electron microscopy



Ordering Phenomena in YbSi1.4

YbSi1.4 crystallizes with orthorhombic symmetry (space group: Cmcm; a = 4.159(1), b=23.510(5), c=3.775(1) Å). The basic crystal structure was determined from single crystal X-ray data. The structure contains trigonal Yb6 prisms that are fully occupied by Si forming zigzag chains which run along the c-axis. Residual electron density intensity that was detected in the other Yb6 prisms can be explained by Si split positions, leading to an occupancy of ~80% of the corresponding prisms. Since the nature of this feature could not be unraveled from the X-ray data alone, a comprehensive TEM investigation of YbSi1.4 has been started.

Electron diffraction pattern (a) and HRTEM image (b) along [100]

Transmissions electron microscopy (TEM) investigations showed the presence of two distinct ordering variants: Additional reflections in the electron diffraction pattern indicate that YbSi1.4-I (Imm2; aI = 4.16, bI = 7.56, cI = 23.51 Å) has a c axis that is twice as long as that of the basic structure. In the structural model derived from HRTEM images, Si systematically fills 3/4 of the partly occupied Yb6 prisms. In YbSi1.4-II, the additional reflections are split (Fig. a). This points to an incommensurate modulation that can be described in the 3+1 dimensional superspace group Cmcm(10γ) (No. 63.3). The evaluation of HRTEM images of YbSi1.4-II revealed parallel domains with the structure of YbSi1.4-I (Fig. b). The modulation is caused by a shift of these domains in respect of each other.

The Real Structure of YbSi1.4 - Commensurately and Incommensurately Modulated Silicon Substructures
C. Kubata, F. Krumeich, M. Wörle und N. Nesper, Z. anorg. allg. Chem. 631 (2005) 546-555 DOI.


ETH Zürich | ETH chemistry department | ETH inorganic chemistry

modified: 6 February, 2015 by F. Krumeich | © ETH Zürich and the authors