitrideNeptunium phosphideNeptunium arsenideNeptunium antimonideNeptunium bismuthide
PlutoniumPlutonium nitridePlutonium phosphidePlutonium arsenidePlutonium antimonidePlutonium bismuthide
AmericiumAmericium nitrideAmericium phosphideAmericium arsenideAmericium antimonideAmericium bismuthide
CuriumCurium nitride[35] Curium phosphideCurium arsenideCurium antimonideCurium bismuthide
BerkeliumBerkelium nitrideBerkelium phosphideBerkelium arsenide?Berkelium bismuthide
Californium??Californium arsenide?Californium bismuthide
Rare-earth and actinoid chalcogenides with the rock salt structure! scope="col"
OxidesSulfidesSelenidesTelluridesPolonides
Scandium(unstable)[36] Scandium monosulfide
YttriumYttrium monosulfide[37]
LanthanumLanthanum monosulfide[38]
CeriumCerium monosulfideCerium monoselenide[39] Cerium monotelluride
PraseodymiumPraseodymium monosulfidePraseodymium monoselenidePraseodymium monotelluride
NeodymiumNeodymium monosulfideNeodymium monoselenideNeodymium monotelluride
Promethium????
SamariumSamarium monosulfideSamarium monoselenideSamarium monotellurideSamarium monopolonide[40]
EuropiumEuropium monoxideEuropium monosulfideEuropium monoselenide[41] Europium monotellurideEuropium monopolonide
Gadolinium(unstable)Gadolinium monosulfide
TerbiumTerbium monosulfideTerbium monopolonide
DysprosiumDysprosium monosulfideDysprosium monopolonide
HolmiumHolmium monosulfideHolmium monopolonide
ErbiumErbium monosulfide
ThuliumThulium monosulfideThulium monopolonide
YtterbiumYtterbium monoxideYtterbium monosulfideYtterbium monopolonide
Lutetium(unstable)[42] Lutetium monosulfideLutetium monopolonide
Actinium????
ThoriumThorium monosulfide[43] Thorium monoselenide(CsCl structure)[44]
Protactinium????
UraniumUranium monosulfideUranium monoselenideUranium monotelluride
NeptuniumNeptunium monosulfideNeptunium monoselenideNeptunium monotelluride
PlutoniumPlutonium monosulfidePlutonium monoselenidePlutonium monotelluride
AmericiumAmericium monosulfideAmericium monoselenideAmericium monotelluride
CuriumCurium monosulfideCurium monoselenideCurium monotelluride
Transition metal carbides and nitrides with the rock salt structure! scope="col"
CarbidesNitrides
TitaniumTitanium carbideTitanium nitride
ZirconiumZirconium carbideZirconium nitride
HafniumHafnium carbideHafnium nitride[45]
VanadiumVanadium carbideVanadium nitride
NiobiumNiobium carbideNiobium nitride
TantalumTantalum carbide(CoSn structure)
Chromium(unstable)[46] Chromium nitride

Many transition metal monoxides also have the rock salt structure (TiO, VO, CrO, MnO, FeO, CoO, NiO, CdO). The early actinoid monocarbides also have this structure (ThC, PaC, UC, NpC, PuC).

Fluorite structure

See main article: Fluorite structure. Much like the rock salt structure, the fluorite structure (AB2) is also an Fmm structure but has 1:2 ratio of ions. The anti-fluorite structure is nearly identical, except the positions of the anions and cations are switched in the structure. They are designated Wyckoff positions 4a and 8c whereas the rock-salt structure positions are 4a and 4b.[47] [48]

Zincblende structure

The space group of the Zincblende structure is called F3m (in Hermann–Mauguin notation), or 216.[49] [50] The Strukturbericht designation is "B3".[51]

The Zincblende structure (also written "zinc blende") is named after the mineral zincblende (sphalerite), one form of zinc sulfide (β-ZnS). As in the rock-salt structure, the two atom types form two interpenetrating face-centered cubic lattices. However, it differs from rock-salt structure in how the two lattices are positioned relative to one another. The zincblende structure has tetrahedral coordination: Each atom's nearest neighbors consist of four atoms of the opposite type, positioned like the four vertices of a regular tetrahedron. In zinc sulfide the ratio of zinc to sulfur is 1:1. Altogether, the arrangement of atoms in zincblende structure is the same as diamond cubic structure, but with alternating types of atoms at the different lattice sites. The structure can also be described as an FCC lattice of zinc with sulfur atoms occupying half of the tetrahedral voids or vice versa.

