Anomalous Debye-Waller Factor Associated with an Order-Disorder Transformation in an Al72Ni20Co8 Decagonal Quasicrystal


Hiroshi ABE, Hiroyuki SAITOH1, Takashi UENO1, Hironori NAKAO2, Yoshie MATSUO3, Ken-ichi OHSHIMA1 and Hitoshi MATSUMOTO

Department of Materials Science and Engineering, National Defense Academy, 1-10-20 Hashirimizu, Yokosuka 239-8686

1Institute of Materials Science, University of Tsukuba, 1-1-1 Tennoudai, Tsukuba 305-8573

2Department of Physics, Tohoku University, Sendai 980-8578

3Department of Physics, Nara Women's University, Kitauoya-Higasi, Nara 630-8506

J. Phys. Soc. Jpn. 72, 1828 (2003).


Abstract
An order-disorder transformation in a single decagonal quasicrystal of Al72Ni20Co8 is studied in detail. In X-ray diffraction, the anomalous attenuation of intensities of Bragg reflections was found around the transformation temperature, Tc. The intensity attenuation at high temperature is explained by the anomalous Debye-Waller factor in thermal lattice dynamics. In particular, the intensity ratio above Tc and below Tc depends on |Gperp|2 values. In addition, the intensity ratio between room temperature and high temperature shows |Gperp|2 dependence. The results correspond to the in situ observation of a local vibrational anomaly related to an atomic flip by electron microscopy (Abe et al.: Nature 421 (2003) 347.). By X-ray diffraction, dynamic fluctuations as observed in electron microscopy are also realized even on a macroscopic scale at high temperature
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KEYWORDS: quasicrystal, phason, atomic flip, order-disorder transformation, Debye-Waller factor




Fig. 1

Temperature dependences of (a) the intensities and (b) FWHM for the 30440 and 12540 Bragg reflections. The intensities of the Bragg reflections are almost reversible. Anomalous decreases of Bragg intensities were seen below Tc. At the same time, peak broadening occurred.



Fig. 2

(a)|Gpara|2 dependence of the intensity ratio of Bragg reflections at 965 K (=T1<Tc) and 1096 K (=T2>Tc). (b) |Gperp|2 dependence of the intensity ratio between room temperature (Trt) and high temperature.




Figure 3

(a) Occupation of domains of (1/5 1/5 1/5 1/5 1/4) (left) and (2/5 2/5 2/5 2/5 1/4) (right). (b) Preoccupation domains of ƒ¿ and ƒÀgenerate phason-related atomic positions. The distance between them is 0.095 nm. The lines indicate the HBS tiling with an edge length of 0.636 nm.


Fig. 4

Calculated intensities of the 12540 and 30440 Bragg reflections without the Debye-Waller factor. p(ƒ¿) is the occupation probability of Al on ƒ¿-sites.


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ab@nda.ac.jp
Department of Materials Science and Engineering
National Defense Academy

Last Modified: April 1, 2009