Al72.0Ge26.3Mn57.7, orthorhombic, Pnma (no. 62), a = 14.516(2) Å, b = 12.484(2) Å, c = 12.405(2) Å, V = 2248.0 Å 3 , Z = 1, Rgt(F) = 0.036, wRref(F 2 ) = 0.108, T = 297 K.
Source of materialA needle-like crystal was picked up from a master ingot with nominal composition of Al40Mn35Ge25, which was prepared by arc-melting the mixture of pure Al, Mn and Ge in an argon atmosphere. The chemical composition of the title compound Al46.1Mn37.0Ge16.9 was determined by the electron probe microanalysis. Another crystalline phase, Al 34.5 Mn 33.7 Ge 31.8 , which is frequently discussed as a magnetic ternary AlMnGe alloy [1], was also appeared in the present sample.
DiscussionSince the discovery of quasicrystals in rapidly solidified Al-rich manganese alloys [1,2], the so-called approximant structures have been used for providing structural models of quasicrystals. In particular, the crystal structure of Al3Mn with a pentagonal columnar structure serves an essential idea for the structure of decagonal quasicrystal with a period of about 12 Å [3-6]. Magnetic properties for quasicrystals were extensively studied in a variety of Al-Mn based quasicrystals and Mn-Mn interactions were counted as one of the possible origins for their properties [7][8][9][10]. Since an Al3Mn-type approximant for the Al-Mn-Ge decagonal quasicrystal also indicated a large magnetization anisotropy [9], we carried out the structural analysis of the Al3Mn-type approximant in this ternary alloy system. The diffraction patterns of the title compound are quite similar to those of the typical Al3Mn phase including the systematic absences of k + l = 2n for the 0kl plane and h = 2n + 1 for the hk0 plane [3][4][5][6]. These results readily lead the space group of Pnma or Pn2 1 a. The converged parameters in the non-centrosymmetric Pn21a model serve no significant differences from those in the Pnma model, and present analysis selects the centrosymmetric space group Pnma. It is usually difficult to determine the distribution of three elements by using the diffraction data alone. Nevertheless, we can obtain here one of the most feasible distribution models as follows. The electron density distribution and corresponding first nearest neighbor distances indicate that Mn1, Mn2, Mn3, Mn4, Mn/Al5, Mn/Al6 and Mn7 are almost fully occupied by Mn. The highest electron density was observed at Ge/Al25 and Ge is suggested to reside here. Mn/Al8, Mn9, Mn/Al15 and Mn/Al16 are coordinated by Ge/Al25 with distances from 2.51 Å to 2.58 Å, suggesting the preference of the smallest Mn at these sites, again. The fundamental preference of Al at remaining thirteen sites was revealed and interatomic distances among them lie over 2.66 Å, except for d(Al/Ge18Al/Ge18) = 2.276(3) Å. Taking into account such features, the structure of the title compound was refined starting from the structural model of Al3Mn with chemically disordered eleven Mn/Al sites and fourteen Al/Ge sites. Several least-squares iterations revealed the chemically ordered sites of Mn1, Mn2, Mn3, Mn4, Mn7, Mn9, ...