Examples of compounds with this structure include zincblende itself, lead(II) nitrate, many compound semiconductors (such as gallium arsenide and cadmium telluride), and a wide array of other binary compounds. The boron group pnictogenides usually have a zincblende structure, though the nitrides are more common in the wurtzite structure, and their zincblende forms are less well known polymorphs.[52] [53]

! scope="col"
FluoridesChloridesBromidesIodides
CopperCopper(I) fluorideCopper(I) chlorideCopper(I) bromideCopper(I) iodide
! scope="col"
SulfidesSelenidesTelluridesPolonides
BerylliumBeryllium sulfideBeryllium selenideBeryllium tellurideBeryllium polonide[54] [55]
ZincZinc sulfideZinc selenideZinc tellurideZinc polonide
CadmiumCadmium sulfideCadmium selenideCadmium tellurideCadmium polonide
MercuryMercury sulfideMercury selenideMercury telluride
This group is also known as the II-VI family of compounds, most of which can be made in both the zincblende (cubic) or wurtzite (hexagonal) form.
! scope="col"
NitridesPhosphidesArsenidesAntimonides
BoronBoron nitrideBoron phosphideBoron arsenideBoron antimonide
AluminiumAluminium nitrideAluminium phosphideAluminium arsenideAluminium antimonide
GalliumGallium nitrideGallium phosphideGallium arsenideGallium antimonide
IndiumIndium nitrideIndium phosphideIndium arsenideIndium antimonide
This group is also known as the III-V family of compounds.

Heusler structure

See main article: Heusler compound. The Heusler structure, based on the structure of Cu2MnAl, is a common structure for ternary compounds involving transition metals. It has the space group Fmm (No. 225), and the Strukturbericht designation is L21. Together with the closely related half-Heusler and inverse-Huesler compounds, there are hundreds of examples.

Iron monosilicide structure

The space group of the iron monosilicide structure is P213 (No. 198), and the Strukturbericht designation is B20. This is a chiral structure, and is sometimes associated with helimagnetic properties. There are four atoms of each element for a total of eight atoms in the unit cell.

Examples occur among the transition metal silicides and germanides, as well as a few other compounds such as gallium palladide.

! scope="col"
SilicidesGermanides
ManganeseManganese monosilicideManganese germanide
IronIron monosilicideIron germanide
CobaltCobalt monosilicideCobalt germanide
ChromiumChromium(IV) silicideChromium(IV) germanide

Weaire–Phelan structure

A Weaire–Phelan structure has Pmn (223) symmetry.

It has three orientations of stacked tetradecahedrons with pyritohedral cells in the gaps. It is found as a crystal structure in chemistry where it is usually known as a "type I clathrate structure". Gas hydrates formed by methane, propane, and carbon dioxide at low temperatures have a structure in which water molecules lie at the nodes of the Weaire–Phelan structure and are hydrogen bonded together, and the larger gas molecules are trapped in the polyhedral cages.

See also

building which is a model of a bcc unit cell, with vertical body diagonal.

