中国物理B ›› 2006, Vol. 15 ›› Issue (9): 2065-2079.doi: 10.1088/1009-1963/15/9/029

• CONDENSED MATTER: STRUCTURAL, MECHANICAL, AND THERMAL PROPERTIES • 上一篇    下一篇

Group-theoretical method for physical property tensors of quasicrystals

龚平, 胡承正, 周详, 王爱军, 缪灵   

  1. Department of Physics, Wuhan University, Wuhan 430072, China
  • 收稿日期:2006-02-24 修回日期:2006-04-13 出版日期:2006-09-20 发布日期:2006-09-20

Group-theoretical method for physical property tensors of quasicrystals

Gong Ping(龚平), Hu Cheng-Zheng(胡承正), Zhou Xiang(周详), Wang Ai-Jun(王爱军), and Miao Ling(缪灵)   

  1. Department of Physics, Wuhan University, Wuhan 430072, China
  • Received:2006-02-24 Revised:2006-04-13 Online:2006-09-20 Published:2006-09-20

摘要: In addition to the phonon variable there is the phason variable in hydrodynamics for quasicrystals. These two kinds of hydrodynamic variables have different transformation properties. The phonon variable transforms under the vector representation, whereas the phason variable transforms under another related representation. Thus, a basis (or a set of basis functions) in the representation space should include such two kinds of variables. This makes it more difficult to determine the physical property tensors of quasicrystals. In this paper the group-theoretical method is given to determine the physical property tensors of quasicrystals. As an illustration of this method we calculate the third-order elasticity tensors of quasicrystals with five-fold symmetry by means of basis functions. It follows that the linear phonon elasticity is isotropic, but the nonlinear phonon elasticity is anisotropic for pentagonal quasicrystals. Meanwhile, the basis functions are constructed for all noncrystallographic point groups of quasicrystals.

Abstract: In addition to the phonon variable there is the phason variable in hydrodynamics for quasicrystals. These two kinds of hydrodynamic variables have different transformation properties. The phonon variable transforms under the vector representation, whereas the phason variable transforms under another related representation. Thus, a basis (or a set of basis functions) in the representation space should include such two kinds of variables. This makes it more difficult to determine the physical property tensors of quasicrystals. In this paper the group-theoretical method is given to determine the physical property tensors of quasicrystals. As an illustration of this method we calculate the third-order elasticity tensors of quasicrystals with five-fold symmetry by means of basis functions. It follows that the linear phonon elasticity is isotropic, but the nonlinear phonon elasticity is anisotropic for pentagonal quasicrystals. Meanwhile, the basis functions are constructed for all noncrystallographic point groups of quasicrystals.

Key words: quasicrystals, elastic constants, basis functions

中图分类号:  (Tokamaks, spherical tokamaks)

  • 52.55.Fa
52.25.Vy (Impurities in plasmas) 52.38.Mf (Laser ablation)