Saul H. LapidusJamie L. MansonKimberly E. CarreiroPeter W. Stephens
Poster Sessions C703 edge-sharing MO 6 (M = octahedrally coordinated cations) octahedra forming parallel MO 4 chains.The crystal structures of all compounds in this family are derived from an aristotype structure in space group P4/mbm following a hierarchical scheme of subgroup relationships.Meanwhile, several compounds are added to this family, also extending the Bärnighausen tree representing all branches and cross-relationships of the symmetry derivations.Mullite itself is an aluminosilicate with an incommensurately modulated structure [3] reinvestigated here by single-crystal neutron-diffraction analysis of a high-quality 2:1 mullite.Its average crystal structure can be derived from the sillimanite structure by a disordered arrangement of (Al,Si)O 4 tetrahedra linking the octahedral chains according to the substitution scheme 2Si 4+ + O 2- 2Al 3+ + vacancy.The reaction involves removal of oxygen atoms from the structure and the formation of oxygen vacancies.Replacing Si by Al yields the oxygen vacancies and causes a migration of undersaturated Al to the so-called T* sites (red tetrahedra linking to bridging oxygen forming the T 3 O clusters.We have performed statistical calculations in a 2×2×2 and a 3×3×2 supercell to find the maximum number of symmetrically independent oxygen-vacancy configurations assuming one to four vacancies in the 2×2×2 case and up to seven vacancies in the 3×3×2 supercell.The total number of combinations is given just by the binomial coefficient with k representing the number of vacancies and n being the site multiplicity of the vacancy positions.As an example, the number of combinations for k = 2 vacancies distributed over n = 8 sites in the 2×2×2 supercell (corresponding to mullite with x = 0.25) is 28 as calculated from the binomial coefficient.Out of this number, only 20 combinations are crystal-chemically possible, and among these combinations, there are only 6 which are symmetrically independent.We are representing here the full ordering scheme of possible and independent oxygen vacancy distributions as a basis for the interpretation of the incommensurate modulation scheme of mullite.
Jamie L. MansonSaul H. LapidusPeter W. StephensPeter K. PetersonKimberly E. CarreiroH.I. SoutherlandTom LancasterStephen J. BlundellAndrew J. SteelePaul GoddardF. L. PrattJohn SingletonYoshimitsu KohamaR. McDonaldRico E. Del SestoNickolaus A. SmithJesper BendixS. A. ZvyaginJinhee KangChanghoon LeeMyung‐Hwan WhangboVivien S. ZapfAlex Plonczak
Klaus BenderD. SchweitzerH. J. Keller
Tina BuničMelita TramšekEvgeny GoreshnikBoris Žemva
H. P. GeserichR. WilckensWolfgang RuppelVolker EnkelmannGerhard WegnerGerhard WienersD. SchweitzerH. J. Keller
Katarina ĐurišJürgen NußMartin Jansen