Further reading

External links

Notes and References

  1. Nomenclature for crystal families, Bravais-lattice types and arithmetic classes. Report of the International Union of Crystallography Ad-Hoc Committee on the Nomenclature of Symmetry. 1985. Acta Crystallographica Section A. 41. 3. 278. 10.1107/S0108767385000587. free. De Wolff . P. M. . Belov . N. V. . Bertaut . E. F. . Buerger . M. J. . Donnay . J. D. H. . Fischer . W. . Hahn . Th. . Koptsik . V. A. . MacKay . A. L. . Wondratschek . H. . Wilson . A. J. C. . Abrahams . S. C. .
  2. Book: International Tables for Crystallography . 10.1107/97809553602060000001 . 978-1-4020-4969-9 . E. . Prince . 2006 . 146060934 .
  3. http://webmineral.com/crystall.shtml Crystallography and Minerals Arranged by Crystal Form
  4. The original discovery was in J. Chem. Phys. 14, 569 (1946).
  5. Web site: Cubic Lattices and Close Packing. 3 October 2013. live. https://web.archive.org/web/20201101010927/https://chem.libretexts.org/Bookshelves/General_Chemistry/Book%3A_Chem1_(Lower)/07%3A_Solids_and_Liquids/7.08%3A_Cubic_Lattices_and_Close_Packing . 2020-11-01 .
  6. Seitz, Modern Theory of Solids (1940), p.49
  7. http://cst-www.nrl.navy.mil/lattice/struk/b2.html The CsCl (B2) Structure
  8. Saccone . A. . Delfino . S. . Macció . D. . Ferro . R. . Magnesium-rare earth phase diagrams: Experimental investigation of the Ho-Mg system . Journal of Phase Equilibria . 14 . 3 . 1993 . 10.1007/bf02668225 . 280–287. 95011597 .
  9. Kanematu . K . T. Alfieri . G. . Banks . E. . Magnetic Studies of Rare Earth Zinc Compounds with CsCl Structure . Journal of the Physical Society of Japan . 26 . 2 . 1969 . 10.1143/jpsj.26.244 . 244–248. 1969JPSJ...26..244K .
  10. Buschow . K. H. J. . Magnetic properties of CsCl‐type rare‐earth cadmium compounds . The Journal of Chemical Physics . 61 . 11 . 1974. 10.1063/1.1681788 . 4666–4670. 1974JChPh..61.4666B .
  11. http://cst-www.nrl.navy.mil/lattice/struk/b1.html The NaCl (B1) Structure
  12. Sundquist . J. J. . Lin . C. C. . 10.1088/0022-3719/14/32/016 . Electronic structure of the F centre in a sodium fluoride crystal . Journal of Physics C: Solid State Physics . 14 . 32 . 4797–4805 . 1981 . 1981JPhC...14.4797S .
  13. . 1965 . 18 . 926–932 . Accuracy of an automatic diffractometer. Measurement of the sodium chloride structure factors . S. C. . Abrahams . J. L. . Bernstein . 10.1107/S0365110X65002244 . 5 .
  14. Kao . W. . Peretti . E. . 10.1016/0022-5088(70)90174-8 . The ternary subsystem Sn4As3-SnAs-SnTe . Journal of the Less Common Metals . 22 . 39–50 . 1970 .
  15. J. Aigueperse, P. Mollard, D. Devilliers, M. Chemla, R. Faron, R. Romano, J. P. Cuer, "Fluorine Compounds, Inorganic" (section 4) in Ullmann’s Encyclopedia of Industrial Chemistry, Wiley-VCH, Weinheim, 2005. .
  16. Broch . Einar . Präzisionsbestimmungen der Gitterkonstanten der Verbindungen MgO, MgS, MgSe, MnO und MnSe . Zeitschrift für Physikalische Chemie . 127U . 1 . 1927-06-01 . 10.1515/zpch-1927-12724 . 446–454. 100227546 . de.
  17. Mir . Showkat H. . Jha . Prakash C. . Dabhi . Shweta . Jha . Prafulla K. . Ab initio study of phase stability, lattice dynamics and thermodynamic properties of magnesium chalcogenides . Materials Chemistry and Physics . 175 . 2016 . 10.1016/j.matchemphys.2016.02.066 . 54–61.
  18. Louail . L. . Haddadi . K. . Maouche . D. . Ali Sahraoui . F. . Hachemi . A. . Electronic band structure of calcium selenide under pressure . Physica B: Condensed Matter . 403 . 18 . 2008 . 10.1016/j.physb.2008.03.009 . 3022–3026. 2008PhyB..403.3022L .
  19. Book: Brown . S.A. . Brown . P.L. . The Aqueous Chemistry of Polonium and the Practical Application of its Thermochemistry . Elsevier Science . 2019 . 978-0-12-819309-9 . 25.
  20. Book: Hulliger, F. . Handbook on the Physics and Chemistry of Rare Earths . Chapter 33 Rare earth pnictides . Elsevier . 1979 . 4 . 10.1016/s0168-1273(79)04006-x . 153–236. 9780444852168 .
  21. Gschneidner . K. A. . Calderwood . F. W. . The As−Sc (Arsenic-Scandium) system . Bulletin of Alloy Phase Diagrams . 7 . 4 . 1986 . 10.1007/bf02873011 . 348–349.
  22. Hayashi . J . Shirotani . I . Hirano . K . Ishimatsu . N . Shimomura . O . Kikegawa . T . Structural phase transition of ScSb and YSb with a NaCl-type structure at high pressures . Solid State Communications . 125 . 10 . 2003 . 10.1016/s0038-1098(02)00889-x . 543–546. 2003SSCom.125..543H .
  23. Book: Horovitz, C.T. . Scandium Its Occurrence, Chemistry Physics, Metallurgy, Biology and Technology . Elsevier Science . 2012 . 978-0-323-14451-3 . 273.
  24. Ono . S. . Despault . J.G. . Calvert . L.D. . Taylor . J.B. . Rare-earth arsenides . Journal of the Less Common Metals . 22 . 1 . 1970 . 10.1016/0022-5088(70)90175-x . 51–59.
  25. Schmidt . F.A. . McMasters . O.D. . Lichtenberg . R.R. . The yttrium-bismuth alloy system . Journal of the Less Common Metals . 18 . 3 . 1969 . 10.1016/0022-5088(69)90159-3 . 215–220.
  26. Natali . F. . Ruck . B.J. . Plank . N.O.V. . Trodahl . H.J. . Granville . S. . Meyer . C. . Lambrecht . W.R.L. . Rare-earth mononitrides . Progress in Materials Science . 58 . 8 . 2013 . 10.1016/j.pmatsci.2013.06.002 . 1316–1360. 1208.2410 . 118566136 .
  27. Ono . S. . Nomura . K. . Hayakawa . H. . Syntheses of new rare-earth phosphides . Journal of the Less Common Metals . 38 . 2–3 . 1974 . 10.1016/0022-5088(74)90055-1 . 119–130.
  28. Yoshihara . K. . Taylor . J.B. . Calvert . L.D. . Despault . J.G. . Rare-earth bismuthides . Journal of the Less Common Metals . 41 . 2 . 1975. 10.1016/0022-5088(75)90038-7 . 329–337.
  29. Hayashi . J. . Shirotani . I. . Tanaka . Y. . Adachi . T. . Shimomura . O. . Kikegawa . T. . Phase transitions of LnSb (Ln=lanthanide) with NaCl-type structure at high pressures . Solid State Communications . 114 . 11 . 2000 . 10.1016/s0038-1098(00)00113-7 . 561–565. 2000SSCom.114..561H .
  30. Gschneidner . K. A. . Calderwood . F. W. . The As−Eu (Arsenic-Europium) system . Bulletin of Alloy Phase Diagrams . 7 . 3 . 1986 . 10.1007/bf02869009 . 279–283.
  31. Taylor . J. B. . Calvert . L. D. . Wang . Y. . Powder data for some new europium antimonides and bismuthides . Journal of Applied Crystallography . 12 . 2 . 1979 . 10.1107/s0021889879012309 . 249–251.
  32. Okamoto . H. . Bi-Yb (bismuth-ytterbium) . Journal of Phase Equilibria . 20 . 4 . 1999 . 10.1361/105497199770335640 . 453.
  33. Duan . Xu . Wu . Fan . Chen . Jia . Zhang . Peiran . Liu . Yang . Yuan . Huiqiu . Cao . Chao . Tunable electronic structure and topological properties of LnPn (Ln=Ce, Pr, Sm, Gd, Yb; Pn=Sb, Bi) . Communications Physics . 1 . 1 . 2018 . 10.1038/s42005-018-0074-8 . 71. 2018CmPhy...1...71D . free. 1802.04554 .
  34. Vogt . O. . Mattenberger . K. . The magnetism of localized or nearly localized 4f and 5f shells . Journal of Alloys and Compounds . 223 . 2 . 1995 . 10.1016/0925-8388(94)09005-x . 226–236.
  35. Book: Benedict . U. . Holzapfel . W.B. . Lanthanides/Actinides: Physics I . Chapter 113 High-pressure studies — Structural aspects . Handbook on the Physics and Chemistry of Rare Earths . Elsevier . 1993 . 17 . 10.1016/s0168-1273(05)80030-3 . 245–300. 9780444815026 .
  36. Leger . J.M. . Yacoubi . N. . Loriers . J. . Synthesis of rare earth monoxides . Journal of Solid State Chemistry . 36 . 3 . 1981 . 10.1016/0022-4596(81)90436-9 . 261–270. 1981JSSCh..36..261L .
  37. Roedhammer . P. . Reichardt . W. . Holtzberg . F. . Soft-Mode Behavior in the Phonon Dispersion of YS . Physical Review Letters . 40 . 7 . 1978. 10.1103/physrevlett.40.465 . 465–468. 1978PhRvL..40..465R .
  38. Didchenko . R. . Gortsema . F.P. . Some electric and magnetic properties of rare earth monosulfides and nitrides . Journal of Physics and Chemistry of Solids . 24 . 7 . 1963 . 10.1016/0022-3697(63)90062-3 . 863–870. 1963JPCS...24..863D .
  39. Smolensky . G. A. . Adamjan . V. E. . Loginov . G. M. . Antiferromagnetic Properties of Light Rare Earth Monochalcogenides . Journal of Applied Physics . 39 . 2 . 1968 . 10.1063/1.2163619 . 786–790. 1968JAP....39..786S .
  40. Kershner . C.J. . DeSando . R.J. . Heidelberg . R.F. . Steinmeyer . R.H. . Rare earth polonides . Journal of Inorganic and Nuclear Chemistry . 28 . 8 . 1966 . 10.1016/0022-1902(66)80054-4 . 1581–1588.
  41. Wachter . P. . The optical electrical and magnetic properties of the europium chalcogenides and the rare earth pnictides . C R C Critical Reviews in Solid State Sciences . 3 . 2 . 1972 . 10.1080/10408437208244865 . 189–241.
  42. Book: Meyer, G . Synthesis of Lanthanide and Actinide Compounds . Springer Netherlands . Dordrecht . 1991 . 978-94-011-3758-4 . 840310000 . 237.
  43. Kruger . O.L. . Moser . J.B. . Lattice constants and melting points of actinide-group IVA-VIA compounds with NaCl-type structures . Journal of Physics and Chemistry of Solids . 28 . 11 . 1967 . 10.1016/0022-3697(67)90257-0 . 2321–2325. 1967JPCS...28.2321K .
  44. D'Eye . R. W. M. . Sellman . P. G. . The thorium–tellurium system . J. Chem. Soc. . 1954 . 10.1039/jr9540003760 . 3760–3766.
  45. Friedrich . Alexandra . Winkler . Björn . Juarez-Arellano . Erick A. . Bayarjargal . Lkhamsuren . Synthesis of Binary Transition Metal Nitrides, Carbides and Borides from the Elements in the Laser-Heated Diamond Anvil Cell and Their Structure-Property Relations . Materials . 4 . 10 . 2011 . 10.3390/ma4101648 . 1648–1692. 28824101 . 5448873 . 2011Mate....4.1648F . free .
  46. Venkatraman . M. . Neumann . J. P. . The C-Cr (Carbon-Chromium) System . Bulletin of Alloy Phase Diagrams . 11 . 2 . 1990 . 10.1007/bf02841701 . 152–159.
  47. Web site: Fluorite. aflow.org. 2020-05-22.
  48. Web site: Rock Salt. aflow.org. 2020-05-22.
  49. Book: Quantum Theory of the Solid State. Kantorovich, L. . 32. Springer. 2004. 1-4020-2153-4.
  50. http://img.chem.ucl.ac.uk/sgp/large/216az1.htm Birkbeck College, University of London
  51. http://cst-www.nrl.navy.mil/lattice/struk/b3.html The Zincblende (B3) Structure
  52. Wang . L.D. . Kwok . H.S. . Cubic aluminum nitride and gallium nitride thin films prepared by pulsed laser deposition . Applied Surface Science . 154–155 . 2000 . 1–4 . 10.1016/s0169-4332(99)00372-4 . 439–443. 2000ApSS..154..439W .
  53. Oseki . Masaaki . Okubo . Kana . Kobayashi . Atsushi . Ohta . Jitsuo . Fujioka . Hiroshi . Field-effect transistors based on cubic indium nitride . Scientific Reports . 4 . 1 . 2014 . 10.1038/srep03951 . 3951. 24492240 . 3912472 . 2014NatSR...4E3951O .
  54. .
  55. Moyer . Harvey V. . Chemical Properties of Polonium . 33–96 . Polonium . Moyer . Harvey V. . TID-5221 . 10.2172/4367751 . 1956 . Oak Ridge, Tenn. . United States Atomic Energy Commission. free . .